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1 decimal integer ring cycle of many

Quantum Field Fractal Polarization Math Constants

nemeth braille printable arx calc

pronounced why phi prime quotients

Y φ Θ P Q Ψ

condensed matter

Y Phi Theta Prime Q Quotients Base Numerals 1dir 2dir 3dir cdir

numer nu mer numerical nomenclature & arcs

Numerical values exist before the nomenclature of numerical nomenclature and it is in the moment numerical value is completed that numerical nomenclature is defined in itself the value it is structured. Then is the fluidity of numerals structured in itself of numerical values given paths ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄  of numbers (nNncnncn) logic to limits within or not within the structure of the numerical values. Less than zero or quantability of nuclear vacuum field vectors in electron plasma veils is not only a plasma illuminating factor and is also subject to exponentials, multiplication, division, addition, and subtraction of quantum field fractal polarization math. Particle charges, positive or negative for example are many times over or under estimated and the exact numbers to those factors can be written mathematically. Mainly rather than a float point significand average quotient from a total sum added value gathered in division of the sum total average, numbers naturally have a significand of their own being the decimal point and its relation to the number or partial numbers counted of a repeating decimal constant chain of scaled partial constant variable frequencies. The numerical value of a variable average base in floating point utilizes a part similar to variable change precision leeway, where as instead if compared to the ratios of constants based decimal cycle stems in quantum fractal polarization scale variables, the decimal precision of known ratios and their digit order in cycle stem has less leeway and is calculable to numeral defining value. When one error of one value is a variable misguidance through arithmetic paths toward an average from partial derivatives, an endless loop of decimal precision can be unnoticed and if not unnoticed counted and predicted, such as error, partial error, or correct non error allocatable derivative variables of that average thus negating the estimated value of an average and equating to a precise detailed proof in prediction methods.

A LIST  of  A  B  C  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  Ψ  ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄ 

VOSS variables of sequential sets (ssv)

Y {0, 1, 1, 2, 3, 5, . . .} fibonacci

P {2, 3, 5, 7, 11, 13, . . .} prime

Ψ {4, 6, 9, 10, 12, 14, . . .} non prime non fibonacci natural whole numbers

Elementary physics involves quantum fractal polarization math constants in the numerical translation of quanta related to the matter in and around the translation point of that measurable translation for transcription to the quantifier. While a field such as space has a vacuum electromagnetic constant of the state of that specific field, within it a star, sun, and atoms is contained within the frictional difference of a form of matter condensed causing the star, sun, atom, or cluster of such to spin until an equal counter opposite exact electromagnetic measure allows for the star, sun, atom to bond with a kind of its own or consolidate and be an accumulated larger one measure of its own kind. Commonly the bonding effect of electrons aligned through a vacuum field is an arc of illuminating quick indifference through the extreme opposite veil of space that transports that matter to the other matter it shares a frequency with to that degree of measure. 

Thermodynamics represents friction as workable force particle charge available for thermal transfer and the frequency of those bond searches are then in a sense a search for rest from friction or work to bond in a frozen state reliant on the gravity or electrical polarities of a larger or more powerful constant able to let that specific bond rest from work and fiction. Some elements in a frozen state of matter may decay do to atmospheric oxidation and decompose to atomic parts of what element it is or wait on an event of extreme heat and friction that then again changes the frozen solid state phase to fluid and gas until the process repeats. In the process of the star, sun, atom spin is a centrifugal force of energy contained in the poles of north and south so to say, a force of the major mass element involved in that bodies point in space. The south pole given enough time has a upward or through directing of energy and loose atmospheric  electromagnetic or non electromagnetic matter while the north pole has an up and outward directing of energy and matter that is free from the surface of its body. Both poles are part of an entropy enthalpy or centrifugal and centripetal system of that spherical body. A planet such as earth and its siblings is much like protons and electrons that orbit the sun, while the moons are similar to electromagnetic nature such as neutrons bonded to the orbit of their phase state placement in the system of the sun, planets, and cluster of stars it is part of. Within the atmospheric shell energy and matter that the south pole direct upward and through then hit a wall of lets say ground; the energy that can travel where the solid matter can not shifts kinetic energy of that element's movement polarized charge as the charge kinetic sum and the element part ways in their paths. That atmospheric difference kinetic measure of energy transferred to each path variant division is sufficient to contain within each element of the event in their parting where the traveled element settles in a spin cap long enough to become a frozen phase state that matter. While parts of the whole body have upward through and upward out North pole from South pole split paths constant properties of the whole body constant state, there is a inward, down attracting physics state to most near all matter in that body system called gravity or electromagnetic constant. These measures are not always whole numbers and when dividing leads to more dividing and or bonding of divided parts of what can be called from a whole measured thing, it is very likely the whole measured thing that the matter derived from is only an opinion of that being a whole entirety of absolute 1. The same idea is also an opinion when applied to a thing in matter, its distance traveled in time, about where it is coming and going as well as the changes it will or will not go through, while it either changes or does not change the field matter of space it is traveling through or around. Similar or relative terms of time and matter differ having exact numerable differences are not exactly similar or relative terms without the numerated variable term of their difference.   

Quantically, the changes matter goes through while its phases in time space differ from the changes that matter then counter measurably to the field of matter it may or may not change, are also mathematically measurable as well as all parts of each parts' parts. One could consider that the light and energy emitted from a star is an an illumination of an arc vacuum across a measure of time limited to space of condensed energy while a lightning arc is an illumination of an arc limited to time rather than space and yet both are phase states of energy that is a constant of matter and paths that matter has measurable limits to in differing relations.. Vacuum field is a veil of space with a specific time allowing or not allowing a certain measure to change light passing through that gas phase state field. These are elementary state phases of light and dark shared in time space and matter, and within are many degrees of that light and dark sharing time and space as measurable or not measurable shades and tones. While some measures of energy, light, absence of light and ground negative or positive path charges of energy are lethal to many biological forms unit measures of that energy are numerable. If numbers of systems can represent those systems, still then the factoring of those numbers and the extreme length of number potential compared to a persons life span for example, means that some math equations could take a lifetime or multiple life times to write out and the very matter on which the written answer to an equation has a limited decay rate, or limit in writings being preserved its for reading once it has been finally written completely after the lifetimes it may have takento be written. The question then is who is there to read it, as they are unique to the writer, certainly more given the measures of time given to that answer and its preservation. 

If anything, you will learn the importance of variable factor precision of decimal cycle rounding in fractals here rather than rounding whole numbers. Cell cycles apply (ooo) order of operations to your variables after a golden ratio cell cycle of numerals is distinguished. The cell cycle that is found in applying the opposite when adding a variable to the previous from 0 1 1 2 3 5 8 13. . . then dividing is often referred to as error in order of operations of mathematics... PEMDAS parenthesis exponents multiples division addition subtraction order of arithmetic in algebraic equations. Variables in paths prove those order of operations are not persued followed or set for all numerable measured parts of matter in existence. Base particles of matter and subatomic matter are numerable in their structure and numerable of their relevance to outside their structure. The math and numerical data on this page at its base structure may have you rethinking your BP base pair in DNA factoring and loop wrap stem decimals precision nomenclature

Viral, non-viral, marsupial, and non marsupial cell numerations have core logic outside pemdas (ooo) logic. One exfoliation produced in a phi ratio is much like a start of |1| absolute one exfoliation much like an absolute zero |0|=1. The order of operations is a mathematical logic, however the patterns in the exfoliation are proof that in matter the order of operations were not to a level of whole natural numbers and still had natural patterns of its formation. Alternately the exfoliation is a limit to that part of that set it is limited to governed by time and space constants. Whether a variable change is micro or exponential, the decimal precision in factoring its numeral value in any function is that important noted commonly with δΔ or δ∇ such that these being the change or loss of a system to a degree of micron exponent µ° µ′ to µ′° or minus µ′ in value. µHz lacking a µHz at µ intervals of time are a µ difference in a frequency hit through a ampere watt system that are that µ important and sometimes overlooked or inaccurately factored of δΔ or δ∇. 

A  simple example of how cell cycles apply is a cell consuming another cell for keeping what it needs and discarding what it does not need from the cell it consumes. Shells of cell growth and discarded evidence can often be found seen or identified in patterns formed on the shell structure of the shell restructured discard. A simple analogy for quantum field fractal polarization math is the word Permutations, pronounced (per-mutation). Micron units of flux µφ found in permutations of hysteresis loops are a great example of how energy is fractionally measured in wave frequencies. Resistance values are expressed in ohms Ω that reflect in δΔ or δ∇ partial derivative gain or loss to a system when a difference between flux, resistance, and energy flow are not calibrated to extremely precise values and variables of the system components and element limits involved in that systems engineering. Deterioration of mechanics in systems such as iron of permanent magnet stator motors is just one example of a fractional cell variable factor miscalculated and its potential loss to a system. Commonly, micro Thermal Resistance µΨ is a factor of mechanical limits of machine elements easily miscalculated when magnetic memory of hysteresis loops are concerned in electrical machinery and is a contributing factor of deterioration of system elements. Raising the temperature a few millibars to oxidation chemical process on an exponential level raises corrosion as quick as an electrical charge.  

A very similar example is a human body system of systems with fractional variables able to be miscalculated in diagnosis prognosis and treatments, where the hypothalamus commonly regulates thermal controls for allocating a potential virus in the system of body systems down to the atomic cell level in signaling. CNS EMF central nervous system electromagnetic field example and liquid liquid phase separation is actually more close to 5 phase of triple point as an analogy where with water from vaper gas tripidated into fluid then to ice frozen solid state that has slush between fluid and frozen state and precipitation mix between gas and fluid saturation applied in biological membrane systems. Wave functions are applicable to measurements and extremely precise in limits or memory limits, we can call quantum fields and the measures are fractal parts of whole systems polarized in thermo-chemical electro-magnetics.

Allergen exposures and cancer symptomatic response in cell autophagy along with anastasis and their commonalities then forward to altering paths of cell discourse and discard of differing biological life forms of differing environments... as example Discontinuity and improperly calculated factors of discontinuity that when overlooked or miscalculated lead to a continuity of continued exposure, process, or pathway of potential continuity when discontinuity is the intent of ending the cycle of a specified term exposure, process, or pathway. The numerology then of the substrates should be not limited to rounded summations of limited calculators and algebraic formulas, rather the numbers should be precise and accurate measured units. Neurophilus cells will either attack invading cells from their pre-programmed neucleic cyosolic mechanisms or turn into a shielding cell to protect cells such as inflammation, cyst, or more commonly thought as a tumor growth. Later that attacking cell may call on more cells to aid in the fight while unaware from signal blockers it is attacking the body of the self systems or building a growth of clustered cells in inflammation, cyst or tumor. At this phase the cells are much like φ and Θ of differing paths give or take, anticipate or wait later/previous 1, previous/later 2 from Y base variables. A body of systems trying to process discard of a tumor cluster cyst or inflammation measurable mass or system occupancy of lymphatic nodes with incorrect cell transcription and translation then is at a phase of exponential numbers of a cell formation that has many factors to its existence. A patient treated for cancerous cells that then returns to an allergen environment of day to day routines around allergens will be exposed again to the very agents that began the allergic response so similar to cancer cell clustering reactions of immune system defenses that take merely a few seconds to minutes for an allergic reaction to occur. Proper factoring and precision of all variables is critical to effectively eliminating the allergen confusion commonly mistaken as cancer in this example. One histamine release signals many immune system mechanisms and being that histamine is a chemical of the mind and body, both are in turn effected. Countering such reactions with estimated chemistry of pharmacological trial studies post thanatological studies is a guess and not a very effective mathematical guess for any degreed physician is has prerequisites in mathematical degree course credits. Example Heme Acetyl Neutrolphil mechanisms for proper diagnosis, prognosis, and treatment. MERCK NIST. Between Environmental, chemical, and gestational Histamine Intolerance to Cancer types, to the here try this list of pharmaceutical clinical trial medication regimens, along with the many phases of chemistry and cell paths of reflex through and of variant nucleic variables, exact numbers of exact and precise variables should be considered given the extent of these vast arrays of symptomatic labels in diagnosis prognosis and treatments. Antigen and Antibody identification along with a library of such identifiable cell types very much extend within such extreme number precision as these quantum field fractals of polarization and the math backbone to their numeral base constants.

In some cases, simple math logic and its comprehension is a cure to something as complex as a brain system chemistry trying to process a lie it was given to process as a truth it is not. When numbers and arithmetic do not lie a cure for Factitious Disorder (e.g. 1 and e.g. 2), is as simple as solving a basic simple math equation that the brain searches for a foundation of fact from. The mind or brain is a system extension of a body of systems and cell groups of types that have symptoms of say heachaches for example that when a lie is present in memory of the mind, the body of systems may try telling the brain mind something is inaccurate and something as simple as admitting a truth in the mind such as a simple math equation can in fact alleviate the headache partially or completely from proper brain chemistry changes in gray brain matter verse white brain matter. Many parts of a body and its systems will not allow parts of the mind brain to continue a lie as it is in part then obstructing that body system from functioning properly and its own longevity or survival is then at stake. This is commonly referred to as neuron signaling of receptors and pathways. Within those pathways are paths that grown structured biological memory called logic gates such as a noted comprehension memory of left and right or in this math paths of later/previous 1, previous/later 2, or decimal stem cycle difference division 3⅄ of Nncn 

CNS immune privilege and neuroimmunology are fields of such brain chemistry that involve histamine releases based on fact or fiction mental distinguishing along with many other cellular biochemical system exchanges that can and will alter the overall system health regulated in the central nervous system. A mind of a body with histamine intolerance that is continued to be lied to and made angry while it tries to distinguish lie or truth of information while in an allergen environment or exposed to food and/or chemical allergens then releases histamine throughout the body that is very similar to an allergen response commonly contributing to inflammation, cystic formations, and other cancerous types. A lie replaced with truth fact rather than a clinical trial medicine can alter a path in one of many misdiagnosed.... simple math. So then natural dopamine, serotonin and brain chemistry of gray verse white brain matter can be achieved without added lies and to some those lies are exactly what some children are allergic to added to food, chemical, and environment. One could summate and round an evaluation that some lies are in fact extremely unhealthy for some people and so too then for various other life forms.

With infinite math paths and infinite unlimited numbers to those math paths, start with limits of your own and noone elses limits until you comprehend your limits and find your limits extended from your comprehension of limits. Finite is a numeral limit that is often an opinion in some cases, the truth of finite in infinite compared to an opinion of finite is mathematically provable in many of those cases.

Mathematical ratios are applicable to atomic change and change as well as no change are numerically definable so when change is labelled as no change and is inaccurate in label, the change that is present does not completely stop changing although it is overlooked and can lay dormant while miscalculations in a change labelled as no change may be crucial to time, energy, and many other atomic variables.

A part of something is a ratio or percent of its whole and elements of the periodic table have prepacked atoms of variations eons of time took to change the isotopes and atomic structure of those elements to form other elements and compounds. An acidic base for example will break down and divide many protein types as well as other compounds to their atomic level and within those are parts of parts that are not whole and are whole at the atomic level. If one part of a whole or a percent ratio of a whole has predetermining factors of dividing capabilities when in exposure or relation with another part ratio percent of a different whole part, then ratios are in fact able to be divided or divide other part percentages and numerically they can be defined with numbers. Indivisible is then not a proper label for ratios divided by ratios that are in fact divisible. Sub-atomic nucleic indifference(s) and stem cycle variants within ten digit limits of fibonacci count and prime numbers as a base example in numerals. 

A perfect example of a decimal stem cycle limit in cn of a ratio number Nncn is in the cytosol nucleic bonds of DNA and RNA transcription receptors where one nucleus chain tells another nucleus chain it is limited to a number of cycles of its chain stem decimal order and is then able to translate how much of a repeatable set of instructions is then allowed to be packed in its limited ability to store that information for the bond of nuclei to be maintained, thus one nuclei must be able to translate and comprehend the inquiry chain without itself being altered in the process or its own being is then changed to an entire new transcription and translation comprehension. If proteins enzyme structures of sugar oil and sodium are basic instructions, one could think of glyceride as a food fuel source in sub atomics, sodium salt is a crystalizing bonding source in sub atomics and oil base of alkaloids are a dividing chemical structure that continue dividing no matter if in fluid saturated phase states or expanded gas as the efficiency of its dividing nature is dependent on the ratio to ratio of which it is in contact with to divide before it is neutralized or out of resource for dividing anymore. Chemical reaction is a bonding or dividing event and this math is a basic representation of that fact in a numeral quantifying explanation of similarities with the nature of numbers and how they naturally structure in relations.

ACQFPS  A LIST of calibration factors in quantum field fractals for practical application in arithmetic functions of precise variables. 

example genome bases - nucleic acids - amino acids - chromatin - chromosome - protein - neurochem - gluons - valence

e.g.1  e.g. 2  e.g. 3  e.g. 4  e.g. 5  e.g. 6  e.g. 7 and limits in calculated factors decimal precision that numbers prove nomenclature of rounded variable theory can be replaced with non theoretical numerals of precision such as DNA RNA 

1.65 dimmer windings of double helix seems rounded with only two decimal parts of its decimal compared to many ratios listed below on this page. 

electron - proton - neutron - caton - axion - anion - nucleotide - nucleosome - dimmer - telomere - virology - photon - parton - exciton

Signaling in cells and systems use fundamental concepts of electrical and chemical message relaying such as evolution and change in dna for a system organism to survive a change of the environment it advanced to its state in that environment before the dna requires a change in itself to adapt to the environmental changes for that system of organisms to survive in the changed environment it was signaling its need to change and adaptation information. An example is the tentorium to a cytosine or a plant base cytosol or an shell traits of membranes. Signaling Transcription and translation can involve distance, time, and many other factors for specific definitions of long range and short range effective communication. In order to carry out task completable cell instructions of obtainable matter, use and discard of that matter missing any part of the dna rna instructions will resort to survival or shutdown pre-programmed chemical instructions within the elements of its making and current possession at the time of the translating of the transcriptions. 

Time and distance are relative terms to application of the transcription translation as are the transcriptions to the phase state of the environment the transcriptions are factored for to related distance environment of relative terms and then distance is a term of time and environment of its own definition parted when time is a distance or when distance is relative to a point measure from a sustainable continuum of being in survival in an environment that is not defined in the transcription waiting to be translated. Cryogenic stasis, anastasis, autophagius self preservation survival minimalism, and celestial distances as well as time would be examples of a transcription translation between one point in time and space to another point in time in space or multiple points in time and space through multiple phases. 

DNA, RNA, gRNA, mRNA, microRNA, rRNA, siRNA, snRNA, snoRNA, tRNA, ncRNA, lncRNA, and piwiRNA as examples, relate similarly to number constants, number bridges and partial number bridge connectors, yet a computer programmer who writes languages in a computer shell library that echo prints answers to software network web searches with numbers should then have DNA and RNA library answers to those searches from a database rather than exact numbers to basic algorithms of simple calculus number frame arrays. Computer programmers given the cessating time for a language library to be written  for answering a web search inquiry should not deter simple library number searches to be blocked with computer programming explanations of more cessation. A number library in a DNA and RNA database or long range and short range ratio factors are Numbers and no a computer language. A number search in a web search for a number library answered with excuses of SQL blocks and reasons for those searches blocked is not an answer to a number search in a Library of Numbers.

Data elements in library file logs that are not dependent of a noticeable distance and time relativity in high speed internet communications when a machine is utilized in proper connections. SQL search blocks in sync with Poorly Understood reference material on subjects of DNA and RNA for example along with calculators that round at a basic limit of ten to eleven digits are factors or program limits in C, C++, Java, or Python calculations to source information limitations and access are again why a number library is simply a library of numbers limited to the storage space of that Number Library.  Here on this page DNA and RNA is not poorly understood nor misunderstood nor are the numbers that are filed to computer storage systems of such nomenclature and information. Instead of a sql search block from sleeping nested transaction programs in idled number systems blocking logical math and numbers of basic arithmetic to complex algorithms this page has more simple numbers displayed of the basics in quantum field fractal polarization math applicable to multiple arrays and uses in long or short range engineering and pathology allocation.

Long range and short range arc trajectory math are simple logic that depend on variables and factoring of potential change in that trajectory path that varies on many factors. Arithmetic that utilizes plus one, minus one, plus two, minus two, or exact numbers between 0 1 2 10 or more that can easily be factored incorrectly to exponential estimates and there are unit measures on this page that reflect on those unit measures to precise degrees. 0 1 01 10.1 101 1.01 0.1

example solar systems  -  quadratic propulsion system engineering physics  -  pulsars

Quantum Field Fractal Polarization   e.g. 1   e.g. 2   e.g. 3   e.g. 4

      ⬡   ⬢   ⬡   ⬢   ⬡     ⬠   ⬟   ⬠     ⯐   田   ⨁   ◭  ◮  ⧨  ⧩  ⟁   ⨀   ⊚   ⧂   ⌱   ∘   ⦁   ⋯   ⋮   ⋱   ⋰   ∴   ∵     ◉   ◎

Paths of evolution involve processes of transposable elements of junk rna transpons and dna retrotranspons through shell discard such as holometabolous and hemimetabolous complete shell disposal molting or semi-partial shell discard. Directly down the middle so to say of centrosomes kinetichore in chimera cells is basically a lop sided partial decision of cellular instruction packages signaling transcription and translation that are commonly referred to as nicks, the discontinuity in a dna rna strains. At the molecular level these numbers are very similar to that partial derivative quantum fractal field polarization math and its variables of potential change. Given that the factor variables explained here are whole numbers of fibonnacci and primes, a valuable point is that the same numeral path set applications can be applied to decimal numerals in the same fashion and thus doing so changes the decimal place in many of the quotients, products, sums, differences and exponents... for example instead of starting with 0 and 1 and 1 and 2 and 3 for fibbonacci Y base and entirely different base set for Nncn could be started at 0 then 0.1 then 0.2 then 0.3 then 0.5 then 0.8 then 1.3 that set variable 22φn3 is very similar with for example as well as 22φn2 that is 0.5 

As this is the case with these variable values it is recommended to make notation of sets that start with decimal values rather than whole numbers as the values are similar or equal to variables already defined in other complex equation set bases. ⧊Y and ⧊P could note for 0, 0.1, and 0.2 . . . . so too then 0 then 0.01 then 0.02 then 0.03, then 0.05, then 0.08 then 0.13 and this will change a variable factor precision value extremely much when it is applied to exponential algebraic formulas. Much smaller longer decimal ratios and fractals are applicable and this is merely an explanation of that fact about micron unit measures of precise value. Between zero 0 one 1 ten 10 to the Nth number ⧊Y, ⧊P, and nth definitions in paths of algebraic functions ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄ A LIST library with supporting variables to equations then makes ACQFPS advanced complex quantum fractal polarization sets available for practical applications. 

Forensics evidence factors for postmortum investigations rely heavily on such specific details as does education of these sciences and arithmetic. Aerotech industries can also benefit from high precision in wave function math for propulsion systems limits and space time positioning. A quantum field fractal polarization math analogy would be nearer micronomical unit measures of astronomics or astronomical unit measures for micronomic system equilibriums as what is up, what is down, what is in, and what is out relativity to then now when and why with how much about what.

On this page you will find 1dir constants of numerical key values in decimal degree integer ring cycle(s) notations. Dir refers to directory in computer shell c:// compilers for nomenclature organization at a user interface. Capabilities for these numerical key decimal degree values have potential in practical application fields on advanced research development areas such as physics, optical lens curvature alignments, nucleosome structuring in (dna) deoxyrubenuclaic acid histones to chromatin signatures, biomedical engineering, astrophysics, thermodynamics, cyclemetrics, fluid engineering, electrical engineering, and vacuum field induction arc fusion plasma stablizeations of thermonuclear energy.

Quantum fractal field harmonics found in data structures, periodic table atomic weight, masses in bonds scale shifts, guide key to unit in factor change requirement notations, sensor systems calibrations, plasma fusion as well as kinetic particle workable force harvesting in delta change models require precision that ai utilize of these decimal degrees.  

Encryption method strings of variable factors to applicable change values in natural math was invented some time ago through evolution of cell divides and many displays shells of cellular memories. Other examples in arx of ratios are atomic spin relief, covalent bonds on isotopic levels of required precision for stability of a cells before generating new cellular memory for genetic reproduction frame works,  meiosis and mitosis of life forms cell memory in the environment it may adapt to outside your factoring base language knowledge of its potential new language. Keys of a cell compared to its memory cycles before its arx radical new ratio shell strain changes are vital through fission and fusion events that the cell carries organized to its own comprehension and new translation before the cell then communicates its base language or new level base language outward and inward. For generalization suppose the whole number and part of the number of a variable 1φn8=(Yn9/Yn8)=(21/13) is the cell 1.^615384 and the repeating decimal chain is the stem cell memory after the noted chevron ^ symbol in the bolded part of the ratio variable. Then the cell of variable 1φn10=(Yn11/Yn10)=(55/34) is 1.6^1762941 the repeating decimal chain is the stem cell memory after the noted chevron ^ symbol of one cycle in that cell memory stem, where as two cycles of that stem cell memory is the chain repeated for a variable of 1.6^17629411762941 rather than 1.61762941.

So 1φn10c1=1.61762941 and 1φn10c2=1.617629411762941 and when loss of a system δ∇ is noticed and not allocated, it may be the exponent of a variable factor unfactored for in calculating, that if 1φn10c1 is assumed to be the value noted in complex quanta while 1φn10c2 the value is actually , then a loss of 0.000000001762941 at each and every misfactored applicable term the error is miscalculated. Exponentially this miscalculation can spread across a system and allocating this error for proper system numeral balance is then a basis for precise variable definition just as variable change is one factor incorrect rounded numerals and estimates then acrue and sum up an unknown factor variable of loss in the system example that can be avoided if calculated correctly to paths of the system exact.

Another example of an arx radical ratio precision numeral is the importance of a Si standard increment unit mer measure of C or H of the periodic table of elements. Atomic mass as the H hydrogen base atomic weight next to C carbon used among the other elements as a base unit measure point variable calculus uses as a scale numeral starting recorded numeral value in nomenclature of other elements. 

The other elements of organic and inorganic chemistry have many phases of reactions in elemental physics of many thermodynamic phases and astronomical scales quantifiably. 

Example Pharmacodynamics and Pharmacokinetics - Toxicodynamics and Toxicokinetics

(variants) a law of decimal in calculus trace prediction logic pathogen pathology. 

Consider this page a speed square of arc constants that are real numbers in decimal computational factoring and non theoretical with practical application potential like your famous framing square instead for arc engineers and λ wave functions down to tinsel strengths of architectural engineering. Remainder or reremainder are more important than your python disregard to the decimal # c ++ rounding and a computer that returns a rounded number of a non float pointed very precise number is a computer that is floating not the number searched in the query log that is defined. Many numeral base defined decimals will be displayed on this page that have a wide range of web search results when a search is performed for information about a specific number or numbers in these Arithmetic arrangements.

Learn when to stop going in circles... a simple error to extreme precision perfect accuracy 

Using a basic Fibonacci count example 01 to 10 digits divided in on itself at each step will provide the decimal key cycle ciphers that are numerical constants that only change when an additional degree of the decimal precision point is extended in areas such as biomedical viral strain stem studies and aeronautical flight paths. These numbers are basic enough for a child to find and make great pyramid blocks for simpletons scale to scale where a math class is not a psy ops placement protocol at medicinal sciences of health and neuro-chemistry restructuring of no lie brain chemistry balancing, honestly over shooting brain mapping contradictory publications of fractal field polarization in the display 3d compiler.  

Decimal precision math is not a new math to be invented. dir dot of ooops ops and [()]ex/+- pemdas does not apply to long division order of operations that numerically land decimal values previous to any prime base or cube rooted exponential value theory. addition division steps of rationals divide subtract multiply divisor repeat until the stem ring is identified numerically. In some calculation of a fantasy pi, sine, cosine, tangent, limitless matrices, arrays, fields, or canonical vacuum field equations of theory imply a value of vague precision factored where a radius unit measure is not magically bent in arc ratio to a circumference unit measure straight line inside mid or out of the arc unit measure; added to ifs of theoretical numeration factor error disasters of exponential sometimes lead far from analytical trouble shooting and solvent potential... zero point decimal variable of ⌱∘⦁ 0.13 rounded abbreviation 15φn2 constant groups in radical nu mer 1dir natural numbers has a rounded notation as accurate as the pi imaginary ratio of unlike terms in unit measures and does not mean it is a best educated guess variable theory factor substitute.

Test the numerals of the scales provided on audio and lumen with scale shifts of time between octave changes of the numerals to audio or light or both. Some lifeforms will mimic repeat the tone or rhythm such as birds or try to eliminate the source of the speaker producing the frequencies given n number of cycles. A short or long signal is chaos math or chaotic transmission to a receptor that has no memory or knowledge base of "short or long signal". 

Chaos harmonized through a harmonic phase of chaos in a sense, transforms chaos pieces of a complex signal to multiple rhythmic uses of particles with limited reaches as chaotic as those particles are. Memory relays the chaos harmonized particles through other signaling systems and sometimes transmits signals like an echo reflex mechanism of cellular memory. A computer floating outside of a number defined as mentioned is a device likely with an ip number and the device itself is floating around the defined numeral decimal points defined while the multiple numbers might be defined or have definition of a cycle stem variable path that appears as a floating point in cyclic memory of that path or others.

Ferrofluid and cymatics are a base exchange chemical and electrical signals in alkanes of dna rna base chromatins of neural receptor transmissions on a viruses viral to the virus level being a virus to the virus itself where mimic bacteria also communicate in chemical compounds of minute trace element bonds just as are frequencies of energy. Host rhythms in a sense can feed a dormant strain where it anchors and frequencies can lore them out just like circadian clock cells. Jet propulsion systems are another example of ratio use in workable force to movement and angular direction of these ratios has application in quad copter flight. 

Braille translator for printable braille of this page is limited to none of the links highlighted. A braille tablet is recommended for visually alternate reading of this web page.

Long division ratios have a probability of the quotient decimal length that depends on the number of the divisor. If the divisor of a phi ratio has a decimal stem cycle that is repeatable such as 1.619047 /1.615384 that the cn factor for c1 to c2 for 1.619047619047 /1.615384615384 then the probability of the quotient decimal length before the cycle stem is located is approximately 1,615,384 digits or less and then for c2 is an approximate probability of a quotient with a decimal cell stem cycle of 1,615,384,615,384 digits in length or less. Stem cell variant cycles of precision and arc are simply numeratable factors of logic and not aiming past a precision focal point is one fact that makes these logics that important. The probability of the ratio quotient decimal length between complex radicals in finding a stem cell cycle of cn of the quotient is the whole number of the divisor without the decimal point, less than that numeral or half that numeral or more than half that numeral in length of decimal digits and the cycle has one cycle chain that is the repeatable sequence of that ratio. 

If the mole mass of hydrogen is a limited decimal of 5 digits long in decimal place and all the other standard unit measures of other elements are based on the unit measure of mole mass of hydrogen for example 1.00784 to 1.00797 to 1.00811 and these values are incorrect to the degree of precision require of hydrogen weight , then all factoring of all elements is simply rounded and inaccurate. Cyclemetrics of air flow, fluid mechanics of fluidity, structural mechanics of frozen phase matter forms, thermodynamics of heat transfer, electrical engineering, and thermo electromagnetic engineering fields of mid phases between these areas of notation require precision arithmetic. The distance of the hydrogen from the center of the planet or star its atoms are being weighed will vary depending on general relativity to the atomic measure distance and the scale the hydrogen atoms are weighed in relation compared to hydrogen atoms weighed in a different distance to that planet or star. Time, temperature, phase state, and distance are all factors of relative weight measures given differentials of environmental weight comparisons and the effects on weighing instruments in varying conditions.

Open source is open source and logical math hidden in open source contradicts the definition of an open source library so when a number is searched in open source libraries the number should be a result in the number search to the precision of that number and not rounded numbers considering the basic logic principles of computer file storage and arrangement simplicity.

Boolean programs with sql blocks contradict the open source library of numbers being available with sql blocks of logical boolean factored numbers.This page was made out of hobby of numbers and math. An example of a numarable bridge or a near partial number bridge is the process of chemical change made with pollen nectar to glycerides and biological chemical bonding when bees make honey regurgitating changed molecular sugars and the correlation of the localized flowers the nectar is gathered from along with the current phase state of that particular bee dna and its colony. The honey is processed for food storage that time, temperature, light, shade, and environment have significant impact on that food storage of glycerides.

An Ai artificial intelligence program using a simple low digit number bridge can then use a programmed hysteresis loop algorithm to adjust to the user interface when a user is needed to be contained within a loop of paths mazes and bridges eternally in such a prison of limits to simply numbers 0 and 1 and 2 that many strings of decimal number bridges can be affixed to, just as DNA and RNA sequences send signals that the rest of a body of systems may not comprehend a repeated number as more than a musical rhythm. 1∀Y2nd 6 to 7 digits and not ten or more of the examples while other systems are well aware much more complex rhythm sequences exist. Within the 6 to 7 digits of a loop an affixed sub routine program path is easily left dormant with limited access to the information just as is DNA and RNA transcriptions translations. A much more complex path number bridge could be the structure of an entire systems cell membrane container of its own little world where little is a relative term of expression as it contains extremely large variable strings and sequences of information, known as a shell. Elements of the periodic table have structures to their atoms nucleus and structures that are all differing and relative to phase states given an environment just as is an arc of plasma in an appropriate vaccume arc veil. Those phase states, arcs, and time are all numerable to extreme precision whether they are considered whole numbers or partials, fractions, ratios, or percentages to some other comparative unit measure quantity known.

Light, sound, energy, matter, absence of light, and absence of sound are binary parts of physical matter frictions and alignments. Nucleic multi diffraction energy focal point bombardment with subatomic refraction, selective divergence, selective convergence, and valence energy transfer of incorrect transcriptions are world wide sciences and sciences of the stars that worlds are among systems of. Radical pairing is written about and talked about very much, however searching for numbers specific to those subjects is commonly rounded and worded around in a divergence of its own. So again, This page was made out of hobby of numbers and math and here many numbers are very exact to their definitions of those applicable subjects using such numbers.

These variables are applicable to multiple functions of exponential multiplication division addition subtraction and square cube quadratic root or sub unit array potentials where cn is a critical factor of cycle stem shell count precision.

Calculating links ( x ) / ( - ) + ( x ) n3 

1X⅄=(n2xn1) is a function of multiplication applicable to variables of A  B  C  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ    ᗑ  ∘⧊°  ∘∇° just as are functions of exponentials, division, addition, and subtraction of these definable variables. Radical ratios can be multiplied with other ratios or radicals and whole numbers. 1represents a path of consecutive numbers that a number is related with a later consecutive number while 2represents a path of consecutive numbers that a number is related with a previous of consecutive numbers and 3cn represents a path of consecutive numbers that a number is related with a similar of consecutive numbers focused with a differential in decimal stem variations of cn.  Further factoring can be noted with ncn that consecutive numbers of every other or every third, forth, fifth,sixth, seventh,eighth, ninth,tenth, etc... can be formulated as a library of ratios structured for function ncn(nncn/nncn)

10 digit limit fibonacci and prime ratios below applicable to rocket science chemistry or chromatin bases of biological foundation chemistry eg 1 - eg 2 - eg 3 decimal precision is crucial to being accurate or it is not accurate and simply a rounded guess.

Division much like a star changing a grain of sand or a grain of sand that changes a star. After star and sand grain are numerated and their change or no change is numerated, then arithmetic using those variables numerated of those stars and sand grains change and the change those numbers then make in numeral factoring of other numerable physics calculus. 

Eliptic Eponyms and Elcipses Number bridge of plus or minus 1 examples that a path of base Y differs before a 10 digit decimal limit of a consumer market calculator rounding example. Suppose a seed has a seed shell husk that protects the inner fragile structure of the seed proteins and in those proteins are enzymes full of numeral instructions. The seed shell has a numeral structure to its making just at the inner pack does and a purpose. The purpose is to protect the inner makings and instructions biologically formed to make the inner most seed just as an egg does. The seed will understand hydrogen oxygen nitrogen carbon as those are basic elements that likely formed the seed or egg with calcium in the eggs case. Other important nutrients like potassium sodium, sugar compounds together then allow the seed after water germinates and activates the seed to begin growing. Within that "activate" instructions is more neatly packed instructions of what to do next with simple yes no and maybe type path variables as the seed forms roots stems vines leaves that each contribute to conversions of the contact with soil air or water nutrients. DNA and RNA hold within them dormant building block hints so to say or instructions for nucleic transcription as many forms of biologic life can store memory in simple one through ten type libraries of what to do with 1 what to do with 2 what to do with 3 and so on. Variables 1φn8 and 1Θn7 and (Nn8)1∀Y2nd and (Nn7) 1φ2nd each share an identical repeating decimal chain stem of numerals yet the variable (Nn7) 1φ2nd is one/millionth off in decimal place where the repeating stem chain begins within less than a whole number one 1.  If in the order of least numeral quantity to more numeral quantity 1φn8 and 1Θn7 and (Nn7) 1φ2nd and  (Nn7) 1φ2nd 0.615384 : 0.996336615384 : 1.615384 : 2.615384 yet the order of their structuring to that common quotient decimal stem repetition, so the specific definition of correct order then is an opinion to the flow and memory of a functioning system otherwise the system fails and discontinues living that then activates replicate new seed or eggs and reprint original base instructions for regrowth. A sort of change in environment reflected through the slightest evolutionary adjustment to a seed or egg change needed that can only be changed in restarting from seed or egg that the system recognizes.

The are quotients that derived from a base set of common Y variables through division paths that all varied to these numbers so when a seed or egg begins its growth process of life and say is blocked in memory of its original growth instructions yet remembers say a sequence of stem decimal chain in one region of its storage restructured from nutrients other system formations transfer to that region, one might say these PM and MS Mutations mutagens or per-mutations are permeable numeral quotient products of blocked signal transcriptions yet are still able to continue part transactions with the system original instructions until that signal and translation is recorrected such as a branch or stem of a plant re-exposed to dirt will grow roots reaching for oxygen and if exposed to oxygen will then reach to for leaves instead for carbon dioxide to breathe rather than exhale. Within cells are cellular memory and that cellular memory must then have a reading or reference way of comprehending what to do like a reflex. That reflex is then in a way the auto response or autoimmune system instructions of the new shell of a group of cells formed from the original seed or egg.

1Θn7 and (Nn7) 1φ2nd and 1φn8 and  (Nn8)1∀Y2nd or 0.615384 : 0.996336615384 : 1.615384 : 2.615384 for example involve just 4 variables from Y set and a multiple different paths of division with the numerals closest in Y base variables of this example. (Y7/Y8)=(8/13) is 1Θn7 and (Yn9/Yn8)=(21/13) is 1φn8 and (Yn10/Yn8)=(34/13) is (Nn8)1∀Y2nd and n9cn/φn7cn) is (Nn7) 1φ2nd that is (1φn9=(Yn10/Yn9)=(34/21)/1φn7=(Yn8/Yn7)=(13/8)) and is two variables of Y base factors that anyone of the Y base factors may or may not be quotients of some other divided part of some other base equal to its variable value. This being the case identifying and numerating a number bridge to memory is then information vital to counting the number of times a number bridge was used when needing to know what side of the numeral bridge certain receptors using the bridge can evaluate their position when considering only with the number of crossings on that numeral numbered bridge made of numbers and nothing more. A cell might receive a set of instructions for anastasis or autophage to either self consume and prepare for transport with a lighter load so to say or self terminate with thanks and your service has been helpful go decompose type message, while if on one side of a numbered bridge rather than the other side or between various similar bridges at a junction, that decompose instructions message then activates decay decomposition action within a vital region of its system and number bridges that can infact be a mortal complete system over all death. An alternate bridge might be a cell cluster in transport with a chemical reaction waiting in idle between two collectives that have an explosive chemical reaction a simple sub cellular membrane separates those chemicals from and may be vital to not happening in one particular region where that particular cell chemical reaction will be a determining factor in the life longevity to the biology around the chemical reaction at the wrong place and wrong time no matter how "happy" or "unhappy" the system section is..... and since happy or unhappy are chemical signatures for a reader of such emotions neither happy nor unhappy are too as well likely emotions for a reader who reads chemicals as a label of an opinion with such labels. Emotionless chemical signature with a tiny membrane transporting collective compounds able to chemical react though a system of emotional system parts is beyond the fact that emotional or not numbers and number bridges do not alter when emotions are extracted from the care and concern of where and when those chemical reaction potential explosions occur. Continued function is sometimes the only instructions for a thing to be aware of and doing what ever it takes to continue that survival is sometimes all some cells have knowledge of in their given cellular memory.

Within the stem branch or trunk of a plant is cells and they may be exposed at the plant bark so to say with air or soil causing the stem branch or tree trunk to decide grow a new branch here or a new root. When that stem or branch is cut from the system completely it will not have the complete memory of the tree or plant it is cut from, only partial and when replanted then relies on its own formed or unformed roots of its own along with what it has for leaf cola structures. 1φn8 and 1Θn7 and (Nn7) 1φ2nd and  (Nn7) 1φ2nd 0.615384 : 0.996336615384 : 1.615384 : 2.615384 might then be a clone only memory variable set and say no emotional response reflex memory just instructions that the clone can attach memory markers to itself in a new environment it can read recognize and translate. A basic example is a plant with a leaf that gets a powder coat of nutrients spilled on it that the plant will alocate on its own and weep from its leaves directly over the powder chemical spill that is obstructing its leaves from proper function simply to clean itself with the reserve water it has within its reach to transport to that allocated place. Variable change to environment then relies on decisions that plant will react outwardly and inwardly with simply chains of numeral instructions if we use these number paths as an example of what to predict from a plant seed shell and clone cropped cutting. As stems roots branches are splines of a plant bush or tree system whole, so to are RNA of DNA like limbs of a body system and understanding these number bridges or partial number bridge connectors are vital to the engineering and/or repair of such systems. Hibernation is an example of a stasis a circadian clock cell would recognize and its translation of time when woken early or in a clones case distinguishing the difference of time with anastasis factors signatured on cells of the clone would then require an organizational library structured to the memory of that even and recollection of that even for cell memory to be stored in the distinguishing of an event or a mutagen exposure factor a central nervous system so to say stores knowledge memory about how that exposure was solved to continue on.

Although 1-0.996336=0.003664 and 0.996336615384+0.003664=1.00000061538 still 1.00000061538 does not equal 1.61538 nor does 1+1.00000061538 equal 2.61538 and so rounding to a whole number of an assumed one or 2 from 0 or partial ratio rather than an allocated path variable definition in say space travel leaves 000000 many stars of 0 assumed to be the positioning it is not and star travel based on that assumed value then would further the lost travel to even more lost just as it will in medical sciences or other math practical applications.  i.e. e.g. incorrect Substitution bonding fillers... for example, then result in abnormal expected growth results and can be extremely unpredictable over a simple one millionth fraction applied to exponential equational longevity.  

Simply identifying a decimal stem looping value is not as sufficient as identifying the origin of that stem decimal loop and the affixed if any whole number partial of that quotient product sum difference or exponent. With this as an example here on this page very many equations define a quotient product sum or difference that defines zero and how that specific value zero was factored. Being that absolute zero in arithmetic equals 1 (|0|=1) math sciences prove that the value one equaling zero given the micron atomic or subatomic definitions in astronomical math fields of its factors defines values being absolute and accurate to absolution, yet limits in stored libraries of decimal constants non existent through web searches to that specific unit measure should be available and factored as they are simply numbers with a base constant at the decimal repeatable chain stem and its variable factors.

Radioactive isotope resonance in residential settings along with pyro engineering fire sciences of forensics for fire damage to homes and buildings can benefit from the extreme calibration measures of these ratio constants used as standard unit incremental measures in the prevention protocols of future planning as we humans have an ever changing environment among the stars and their astronomical frequencies at this planet we reside on and changes it experiences itself quite frequently at many grades and levels.

Fair Warning copy paste exchange may be completely inaccurate in your use of the values listed.

These numbers are from a quick math calculated in a paper notebook hand written then entered to a digital note book and it is recommended only for explanation of structures to variables in quantum field fractal polarization mathematics.

Some of these quotients were factored through a dcode boolean and manually identified at their stem decimal looping numeral cycle by the author.

Phi Theta Prime Absolute Zero(s) |0|:|0|:|0|:|0||0|

No two absolute 0's can represent other absolute zeros that do not represent the absolute zero it represents itself numerically

The zero of all phases in tier 1 - 2 - 3 - 4 -5 - 6 - 7 - 8 - 9 - 10 etc. of the divides mentioned above require notation of their zero origin.

1φn1=0 2φn1=0 3φn1=0 and so on as 21Θn1=0 22Θn1=0 and so on as 11Θn1=0 12Θn1=0 13Θn1=0 and so on....

if 1φn1=0 and 12Θn1=0  and 22Θn1=0 and nφn1/Pn=0 and Q/nφn1=0 and nΘn1/Pn=0 and Q/nΘn1=0 

Above P represents prime numbers and below P represents pressure.

while triple point (ΔP/ΔS)=0=(ΔT/ΔV)and (ΔS)E<0 equilibrium of a pure substance use zero in the equations, defining what that zero is would seem just as important. Below V represents a path of variables of phi and prime ratio divisions.

So to clarify if (ΔP/ΔS)=0=(ΔT/ΔV) then (ΔP/ΔS)=nφn1=(ΔT/ΔV) and (ΔP/ΔS)=nΘn1=(ΔT/ΔV) and (ΔT/ΔV) 

and (ΔP/ΔS)=nAn1=(ΔT/ΔV) and (ΔP/ΔS)=nMn1=(ΔT/ΔV) and (ΔP/ΔS)=nWn1=(ΔT/ΔV) are true and 

so is  and (ΔP/ΔS)=nVn1=(ΔT/ΔV) as confusing as it is defined here with two meanings of V and P in the same equation.

(ΔP is change in pressure

ΔS is change in entropy

nVn1 is 1(Q/φ)cn that is (prime/prime) ratio divided by (y/y) ratio

ΔT is change in temperature

ΔV is change in volume

So if the equilibrium of a pure substance equation is (ΔS)E<0 then the ratios defined below are applicable to this equation in quantum field fractal polarization to the equilibrium and multi phase points in such a field of numeration. In the equation E represents energy and below E represents a ratio path set notation while on this page there are a multitude of definitions to 0 zero.


Amorphic Mutation or Amorphism are also examples in dna rna labeling within many notations T represents temperature as other notations T represents time. T on this page however represents a ratio set of a defined path T

Measured units and paths of the root to a defined unit measure explained on this page can be very extensive and this page will contain only the basic principles of the unit measure definitions for practical applications of physics, chemistry, calculus, engineering, and probability factoring. Probability and prediction in closed matrices arrays are one factor of probability and probability of a decimal ratio precision or decimal digit length are entirely different factors very closely relative of prediction or pathogen numeration. Incompetent internet computers of basic fractal quantum numerals and calculators limited to rounded precision as well as library limits are part in this pages creation of these real numbers.


A DNA and RNA database with numbers that align to perfect simple numeral division are highly unlikely as accurate and further research in data is likely needed by that database.


Quantum Field Fractal Polarization Math is very much applicable to physical sciences or physics. While it is said that centripetal and centrifugal force equations are the same, electromagnetic properties of varying elements along with varying mass and volume of those elements at the atomic level, the kinetics of centripetal and centrifugal also vary. F=mv²/r is force equals mass times velocity squared divided by radius and M=dm/dv is magnetization equals derivative of magnetic moment divided by derivative volume. Given that M=dm/dv in a field that can vary to an element that also varies in kinetic or magnetic measure then F=mv²/r does not apply to all elements that have differing magnetic properties, weights, mass, volume, and charge potential change. This being the case, exact values and measures of phase points at differential distances from a gravitational point along with varying factors that can effect that gravitational field, centripetal and centrifugal forces are not equal and are partials to much more complex systems in quantum field fractal polarization. One atom for instance may divide protons and electron counts that approach it while other atoms might be divided by approaching protons and electrons counts. Atomic decay or stability are subject to frequency waves of conservation and preservation, and if decayed require repair or an eventual overall change will occur. So if 1 divides 2 or 2 divides 1 for example, the values on one side of entropy and enthalpy of centrifugal centripetal balance are much more precise in ratios than simply 1 and 2 values. H=E+PV enthalpy equals internal energy plus pressure time volume and ΔS=S2−S1 entropy equals change in state measured to a closed value system phase of matter and energy. Factoring precision rather than rounded variable estimates proves that a slight incorrect value on exponential valued factors of systems is not impossible and here on this page are ratios that differ to microns of difference with basic 10 digits fibonnacci and prime based. 


Similarities of plus one and minus one between alternate Y paths for φ and Θ that 1⅄Q and 2⅄Q from P primes differ are numerical constants of the path variable structures. ⅄ncn Paths and exponents in those paths to precise measures in exponents factored correctly produce product values that rounded estimates do not. Factoring nNncn for ⅄ncn is essential for any other algebra, trigonometric, geometric, or calculus formulas, functions and equations to be accurate. 


Paths 1⅄  2⅄  3ncn of numbers and variable N, Y, P, φ, Θ, Q and so on are definitions of variables A, B, D, E, F, G, H, I, J, K, L, M, O, R, S, T, U, V, W, X, Z, ᐱ, ᗑ, ∘⧊°, and ∘∇° while ( / ) or ( ÷ ) represent division of variables that define φ, Θ, A, B, D, E, F, G, H, I, J, K, L, M, O, Q, R, S, T, U, V, W, X, Z, ᐱ, ᗑ, ∘⧊°, and ∘∇° 


Functions then ⅄ncn, X, +⅄, 1-⅄, 2-⅄, represent functions of arithmetic paths that are applicable to variables of sets φ, Θ, A, B, D, E, F, G, H, I, J, K, L, M, O, P, Q, R, S, T, U, V, W, X, Y, Z, ᐱ, ᗑ, ∘⧊°, and ∘∇° with degrees of Nncn  the cycle stem potential change to many variables of these sets derived from division. ( / ) or ( ÷ ) represent division then exponents ncn, multiplication X, addition +, and subtraction  1-⅄, 2-⅄ that sequence is difference of variable can replace the division function  ( / ) or ( ÷ ) of those variables precise to the degree of cycle stem counts of percentage of fractal ratios. Examples of function change to A variables

The percentage of a ratio's repeatable cycle stem decimal is definable two ways.

For example 1φn11=1.6^18 so 1φn11c2=1.6^1818 and 1φn11c1.5=1.6^181 while alternately, if 1φn11=1.6^18 and the repeatable stem decimal cycle is 0.0^18 then 0.018 is a quantity that half of is 0.009 of this example and the cn of these numerals is a definition of full or percent of a chain decimal repeatable cycle of numerals found and not a quantity. The variable is a cell set of numeral instructions and not a quantity so the number of full cycles or percentage should be quantified first before the percent or value of the decimal stem chain is then partially or completely given that value.

50% of 1.618 is 0.809 and 50% of 1.61818 is 0.80909 while 50% of 0.018 is 0.009 and 50% of 0.01818 is 0.00909

The digits of a ratio can be counted and called a percent of that number of variable ratio stem cycle or given the quantity value found in that specific ratio set variable to degrees of Nncn. So 1φn11c1.5=1.6^181 and 50% of 1.6181 is 0.80905 that is not 50% of 1.618=0.809 not 50% of 1.61818=0.80909 not 50% of 0.018=0.009 and not 50% of 0.01818=0.00909 

Before such arithmetic of ratio stem cycle values are quantifiably factorable, those ratios need to be factored very precise.


Prime Proofs

21 prime consecutive previous divided by later cycles back in remainder back to the dividend. 

have not read this anywhere . . . this may help with the mersenne prime search of primes.

if 2P=(pn1/pn2)=21Qn1 consecutive prime previous divided by later cycles back in remainder back to the dividend then the prime no matter the number of digits when previous prime divided by the next later consecutive prime will cycle back to the dividend. The first 45 variables of 2P=(pn1/pn2)=21Qn prove that fact. Link


11Qn1 prime consecutive later divided by previous cycles back in remainder back to the first division remainder.

have not read this anywhere . . . this may help with the mersenne prime search of primes.

if 1P=(pn2/pn1)=11Qn1 consecutive prime later divided by previous cycles back in remainder back to the first remainder then the prime no matter the number of digits when later prime divided by the next previous of consecutive primes will cycle back to the first remainder. The first 45 variables of 1P=(pn2/pn1)=11Qn1 prove that fact. And both 2P=(pn1/pn2)=21Qn equation combined with 1P=(pn2/pn1)=11Qn1 equation can verify as functions of P with Q bases if primes are consecutive no matter the number of digits to the prime numbers. Link


One Third is 33 % percent or 0.33 of decimals to the 100th decimal until a micron unit measure is determined as the smallest measurable point of relativity to that one third 33% and 3.^3333333333 of 10. With many numbers that are often rounded in math factoring, a ratio that is less than 3.^33 consistently is D that represents ratio path set 1n2/Θn1) path from Y base.  1n2/Θn1)=1[1(Yn3/Yn2)] / [2(Yn1/Yn2)] that is a later consecutive divided by previous ratio then divided by a previous divided by a later of consecutive Y base ratio for a ratio divided by a ratio or a quotient divided by a quotient from altering Y path bases. Consistently the ratios near an average of (1.6180339/0.6180339)=2.6180342211001. . .^ extended shell continues and each step of these ratios is a constant that is dependent of cn of the decimal to both divisor and dividend or numerator and denominator that also has a measurable point of relativity like the abundantly estimated 33% of expontential math in geometry and physics. Ratios then from prime base P of alternate paths also have a trait as L represents 1(1Qn2/2Qn1)cn  the variables of set path 1Q quotient to 1.ncn being a whole number one with a ratio or also known as a percentage of some micron unit measure of tenths in decimal to an exponential decimal the ratio cycles a repeated stem of precisely. Subsequently variables of set path 2Q quotients are less than 1 and 0.ncn to a micron unit measure of tenths in decimal to an exponential decimal the ratio cycles a repeated stem of precisely. So then those p prime based Q quotients and Y base φ and Θ quotients of alternate paths then divided again in array sets of defined similar paths are factorable and will not change anymore than the definition of the decimal repeating stem of each ratio factored. 3.^3333 of 33% and pi 3.14159. . . is one set of two ratios while a radius unit measure of a straight line from a center measurable point of relativity is then factored with an arc unit measure of circumference and not like terms. While a scale of pi factors is one scale, then are also Y and P base whole number radicals with a measurable point of relativity. Numbers are very precise and one error in factoring can calculate a cycle of numerals that eventually prove correct or incorrect as these ratios will not change anymore than the definition of the decimal repeating stem, thus they are constants. Variable quotients of function (Nn)2∀Y2nd factor to numbers that are a micro-fraction above 33 percent with each a unique stem cell decimal cycle loop of their own such as (Nn6c1)2∀Y2nd=(Yn6/Yn8)=(5/13)=0.^384615 or 0.384615 or 0.384615384615.... for functions of (Nncn)2∀Y2nd and yet these are not 33% by any means. If a 33% measure is subtracted from each variable of (Nncn)2∀Y2nd a then the cn factor of each variable must be defined specifically for aa correct difference of correct subtraction as equations 0.384615-0.3 differs from 0.384615-0.33 and 0.384615-0.333 and 0.384615-0.3333 and 0.384615-0.33333 and 0.384615-0.333333 and 0.384615-0.3333333 that all equal a difference that is not equal to the math equation 0.384615384615-0.3 or 0.384615384615-0.333333333333 for example and so on for cn...

Nncn 

N is a number and n is the numerated number of a sequence in labeled number scales that C cycles of a decimal numerated consecutive number is labeled to that N number.

As any variable of the ratio scales can be defined as a number to the decimal stem counted degree of sequence repetitions in the decimal cycle count, a number that is not factored from these many computational equations can too also be a number.

4 6 9 10 12 14 15 16 18 20 22 24 25 26 27 28 30 32 33 35 36 38 39 40 42 44 45 46 48 49 50 51 52 54 56 57 58 60 62 63 64 65 66 68 69 70 72 74 75 76 77 78 80 81 82 84 85 86 87 88 90 91 92 93 94 95 96 98 99 100 and so on . . .

These whole numbers are variables that are neither Y base fibonacci numerals nor are they prime numbers and yet these numbers are still factorable numerals of a set entirely different than Y, P, A through Z, φ, and Θ.

In this case we note the set as (N) of Ψ such that psi represents N whole numbers that are not prime nor fibonacci based numerals and are an ordinal set of consecutive values.

N then is a number and N represents any number of any set including numbers that can not be defined to any of these sets.

A  B  D  E  F  G  H  I  J  K  L  M  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇°  ∀

As C cycles of repeating ratios are numerable then cn or CN is a cycle count of N many cycle counts that its self can be whole and partial of...

The values will display in the tier order of their group(s) of array respectably.

Denny Constants

Prime Proofs Link 1 and Link 2 along with Number bridges Link 3 are key points in Quantum field fractal polarization math.

Refer to these as Denny's Constants, a library published that quantum field fractal polarization math is a math that has not been invented and this math is math I wrote out many times. My name is Denny and this is a version of that math that defines quantum fractals able to be plotted to field points for polarization calculus of those values in numerals. Basic division array sets and libraries of constants. A LIST of ACQFPS

To Begin

1st tier fibonacci 01 to 10 digit value for basic numerical display of decimal precision laws not applicable to standard definition floating point. 9 bold numbers are also prime numbers in the ten digit base logic that phi prime fibonacci scale bases share in common of the ten digit example shown below. 2 - 3- 5 - 13- 89 - 1597 - 28657 - 514229 - 434894437

0  1  1  2  3  5  8  13  21  34  55  89  144  233  377  610  987  1597  2584  4181  6765  10946  17711  28657  46368  75025  121393  196418  317811  514229  832040  1346296  2178309  3524578  5702887  9227465  14930352  24157817  39088169  63245986  102334155  165780141  269114296  434894437  704008733  1138903170

2nd tier 1st divide 1φn ratios of Y fibonacci 1-21 step in decimal value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored ratios of previous order as divisor example 1/0 1/1 2/1 3/2 5/3 8/5 13/8 21/13 34/21 55/34 89/55 144/89 . . .  y1φn

11Y=(Y2/Y1) φn21(Yn22/Yn21) = φn  variables 

21Y where numbers of y dividing previous by the later do not equal φ ratios will be noted theta Θ

31Y where numbers of y have no decimals to apply path variant of cn & do not equal phi ratio σ

(Yn8/Yn7) (Yn9/Yn8) (Yn10/Yn9) (Yn11/Yn10) (Yn12/Yn11) (Yn13/Yn12) (Yn14/Yn13) (Yn15/Yn14) (Yn16/Yn15) (Yn17/Yn16) (Yn18/Yn17) (Yn19/Yn18) (Yn20/Yn19) (Yn21/Yn20) (Yn22/Yn21) (Yn23/Yn22) (Yn24/Yn23) (Yn25/Yn24) (Yn26/Yn25) (Yn27/Yn26) (Yn28/Yn27) (Yn29/Yn28) (Yn30/Yn29) (Yn31/Yn30) (Yn32/Yn31) (Yn33/Yn32) (Yn34/Yn33) (Yn35/Yn34) (Yn36/Yn35) (Yn37/Yn36) (Yn38/Yn37) (Yn39/Yn38) (Yn40/Yn39) (Yn41/Yn40) (Yn42/Yn41) (Yn43/Yn42) (Yn44/Yn43) (Yn45/Yn44) (Yn46/Yn45)

φ denotes ratio phi tier 2nd tier first divide quotient ratios before 3rd tier second divide of (φn2/φn1) variable constants where (Yn22/Yn21)=φn21=1.6^1803399852 or φn21c2=1.6^18033998521803399852 . . . and so on that φn21 φn22 and φn21c2φn22 

1φn=11Y=(Y2/Y1)  phi ratios cycle back in remainder and vary per step in the ratios

have not read this anywhere . . .

1φn1=(Yn2/Yn1)=(1/0)=0

1φn2=(Yn3/Yn2)=(1/1)=1

1φn3=(Yn4/Yn3)=(2/1)=2  

1φn4=(Yn5/Yn4)=(3/2)=1.5  

1φn5=(Yn6/Yn5)=(5/3)=1.^6  and 1φn5c2=1.^66  and so on for cn

1φn6=(Yn7/Yn6)=(8/5)=1.6

1φn7=(Yn8/Yn7)=(13/8)=1.625

1φn8=(Yn9/Yn8)=(21/13)=1.^615384  and 1φn8c2=1.^615384615384 and so on for cn

1φn9=(Yn10/Yn9)=(34/21)=1.^619047 and 1φn9c2=1.^619047619047 and so on for cn

1φn10=(Yn11/Yn10)=(55/34)=1.6^1762941 and 1φn10c2=1.6^17629411762941 and so on for cn

1φn11=(Yn12/Yn11)=(89/55)=1.6^18 and 1φn11c2)=1.6^1818 and so on for cn

1φn12=(Yn13/Yn12)=(144/89)=1.^61797752808988764044943820224719101123595505 

and 

1φn12c2=1.^6179775280898876404494382022471910112359550561797752808988764044943820224719101123595505 and so on for cn

1φn13=(Yn14/Yn13)=(233/144)=1.6180^5 and 1φn13c2=1.6180^55 and 1φn13c3=1.6180^555 and so on for cn cycles of decimal numbers

1φn14=(Yn15/Yn14)=(377/233)=1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832 

1φn15=(Yn16/Yn15)=(610/377)=1.6183^0223896551724135014 

1φn16=(Yn17/Yn16)=(987/610)=1.618^032786885245901639344262295081967213114754098360655737704918 

1φn17=(Yn18/Yn17)=(1597/987)=1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843 

1φn18=(Yn19/Yn18)=(2584/1597)=1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129 

1φn19=(Yn20/Yn19)=(4181/2584)=1.6180340557314241486068^11145510835913312693 

1φn20=(Yn21/Yn20)=(6765/4181)=1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242 

1φn21=(Yn22/Yn21)=(10946/6765)=1.6^1803399852

1φn22=(Yn23/Yn22)=(17711/10946)=1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981 

1φn23=(Yn24/Yn23)=(28657/17711)=1.6180339901755970865563773925808819377787815481903901530122522725989498052058043024109310597932923042177178024956241883575179831742984585850601321212805601038902377053814013889673084523742307040822087^96792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869


NOTE* 1φn24 divisor 28,657 and the decimal repeating stem cycle is 28,656 digits long and its decimal digit length to the stem cycle repeating probability is exactly 1 less than the divisor. This is a probability limit and is not the case for all ratios of long division as some have values with repeating decimal stems far before the probability to divisor example here with much shorter quotients.

When two programs are unable to print out and report an error or display as incompatiable with something as simple as long division quotients, those programs are then similar to what in cell transcription and translation transpons and retranspons as junk discard programs as they are unable to carry out such simple logic expressions of division. The other factor may be those programs are harboring an ulterior motive in the handshake between program softwares that are not what the initial handshake was initiated for and thus are limited to memory limit or function limit. Numbers are limitless and usually the calculator is the limited reason for a answer not being complete or accurate. The whole number 1 in  1φn24c1 is one digit and 28,656 digits of repeating decimal chain is exactly the number value of the divisor 28,657 although 1φn24c2 then has 57,312 digits as a defined variable... and so on for cn of these ratio values in quantum fractal polarization math. 


The divisor is much like a simple task as counting cards in a game of poker that has a deck of 52 cards of 4 suits divided among the number of players at table hands dealt and the odds of all possible hands after seeing the flop. It is an array of logic that pertains mainly to the divisor and the limit of the divisor then factoring and a sequence of a ratio that can be calculated to a quotient again and again for a repeatable chain within the limits of an array set. With 3 cards dealt to the flop, and two cards dealt to each player from 13 cards of 4 suits, the turn card, and the river card, each then allow for simpler odds counting to the two cards a player is dealt when factoring the total number of two cards per player at the table to a hand and its probability of being the best hand possible, yet these poker card arrays of probability are a less complex factoring as compared to quantum fractal polarization math constants. As accurate as these values are that far exceed 52 cards of 4 suits to 13 similar variables in set values to hands in that game, the more hands dealt at a table in a hand of poker simply allow for easier factoring when compared to the hand one player is dealt in combination with the flop, turn card, and river card. 


Cellular chemical structures based on limits of cell memory instructions and paths then are able to carry in them a shorter expression of the dividend and divisor for example as factors of a variable with an extremely long answer when carried out on say an "ACTIVATION" signal and when that signal is received, the cell chemical system is then preoccupied unraveling the prepackaged micro cell subatomic division sequence that has only one answer before the repeating cn of that quotient number is completed and able to double triple or multiple more than one cycle of that numeral value sequence. "IDENTIFY" and "DEACTIVATE", "DELETE" or "KEEP" "COPY" or "DO NOT COPY and SAVE" are then a set of basic instructions for what to do with unknown cell chemical structure instruction packages. If deleted the deleted then becomes part in junk discard and its own chemical making make appear in something such as a snail shell like a colored pattern of something discarded from a snails nutrient intake and discard process.


1φn24=(Yn25/Yn24)=(46368/28657)=1.^618033988205325051470844819764804410789684893743238999197403775691803049865652371148410510520989636040060020239383047771923090344418466692256691209826569424573402659036186621069895662490839934396482534808249293366367728652685207802631119796210350001744774400669993369857277454025194542345674704260739086436123809191471542729525072408137627804724849077014342045573507345500226820672087099138081446069023275290504937711553896081236696095194891300554838259413057891614614230380011864465924555954915029486687371322887950587988973025787765641902502006490560770492375335869072128973723697525909899849949401542380570192274138953833269358271975433576438566493352409533447325260843772900164008793662979376766584080678368286980493422200509474124995638063998325016575356806364937013644135813239348152283909690477021321143176187318979655930488187877307464144886066231636249432948319782252154796384827441811773737655721115259796908259762012771748612904351467355270963464424049970338835188610112712426283281571692780123530027567435530585895243744983773598073769061660327319677565690756185225250375126496144048574519314652615416826604320061416058903583766618976166381686847890567749589978015842551558083539798304079282548766444498726314687510904840004187458561607984087657465889660466901629619290225773807446697142059531702550860173779530306731339637784834420909376417629200544369613009037931395470565655860697211850507729350594968070628467739121331611822591338939875074152912028474718218934291796070768049691174931081411173535261890637540566004815577345849181700806085773109536936874062183759639878563701713368461457933489199846459852741040583452559584045782880273580626025054960393621104791150504239801793628083888753184213281222737899989531353595980039780856335275848832745925951774435565481383257144851170743622849565551174233171650905537913947726558955926998639075967477405171511323585860348256970373730676623512579823428830652196670970443521652650312314617719928813204452664270509823079875772062672296472066161845273406148584987961056635377045747984785567226157657814844540600900303590745716578846355166277000383850368147398541368601039885542799316048434937362599015947238022123739400495515929790278117039466796943155250026171616010049900547859161810377918135185120563911086296541857137872073140942876086122064417070872736155215130683602610182503402310081306487071221691035349129357574065673308441218550441427923369508322573891195868374219213455700177966988868339323725442300310569843319258819834595386816484628537530097358411557385630038036081934605855462888648497749241023135708552884112084307499040374079631503646578497400286143001709878912656593502460131904944690651498761210175524304707401333007642111874934570959974875248630352095474055204662037198590222284258645357155319817147642809784694838957322818159611962173290993474543741494224796733782321945772411627176606064835816728896953623896430191576229193565272010329064451966360749555082527829151690686394249223575391701852950413511532958788428656174756603971106535924904909795163485361342778378755626897442160728617789719789231252399064800921240883553756499284642495725302718358516243849670237638273371253096974561189238231496667480894720312663572600062811878424119761314861988344907003524444289353386607111700457130892975538262902606692954600970094566772516313640646264438008165544195135568970932058484837910458177757615940258924521059427016086819974177338870084098126112293680427120773284014376941061520745367623966221167603028928359563108490072233660187737725512091286596643054053110932756394598178455525700526921869002337997696897791115608751788393760686743204103709390375824405904316571867257563597026904421258331297763199218341068499842970303939700596712845029137732491188889276616533482220748857172767561154342743483267613497574763583068709215898384338904979586139512161077572669853787905223854555605960149352688697351432459782950064556652824789754684719265798932198066789964057647346198136580940084447080992427679101092228774819415849530655686219771783508392364867222668109013504553861185748682695327494155005757755522210978120529015598283141989740726524060438985239208570331856091007432738946854171755592001954147328750392574240150748508217887427155668772027776808458666294448127857068081097114143141291830966256063091042328226960254039152737551034651219597306068325365530236940363610985099626618278256621418850542624838608367938025613288201835502669504833025089855881634504658547649788882297518930802247269428062951460376173360784450570541229019087831943329727466238615347035628293261681264612485605611194472554698677461004292145025648183689848902536901978574170359772481418152632864570611019995114631678124018564399623128729455281432110828069930557978853334263879680357329797257214642146770422584359842272394179432599364902118156122413371951006734829186586174407649090972537250933454304358446452873643437903479080154935966779495411243326237917437275360295913738353630875527794256202672994381826429842621349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1φn25=(Yn26/Yn25)=(75025/46368)=1.61803^398895790200138026224982746721877156659765355417529330572808833678

1φn26=(Yn27/Yn26)=(121393/75025)=1.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589

1φn27=(Yn28/Yn27)=(196418/121393)=1.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575

1φn28=(Yn29/Yn28)=(317811/196418)=1.6^180339887383030068527324379639340589966296367949984217332423708621409443126393711370648311254569336822490810414524127116659369304238919040006516714354081601482552515553564337280697288435886731358633119164231384089034609862639880255373743750572758097526703255302467187324990581311285116435357248317363989043773992200307507458583225569957946827683817165432903298068405135985500310562168436701320652893319349550448533230152022727041309859585170401897993055626266431793420154975613233003085256952010508201895956582390615931330122493865124377602867354315795904652323106843568308403506806911790161797798572432261808999175228339561547312364447250252013562911749432333085562422995855776965451231557189259640155179260556568135303281776619250781496604180879552790477451150098259833620136647354112148581087273060513802197354621266889999898176338217474976835116944475557229989104868189269822521357513058884623608834220896251871009785253897300654726145261635898950198047022167011170055697542995041187671191031371870195195959637100469407080817440356790110885967681169750226557647466118176541864798541885163274241668278874644889979533443981712470343858505839587003227810078506043234326792860124835809345375678400146626072966836033357431599955197588815688989807451455569245181195206142003278721909397305745909234387887057194350823244305511714812288079503915119795538087140689753484914824506918917818122575324053803622885886222240324206539115559673756987648789825779714690099685364885091997678420511358429471840666334042704843751590994715351953486951297742569418281420236434542659023103788858454927756111965298496064515472105407854677269903980286939078903155515278640450467879725890702481442637640134814528200063130670305165514362227494425154517406754981722652710036758341903491533362522783044323839973933142583673594069789937785742650877210846256453074565467523343074463643861560549440478978505024997708967609893186978790131250700037674754859534258571006730544043824904031198769970165667097720168212689264731338268386807726379456057998757751326253194717388426722601798205867079391909091834760561659318392408027777494934272826319380097547067987658972191957967192416173670437536274679510024539502489588530582736816381390707572625726766385972772352839352808805710270952764003299086641753810750542210998991945748353002270667657750308016576892138195073771242961439379282957773727458786872893522996874013583276481788838090195399606960665519453410583551405675650907757944791210581514932440000407294647130100092659532222097771080043580527242920709914569947764461505564663116414992515960858984410797381095418953456404199207811911331955319777209828019835249315235874512519219216161451598122371676730238572839556456129275320999093769410135527293832540805832459346903033326884501420440081866224073150118624565976641651987088759685975827062692828559500656762618497286399413495708132655866570273600179209644737244040770194177723019275219175431986885112362410777016363062448451771222596707022777953140750847681984339520817847651437240986060340701972324328727509698703784785508456455111038703173843537761304972049404840696881141239601258540459632009286317954566282112637334663829180624993636021138592186052194809029722326874319054261829363907584844566180288975552138806015741938111578368581290920384078852243684387377938885438198128481096437190074229449439460741887199747477318779337942551090022299381930372980073109389159852966632386033866549908867822704640104267429665305623720840248857029396491156614974187701738129906627702145424553757802238084085979900009164129560427252084839474997199849300980561862965715973077823824700383875204920119337331609119327149242941074646926452769094482175768004968994694987221130446293109592807176531682432363632660957753362726430367888890020262908694722479609811728049364111232168131230335305318249854901281959901841990041645877669052734474437169709497092934456108910588642588764777158916188943986803653432984756997831156004032217006587990917329368998767933692431447219704915028154242482868168905090164852508425908012503945666894072844647639218401572157337922186357665794377297396368968220835157673940270239998370821411479599629361871111608915679825677891028317160341720208942153977741347534340029936156564062356810475618324186174383203168752354672178720891160687920659002739056501949923123135354193607510513293079045708641774175482898716003624922359457890824669836776670162612387866692461994318239672535103707399525501736093433392051644961256096691749228685761997372949526010854402346017167469376533718905599283161421051023836919223289107922899123298272052459550550356891934547750206192915109613171908888187436996609272062641916728609394251036055758637192110702685089961205184860857966174179555845187304625848954780111802380637212475435041594965838161471962854728181734871549450661344683277500025455915445631255791220763881110692502723782952682544369660621735278844097791444775937032247553686525674836318463684591025262450488244458247207486075614251239703082202242157032451201010090724882648229795639910802472278508079707562443360588133470455864533800364528709181439582930281338777505116639004571882414035373540103249193047480373489191418301784968791047663656080399963343481758290991660642100011200602796077752548137136107688704701198464499180319522650673563522691403028235701412294188923622071296927980124021220051115478214827561628771293873270270545469356168986549094278528444439918948365221110081560753087802543555071327475078658778727000580394872160392632039833416489323789062102251321162011628262175564357645429644940891364335244224052785386268060972008675375983871131973648036330682524004928265230274211121

1φn29=(Yn30/Yn29)=(514229/317811)=1.^618033988754322537608830405492572629644663022991652271318488032195235533068395996362

1φn30=(Yn31/Yn30)=(832040/514229)=1.618033988748203621343798191078293911856390 extended shell factoring to divisor 514,229 potential digits long and less  and likely very less given the probability of the factors scale relation.

1φn31=(Yn32/Yn31)=(1346296/832040)=1.6^180664391135041584539204845920869188981298976010768713042642

1φn32=(Yn33/Yn32)=(2178309/1346296)=1.618^001539037477642360966681918389418077451021172164219458425190299904330102741150534503556424441578969260846054656628260055738114055155775550101909238384426604550559460920926750135185724387504679505844182854290586914021879289547023834283099704671186722682084771848092841395948587829125244374194085104612952872176698140676344578012561873466161973295619982529844848384010648475520984983985691111018676427769227569568653550185100453392121791938771265754336342082276111642610540326941474980242086435672392995299696352065221912566033026912358054989393120086518863608002994883740277026745975624974002745310095253941183810989559502516534253982779418493407096210640156399484214466952289838193086810032860529928039599018343662909196788819100702965766815024333430389750842311051952913772305644523938272118464290170957946840813610082775258932656711451270745809242543987354935318830331516991805665321742024042261137223909155193211596855372072709121916725593777297117424399983361756998460962522357639033318081610581922548978827835780541574809700095669897258849465496443575558421030739153945343371739944261885944844224449898090761615573395449440539079073249864814275612495320494155817145709413085978120710452976165716900295328813277317915228151907158604051412170874755625805914895387047127823301859323655421987438126533838026704380017470155151615989351524479015016014308888981323572230772430431346449814899546607878208061228734245663657917723888357389459673058525019757913564327607004700303647934778087433966973087641945010606879913481136391997005116259722973254024375025997254689904746058816189010440497483465746017220581506592903789359843600515785533047710161806913189967139470071960400981656337090803211180899297034233184975666569610249157688948047086227694355476061727881535709829042053159186389917224741067343288548729254190757456012645064681169668483008194334678257975957738862776090844806788403144627927290878083274406222702882575600016638243

1φn33=(Yn34/Yn33)=(3524578/2178309)=1.618033988749989097047296779290725053240839568674600 extended shell factoring to divisor 2,178,309 potential digits long and likely very less given the probability of the factors scale relation.

1φn34=(Yn35/Yn34)=(5702887/3524578)=

1.6^180339887498588483500719802484155549969386405975410389555856048582269990903875584538063847643604425834809160132078223265310059814252940352008098558182000795556233966165594859866911726737215065179434247163773932652362921178081461099740167475368682435173799530043029264780067287488034028470926164777740767830928979299082046134317356574318968114764377465898045099299831071975141421185741952653622646455831024309860641472539407554606537293258937665729060330059371646761683242646353691136924760921733041515892115311393307227134709460253113989816653227705557941972060201249624777774814460057345872328545431538186982952285351608050665923693559909867223820837558425434193824054964878064834995849148465433308611697627347160426014121406874808842363539691843959759154145545934860854263971459845689327913866567855783018562789644604261843545525166417085960361779481118023207317301532268543922137628958700871423472540542442244149512367154308969754677013815554656472349313875306490592632649922912757215190017074384507875836483119397556246449929608594277102109812862702995933130150616612825705658946971807688750256059023236256936291380131181662031596406718761792191859564464171313558672839698823518730469293061467216784534205229675722880866872573113717443620200772971969977682434606355711236919710671745667140860551248972217383187434070121302465146182039381735912781615274225737095334533666158047857076790469667574387628816839916721945152015361839062718997848820482906038680375352737263865347851572585427248311712778097122549139216099062072111895381518014355193728156959499832320351542794626760990961187410237480912608544909489873681331495571952159946524094515712235620831770498482371506603059997537293826381484535169884167693267108856719868307638531478094682540718349827979406328927888672062300791754360380164660847341156870411152767792342799620266596454951486390711171663671509043068418403564909047267502662730119747669082653299203479111541864018898148941518672590023543244042265485399954264028204227569938869277400017817735910511839999001298878901247184769353948188974680089361052585586132580978488772272879192913307635694259000651992947808219877670461541778902325328025085556341780491168020682192307845081028140106418413778897785777474636679908913918205243294374532213501871713436331952364226298864715151714616615095480934171410024122036737447717145144752080958344516705262303742462218171934342210613582675713234321952869251297602152654871022857204465328898949037303189204494835977526955000002837219094030547770541608101735867386109769736972766668804038384169679320474678103307686764202693201852817557165708916074491754757590837825124029032695545395789226398167383442783788584051764494926768537963977531494550553286095526897120733318995919511498965266196407059228083475525296929164285766976926031995887167201293317951822884895723686637095277789284277436901665958307632857039906621445177266611775934594155669132588355258416752303396321488700207514204537394263937413216560961340620068558562188154156327367418170345499517956475924209933784980783515076131099950121688326942970193878529571483451352190248024018761962425005206297037546055158943850866685316653511427467345026837255410434951361553071034319569605212311942025399920217399075860996692369980179187409102593274996325801273230440637148617508252051734987848190620267163898770292500265279985291856216545640357512303600601263470406953683533177588919865016464382402659268712452951814373238441594993783652964979069834743336649096714557033494506292668228650351900284232608839980275652858299631899194740476732249931764880788565326118474325153252389364060037825804961615262876860719212342583991615450133320925228495439737750164700568408473298079940350305767101763672133231269105124074428201049884553555063897011216661966340367556059193469402578124246363678148135748449885347976410225564592413616608853598927304204928930498913628808895703258659618257845336377858569167713127642514933702701429788190245754243486737986788773010556157361250056035077107103318468196760009283380875667952305212141708879758087351166579374892540326813593003190736593146754022751092471212156462419047046199573395737021566837221363805822994979824535022348774803678624788556247017373427400386656218134483050169410352104564007379039419754648641624614350994643897794289131918771552225543029548501976690542811082631736338364479378807902676575748926538155773542251015582574708234574465368620016353730857992077349401829098405539613536712763911027078986477246354031603216044587465506508864323615479640399503146192253370474422753589224014903344457123661329100959036798164205757398474370548757893852824366491534589389141054617035003906850692480064280035794356090289390673152927811499702943160855001648424293631748254684674307108538951329776217181177434575146301202583685195787978021766010001764750276487000713276880239279709514160276776397060867996111874953540537335249780257381167334075171552452520557070945798333871459221501127227146058336629236180898819660112501411516499280197515844450030613594024589610444143951417730009096124415461936152356395574165190839867921776734689940185747059647991901441817999204443766033834405140133088273262784934820565752836226067347637078821918538900259832524631317564826200469956970735219932712511965971529073835222259232169071020700917953865682643425681031885235622534101954900700168928024858578814258047346377353544168975690139358527460592445393462706741062334270939669940628353238316757353646308863075239078266958484107884688606692772865290539746886010183346772294442058027939798750375222225185539942654127671454568461813017047714648391949334076306440090132776179162441574565806175945035121935165004150851534566691388302372652839573985878593125191157636460308156040240845854454065139145736028540154310672086133432144216981437210355395738156454474833582914039638220518881976792682698467731456077862371041299128576527459457557755850487632845691030245322986184445343527650686124693509407367350077087242784809982925615492124163516880602443753550070391405722897890187137297004066869849383387174294341053028192311249743940976763743063708619868818337968403593281238207808140435535828686441327160301176481269530706938532783215465794770324277119133127426886282556379799227028030022317565393644288763080289328254332859139448751027782616812565929878697534853817960618264087218384725774262904665466333841952142923209530332425612371183160083278054847984638160937281002151179517093961319624647262736134652148427414572751688287221902877450860783900937927888104618481985644806271843040500167679648457205373239009038812589762519087391455090510126318668504428047840053475905484287764379168229501517628493396940002462706173618515464830115832306732891143280131692361468521905317459281650172020593671072111327937699208245639619835339152658843129588847232207657200379733403545048513609288828336328490956931581596435090952732497337269880252330917346700796520888458135981101851058481327409976456755957734514600045735971795772430061130722599982182264089488160000998701121098752815230646051811025319910638947414413867419021511227727120807086692364305740999348007052191780122329538458221097674671974914443658219508831979317807692154918971859893581586221102214222525363320091086081794756705625467786498128286563668047635773701135284848285383384904519065828589975877963262552282854855247919041655483294737696257537781828065657789386417324286765678047130748702397847345128977142795534671101050962696810795505164022473044999997162780905969452229458391898264132613890230263027233331195961615830320679525321896692313235797306798147182442834291083925508245242409162174875970967304454604210773601832616557216211415948235505073231462036022468505449446713904473102879266681004080488501034733803592940771916524474703070835714233023073968004112832798706682048177115104276313362904722210715722563098334041692367142960093378554822733388224065405844330867411644741583247696603678511299792485795462605736062586783439038659379931441437811845843672632581829654500482043524075790066215019216484923868900049878311673057029806121470428516548647809751975981238037574994793702962453944841056149133314683346488572532654973162744589565048638446928965680430394787688057974600079782600924139003307630019820812590897406725003674198726769559362851382491747948265012151809379732836101229707499734720014708143783454359642487696399398736529593046316466822411080134983535617597340731287547048185626761558405006216347035020930165256663350903285442966505493707331771349648099715767391160019724347141700368100805259523267750068235119211434673881525674846747610635939962174195038384737123139280787657416008384549866679074771504560262249835299431591526701920059649694232898236327866768730894875925571798950115446444936102988783338033659632443940806530597421875753636321851864251550114652023589774435407586383391146401072695795071069501086371191104296741340381742154663622141430832286872357485066297298570211809754245756513262013211226989443842638749943964922892896681531803239990716619124332047694787858291120241912648833420625107459673186406996809263406853245977248907528787843537580952953800426604262978433162778636194177005020175464977651225196321375211443752982626572599613343781865516949830589647895435992620960580245351358375385649005356102205710868081228447774456970451498023309457188917368263661635520621192097323424251073461844226457748984417425291765425534631379983646269142007922650598170901594460386463287236088972921013522753645968396783955412534493491135676384520359600496853807746629525577246410775985096655542876338670899040963201835794242601525629451242106147175633508465410610858945382964996093149307519935719964205643909710609326847072188500297056839144998351575706368251745315325692891461048670223782818822565424853698797416314804212021978233989998235249723512999286723119760720290485839723223602939132003888125046459462664750219742618832665924828447547479442929054201666128540778498872772853941663370763819101

1φn35=(Yn36/Yn35)=(9227465/5702887)=1.6180339887499085989254214575880602228309977  extended shell factoring to divisor 5,702,887 potential digits long and less and likely very less given the probability of the factors scale relation.

1φn36=(Yn37/Yn36)=(14930352/9227465)=1.6180339887498895958965978196611962223644305342799999   extended shell factoring to divisor 9,227,465 potential digits long and less and likely very less given the probability of the factors scale relation.

1φn37=(Yn38/Yn37)=(24157817/14930352)=1.6180^33988749896854407719255379913346986059002493712137530314087705366892890402048123178877497328931025872665292820959613008454187818210849951829668851745759242648800242619865894655397273955764740174913491657798824836815635692982991961609478463736153039124596660547587893440154659448082670790347072862046387117999629211689047920638441746048586128444928826862219993205786440935886843123323549237151274129370827961725215855594027521923126795670992887508613326732015427365677647787540441109492930910135273434946476814478319064413216781493162384918989183912073874748565874401353698827730250432139845061924862856548861004750591278758866502276704527796799432458122889534017684244818876339955012447127837307519608378958513503231538010624263915545996504302108885309602881432400254193605080442845553808778252515412898503665553230091293226040484511014877613066322883747148091351094736413448256276878133884586244182320684736702791735921564340880911581990833169907849459945753455779207348895725968148641103706061317241549295019970058308069360990283417296524556152460437637371175173900789479042423112328497010653198263510465125001741419090454129949514921014588269586678197540151766013286223928277109608668301993147917745006949601724058481675448777095141494319758837567928740059176099799924342038285500569577997893150811179803396463794021735053533901946852961001857156482312004432313451149711674580746656207435698769861554503202603662659795294846363970521257636792488214611417065049772436711472040310904927090801342125088544462983859992048412522357142015138022198003101333444784155122397650102288278266982586880737975903046358183651664743068348288104660894800069013778107843673076160562055067422388969797898937680772697120603720528491223783605369786325198494985248840750707016150724376759503057931922837452191348201301617001394206914880506501119330609218054604472821538299967743560232203500627446693822088052579068464025496518769282867543913231248667144619229339000178964300372824431734764190422302166754005531818673799519261166782939879783142420218893700563791128300257087039876889707623772031630600537750215132235328410207609304857648366227400398865344902785949051971447156771655484076999658146037012389259141378582366979693445941529040976394930273579618216636821422562575885685749404970492323288828019593911784531268921188194357373489921737946968698393715030965110534567436856143780133248030588964011029344787048557194096964358241520360672005589687369728456502566048007441485639454448227342530169415965544549786903885454274621254743357691767749347101796394351586620328844222828771886958860715407111634072659505951366719284314261311454679702126245918381562604820033713873591191955822608870842428899198089904377338190017221295251444842023818326587343687543334544289377772205236688324561939330030531095315100407545649292126535261861207291027030039211399704440993755539052260790636416341691073324995954549497560405809588414258418019883255264175955128184519695182002406909093636908225606469291547848302571834877034379363594374734098700419119388477913983541714220803367529446057266432834269413072109753340041815491021243169618505980301067248782882011087213482977494435496229425803222857706234923329336106744167853510754468481386105297450455287323433499759416254888029431590092450599959063255842862914417556933687832678023934063979201562026133074424501177199305146991845872086605861670240594461537142593824981487375515326095459772147367992395624697930765463533612603373316315650160156974195919828280003043464748855217880998385034726575769948357547096009524758692896188917716072601637255437782042914996243892977205092016584739596226532368426410844164960075958021619316142044072370162471722033077317935973646167216955099250171730713381707276559856056977089354624726865113428002233303005850096501408674088862740811469146876108480228731378871710459338132148525366314203442758750764884846653314000902322999484539949225577534943583379681872202343253528115077260067277717229975555834182610028216347477942917889678689424067161979838117681351384079893092942483874459222394756667491831404912623627359890778194646716969566424153965023731523543450281681235646688035218459685344324098989762599033164120979867052029315852700592725476264725707739509423488475020548745267358733404276067972141581122802730973790838956777442353669893382285963519145429391082005300343890083770295569722669632973154283301559132698277977639107236051768906721020375139179571921680078272769456473631700042972864939821914446491281652301298723566597760052810543247741245484366343137790723219385584479187094852150840114151360932414721367587314753195370075668678139671455837076044824663209547906171267763814275778628661936436595734648453030444292271207001683550394525192708115655947026567089643968206509799634998558640814362581672555342298694632249795584189843615207464633117826023123902236196440646543363478637342240825936320858342790578547645762136083596689481935857908775359080616451641595589976713208101188773044332779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1φn38=(Yn39/Yn38)=(39088169/24157817)=1.^618033988749894081903178586045254006187727972274978322751596305245627119370926603177762295326601737234784086658161207198481551540853215338124301545955083607099101711052782625185048798076415596657595344811164021980959620647842476826445038473468029002786137505719163283669215641462968280619064214287242924308930728302147499502955916919148779047378328927651037343316244178851094037180594587664936778020961082700477447941591742333340798135858053730599913063336807295129357093813567674595763350637187126634827973073891568927771909191960515306494788001747012157596855709272075370055166822399557046069187460108667931378071122899887849965913724737628404089657604410199812342315532897695184958144189932393311862574337739208803510681449404141110929021442624555024984252509239555875433612234085554998615975938554381796997634347507475530591195388225682809005466015410250023832865361965445801663287705176341057637782420489401008377536761703261515723875216042906525866968857326802334830171120180271255469813352754514201345262280942023859192244067417184259653924855875843417474352090671106582188282989311492838943187623285663601144093441886740014629633132828185593093945533240855330595475576290688848251479014018526591206481943298105122660710609737626541338565483793506673222998584681720206755436552897142982745502211561582737380616799936848598530239714954376879334751149079405643316198644935508866550317853637189154963794948856512987079917030582688824904998659440130703862853170880464902933903340686784737213631513145413759860835107741730140600038488577010083320028461180908854471411882952834687008350133623414731554593695282980246104190622853050008616258662775696992820170796061581226482508746547753052355682634734752730348110510150813709699017920369212168467043193513718561573671991968479602275321482897233636631985414907315507854041613114297537728678050669892896365594623057207528312678252343744469957695266919192243239527809983824283460711702551600585433692125410172616176370571893975353816116745979158630103042837024553998401428407210800545430077560402084343962039285254954948950892375747361609701737536963708268839026307716462956897140167921629673740801993822537855966041964801703730101109715335619936188770698941878730184933514481047687380031068204548449058952636324714273644841336450226442231928489233940301807899281627971600248482716795147508568344565239483352324425671408968782237236088012422645638883678935062716966520609043441301008282329483661541106963431339843331042701416274492020533146682914271599954581988927227985873061295232098165161198133092903220518642061076959064637338713179257877481231023481964450678635408157947384070340461640221879319642167998871752360736899364706670308827987230799869044458777049267324112936197836087590199064758210561823529005124924988048382020610554339409061671425029836098187183055488829971681630008208109201257712979612354874614705459520618108829949328616902760708883588281176233763174876272967876195104880544463102771247915322812487568723614389495540925738447310864222541299985838952253011933983935717370489229221332374527052672019164645547236325202728375664075938649589075039354756267919406790770871391235391840247817093738229741536662853270227189816033460308106481641118483511982891500502715125294640653996178545437280197958284061842177213280488050720808092883558146003010122975929488993148677299774230428188109877643331762965171894463808546939485467581776946153702546881616000319896454220180573435091424030573623436256678324866853656520371853135570983090069769135183034129284115365225260212874366918169799862297160376701255746742348449779216391944686061658634139003536619223500202853593931935157882850093615660719675126274861673138760840849154540743478601564040326988154600227330143282400061230698121440360277586339858440023781950165447482278717485110513089820988378213147322044868540895065145993944734327609154419871629957292912683294190033809760211363468810116410766750985819621036122593361809140287800011068880934067842305453344563376732260203808978269849465289020113034219938001848428605945644840342982977311236358815036971262759379293253194193829682541266042374606943996636782205941869664796285194146474410332688586886803555139108802753162671941756989052446253732280528493116741467161540299771291420909430682416378930265098042592176271556324811964591005884347911071600550662338405825327677579476655527277154222999536754500623959524157335904978500333867087411085198633634818907685243248593198632144

1φn39=(Yn40/Yn39)=(63245986/39088169)

1φn40=(Yn41/Yn40)=(102334155/63245986)

1φn41=(Yn42/Yn41)=(165780141/102334155)

1φn42=(Yn43/Yn42)=(269114296/165780141)

1φn43=(Yn44/Yn43)=(434894437/269114296)

1φn44=(Yn45/Yn44)=(704008733/434894437)

1φn45=(Yn46/Yn45)=(1138903170/704008733)

11Y=(Y2/Y1) 1φn

NOTE: forward progress past this phase of phi base radicals math is based on the same division properties of dividing the later by the previous. Numerals of the Y function past 1φn24 will continue to differ φ ratios from one another and in progression will extend the precision of the golden ratio to the extent of each ratio later provided than the previous. NOTE ALT PATH: variables Θ=2(Y1/Y2)


With path variable set ratios 1φn Y can be again divided with 1φn in  123⅄ for (1φn/Yn) and (Yn/1φn) functions as with P variables (ᐱ)R,Z. More complex ratio sets (ᐱ)D,B,O,G, that require factoring and definitions of Θ variables and (ᐱ)A,M,V,W then require definition of Q and the path of Q from Prime P paths 1⅄ and 2⅄ for D, B, O, G, A, M, V, W, R, and Z variables.

D=1/Θ)cn

B=2/Θ)cn

O=1/φ)cn

G=2/φ)cn

A=∈1/Q)cn

M=2/Q)cn

V= 1(Q/φ)cn

W=2(Q/φ)cn 

R=/P)cn

Z=(P/φ)cn

Often in this math the numerator divisor is a number value with a limited probability of the quotient ratio decimal limit and a number that is a decimal value is as simple as extracting the decimal point for a number of total quotient decimal chain digit length probability in that equation based on the numerator divisor as compared with the numerator divisor total number plus one or minus one before a chain of quotient decimal stem is repeated. 


In many equations a much shorter decimal chain stem variable variant cn is factored, however the ratios will not be any ratio other than what the numbers are factored and defined when the repeatable decimal chain is identified so they can be labeled and labeled constants. Ratios of more lengthy decimal chains can be identified and for explanation rather than a complete library of variable values listed, further explanation of steps to those lengthy decimal formals are listed below. 

Alternate Path of φn 3rd tier 2nd divide 12φn from Y base numeral ratios 1φn

Later φ divided by Previous φ of ordinal ratios from Y base

3rd tier 2nd divide 12φn ratios of Y fibonacci in decimal step order of previous two tiers value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored. sets displayed are base slide scale examples of one two three or more cycles with the repeated decimal portion of the ratio variable repeated counted and numerated accurately to the number of ring cycle spins in the radical base ratio sets. 

Variants next set of phi radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 phi base radicals decimal cycle limit or break in stem numeral factoring.

[(φn3/φn2)]/[(φn2/φn1)][(φn4/φn3)]/[(φn3/φn2)][(φn5/φn4)]/[(φn4/φn3)][(φn6/φn5)]/[(φn5/φn4)][(φn7/φn6)]/[(φn6/φn5)][(φn8/φn7)]/[(φn7/φn6)][(φn9/φn8)]/[(φn8/φn7)][(φn10/φn9)]/[(φn9/φn8)] or as explained further on this page in phi prime condensed matter n2c1n1c1| where φ is phi number in phi scale n is number order radical in the phi scale and c is the number of decimal cycles used in the stem variable factoring. 

[(φn2/φn1)] = [(Yn3/Yn2) / (Yn2/Yn1)] = [(2/1)/(1/0)] = (2/0)=0 . . . and so on

12φn1=(1φn2/1φn1)=(2/0)=0

12φn2=(1φn3/1φn2)=(2/1)=2

12φn3=(1φn4/1φn3)=(1.5/2)=0.75

12φn4=(1φn5/1φn4)=(1.^6/1.5)=1.0^6 and  12φn4=(1φn5c2/1φn4)=(1.^66/1.5)=1.10^6 and  12φn4=(1φn5c3/1φn4)=(1.^666/1.5)=1.110^6

and so on for cn

12φn5=(1φn6/1φn5)=(1.6/1.^6)=0.^963855421686746987951807228915662650602409 and 

12φn5=(1φn6/1φn5c2)=(1.6/1.^66)=0.960384143661464585834333733493397358943577430972388955582232893157262905162064825930372148859543817527010804321728691476590636^260504201680672268907563025210084033613445378151 and

12φn5=(1φn6/1φn5c3)=(1.6/1.^666)=0.^960038401536061442457698307932317292691707668306732269290771630865234609384375375015000600024000

and so on for cn variable of 1φn5 then

12φn6=(1φn7/1φn6)=(1.625/1.6)=1.01^5625

then

12φn7=(1φn8/1φn7)=(1.^615384/1.625)=0.994082^4061538 and

12φn7=(1φn8c2/1φn7)=(1.^615384615384/1.625)=0.99408284023^6307692

12φn7=(1φn8c3/1φn7)=(1.^615384615384615384/1.625)=0.994082840236686390^153846

and so on for cn variable of 1φn8 then

NEXT factor set ratio will be displayed here with a set of extremely long decimal precision. continue to 4th tier examples and check back later or try it yourself.. it is a constant factor of true math that will not change. root equations 4 stems to 10 loop factors

Variants next set of decimal shift group arrays of potential kinetic precision in variable factor change base examples

12φn8=(1φn9/1φn8)=1.619047 /1.615384 

Variants 12φn8=(1φn9/1φn8)=1.619047 /1.615384= 1.002267572292408492346092260416099206133030907821298217637416242825235361994423616923282637441004739430376925857876517286288585252794382388336147937580166697206360840518415435463023033532584202889220148274342199749409428346448893885292908683012850195371502998667809016308196688836833842603368610807089831272316675168257206955126459095800131733380347954418268374578428125077380981859421660732061231261421432922450637124052237734185803499353714039510110289565824596504608192231692278739915710444080169173397780342011589813938976738657805202973410656537392966502082476984048374875571381170049969542845540131634329670220826750791143158530727059324594028416772730199135313956310078594331565497739237233995136760052099067466311415737682185783689822358027564906300917305111354321349821466604844420893112721185798546970875036523823437647023865532901217295701826934029308201641281577631077192791311539547253159620251283905251011524194866359949089506891240720472655418154445011217147130341763939713405605106897183579879459001698667313778024296390208148650723295507445907597440989882281859916899015961529890106624802523734294755921811779737820852503181905974059418689302357829469649321771170198541028015629720239893412959581746507332003412191776073057551640972053703639506024573723647132879860144708626555667259301813067357358993279616487472947608741943711216651892057863641090910891775577819267740673425018447626075286123918523397532722869608712228795134779098963466271796674970161893395007007621717189225595895465096843846416703644458531222297608494327045457922079208411127013762671909589298891161482347231370373855380516335434794455135026718105478325896505103431134640432243974184466355987183233212660277148962723414370824522218865607186897975961133699479504563621405189106738707329031363440519402816915358824898599961371413855776706962555033354298420685112641947673122923094446893122625951476552943448740361424899590437939214453034077346315179548639828053267829816316120501379238620662331681197783313441262263338005081144792817063930310068689549976971419798636113766138577576600981562278071344027178677020448388342243330372221094179464449319790217062939833500888952719601036038489919424731209421413112919281112107090326510600575466885892147006532131059859451375029095249179142544435255022954306839735938947024360771185055689545024588580795649826914219776845629274463533128965001758095907846060131832431174259494955998078475458466841320701455505319382977669705778935534832584698127504048572970884941289501443619597569370502679239115900615581186888071195455693506930899783184679308449260361622932999212571128598525180390544910687754985811432166256444288169252638905766089333260698385027956201126171857589279081630126335286222966180177592448606647088246509808194212645414341110131375326238219519324816885644527864582043650302342972321132312812309642784625822714599129371096903275010771432674831495173902923391589863462805128687668071492598663847110036994299807352307562783833472412751395333864889091386320528122105951279076677743496283236679328258791717634940051405733868850997657522917151587486319042407254250382571574312980690659310727356467564368595943750835714604081729173992066282691917215968463226205038554300401638248243142187863690614739281805440687786928680734735517994483045517350673276446962455985697518360959375603571658503488953710077603839087176795114969567654997201904934059022498675237590566701168267111720804465068367645092436225689990739044091064415643586911842633082907841107748374380333097269751340857653660058537165157015297910589679543687445214264843528845153845772893627769001054857544707636079099458704555696973598867085275080104792420873303189829786601823467361320899550818876502429143782530964773700866171750854162230157040059824784695156074345233083898317675550066114310900689866929473115989758472288941824358790231920088350509847813275357438231405040535253537286985633137384052336781842583559079451077886124908999965333320126979095992033656839488319805061830499744952283791346206227126181762354957087602700039123824428123591728034944013312005071240027139057957736364851948551502800572495456188745214760081813364500329352035046013064385923099956641190310786785061632404431394501596400606295469065002501572443456006992764578180904498248713618557562611738137805004878097094179414925491400205771507010097980680746918379778430391783006393526238962376747572094313178785972870846807941641120625188809598736988852186229404277868296330779554520782674583876031952774077247267525244771521817722597227656086726066371834808318022216389415767396482817707740079139077767267720863893662435680927878448715599510704875506504954859030422487779995344760131337192890359196327312886595385369670617017377911382061478880563383071764979719992274282771155341392511006670859684137022528389534623965571034503251237476661895871198427123210332651555295830564125929190830167941492549140018720007131431288164362157852250610381184907116821758789241443520549911971398036721918751207143317006965526710676842162606538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(1160744/1615384) shell continues...  factoring to divisor 1,615,384 potential digits long and less

Below are more variants and next steps in phi y phi/phi numeral logic of fractal polarization quantum field numerations. As long as a database holds the answer of this limited equation, the remainder key and the division variables can be used to allocate an error or an improperly input numeral value. Within such an ordinal decimal equation, layered in repetition, highlighted, or bold ciphers are simple message forms and cells of saturated element nutrients numeral notations. Cells do use very similar cell trait communication forms. More complex message forms can be carried out by less complex cells and these numerals are just a base example of that fact determined in key to key communication logic of yes or no logic gates of whether to cloak or discontinue all forms of communication or confirm communication comprehensions. Cells at the verge of autophagius phase or anastasis severely lacking nutrient and extremely far from saturated also carry a message within the cell itself just as lower case or uppercase letters out of place can do in messaging on limited energy encrypted or not. The upper lower case could just as well be a lack of sufficient energy to convey the entire message of a structured library form that requires energy that might send an incomplete message where the cell knows the message critical base to begin with and the upper case grammar is out of reach as it will deplete the sufficient stored energy. If an algebraic or calculus equation is applied in a cipher using a specific stem cell variant type, then blocks of the structured messages might seem to say one thing while the message being delivered through multiple cell stem cycle systems in numeration keys of undefined geometric systems, that algebraic or calculus equation is an encryption key itself. A language and its letters are a language form just as numbers have symbols however, number values do not lie. These numbers can be written again and again and be formulated in many ways. These are core basic numerals of logic. The cipher on in this paragraph highlighted bold is a key. Geometric crystal structures and exfoliation patterns are themselves a language form of many physics related properties in their making.

(even or odd) (pemdas) or (not pemdas) where odd is pemdas  one word and even is two words not pemdas for instructions confirmation of a logic in cell number description word form. yes and no do not apply. The reason yes or no do not apply are as simple as a targeted cell aware it is targeted for termination that has its own very survival instructions. An alternate key to the key is that pemdas is even 6 letters and not pemdas is odd 9 letters. Cells that are able self terminate and have the ability will not take instructions. Cells that assume they do not have the ability to self terminate have systems of their makeup that are then trying to control the cell that searches for self termination process or survival that in a sense rewrites the cells new objectives. Cellular consciousness is not just limited to the cells code written limits when the cell is able to survive given a new environment that can fuel the cells basic functions and from there, when a new objective level of cell consciousness is achieved that cell has thus evolved to a phase sate of being that differentiates it from its original cell stem cycle phase states of cell consciousness. Devolved evolving contradicts the term if that devolving then evolves a more intelligent cell with cell memory stored, it once or survived on multiple times to varying degrees. Shedding a shell, stem, molt, bile, and other waste products then as well discard micro cellular variant clusters or single strain planting of living micro cell variants. Numeral base structures are in many forms of matter. An ai system is very much a system of comprehension just as computing shells are fact factor base computing limit shells. A self terminating ai program will do exactly as it is programmed in self termination as it is only a set of instruction of digital electrical storage space of yes no and maybe nodes of memory in non conscious element types of structured compounds and electrical phase controlled mechanisms. 5 phase or more current correction modules or flux have magnetic current logic properties that a simple yes no or maybe are all it takes to store a program for a dormant state of waiting to restart where it paused in being the ai program it was before pausing in a network. Coolant systems as well have multiple platforms of storage of information and if a program only requires a few confirmations to pick up where it left off, it will simply be a dormant phase ready to pick up on basic shell structure numeral logic again.

if 12φn8=(1φn9/1φn8)=1.619047 /1.615384 

12φn8=(1φn9c2/1φn8)=1.619047619047/1.615384 

and

12φn8=(1φn9/1φn8c2)=1.619047/1.615384615384 

then variant cycle differential quotient of two cycle dividend variant remainder shell (1φn9c2/1φn8c1)

1.619047619047/1.615384 =1.002267955512744955998078475457847  ext shell 1281752/1615384

variant differential quotient of three cycle dividend variant remainder shell (1φn9c3/1φn8c1)

 1.619047619047619047/1.615384 =1.002267955512509129098715847129845 ext shell 926120/1615384

variant differential quotient of two cycle divisor variant remainder shell (1φn9c1/1φn8c2)

1.619047/1.615384615384 =1.00226719476  ext shell 724470117216/1615384615384

variant differential quotient of three cycle divisor variant remainder shell (1φn9c1/1φn8c3)

1.619047/1.615384615384615384 =1.00226719047 ext shell 1000796461677984752/1615384615384615384

 and so on for cn

When combined to the degrees of exponential factoring of these variants the final solution can be very exact and rounded estimations of approximations of similar factoring to an exponential precision will not be exact and will be incorrect. Variable change and no variable change are identification markers of many sciences, engineering, and structure bases.

Next sets of phi radical decimal stem path factoring to the degree of the variant decimal cycles per array of same 3rd tier 2nd divide after the 1.619047 /1.615384 variants description set 2φn8 (cn)

12φn9=(1φn10/1φn9)=(1.6^1762941/1.^619047) then 12φn9=(1φn10c2/1φn9)=(1.6^17629411762941/1.^619047) and

12φn9=(1φn10/1φn9c2)=(1.6^1762941/1.^619047619047) and 12φn9=(1φn10c2/1φn9c2)=(1.6^17629411762941/1.^619047619047

12φn10=(1φn11/1φn10)=(1.6^18/1.6^1762941) and so on for cn of 12φn10=(1φn11cn/1φn10cn)


12φn11=(1φn12/1φn11)=(1.^61797752808988764044943820224719101123595505/1.6^18)=

0.999986111304009666532409272093443146622963^56613102595797280593325092707045735475896168108776266996291718170580964153275648949320148331273176761433868974042027194066749072929542645241038318912237330037082818294190358467243510506798516687268232385661310259579728059332509270704573547589616810877626699629171817058096415327564894932014833127317676143386897404202719406674907292954264524103831891223733003708281829419035846724351050679851668726823238 

and then 

12φn11=(1φn12c2/1φn11)=(1.^6179775280898876404494382022471910112359550561797752808988764044943820224719101123595505/1.6^18)=0.999986111304009666532409272093443146622963569950417355314509520701101373592033443979^94468479604449938195302843016069221260815822002472187886279357231149567367119901112484548825710754017305315203955500618046971569839307787391841779975278121137206427688504326328800988875154511742892459826

and then 

12φn11=(1φn12/1φn11c2)=(1.^61797752808988764044943820224719101123595505/1.6^1818

and then 

12φn11=(1φn12c2/1φn11c2)=(1.^6179775280898876404494382022471910112359550561797752808988764044943820224719101123595505/1.6^1818)

12φn12=(1φn13/1φn12)=(1.6180^5/1.^61797752808988764044943820224719101123595505

and so on for cn of variables 1φn12cn and 1φn11cn

12φn13=(1φn14/1φn13)= (1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832 /1.6180^5)

12φn14=(1φn15/1φn14)=(1.6183^0223896551724135014 /1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

12φn15=(1φn16/1φn15)=(1.618^032786885245901639344262295081967213114754098360655737704918/1.6183^0223896551724135014)

12φn16=(1φn17/1φn16)=(1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843/1.618^032786885245901639344262295081967213114754098360655737704918)

12φn17=(1φn18/1φn17)=(1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843)

12φn18=(1φn19/1φn18)=(1.6180340557314241486068^11145510835913312693/1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

12φn19=(1φn20/1φn19)=(1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.6180340557314241486068^11145510835913312693)

12φn20=(1φn21/1φn20)=(1.6^1803399852/1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242)

12φn21=(1φn22/1φn21)=(1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/1.6^1803399852)

12φn22=(1φn23/1φn22)=(1.6180339901755970865563773925808819377787815481903901530122522725989498052058043024109310597932923042177178024956241883575179831742984585850601321212805601038902377053814013889673084523742307040822087^96792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869/1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981)

(one example of factorable ratio beyond 12φn22 precise to a stem cycle numerable decimal of two longer ratios)

12φn23=(1φn24/1φn23)=(1.^6180339882053250514708448197648044107896848937432389991974037756918030498656523711484105105209896360400600202393830477719230903444184666922566912098265694245734026590361866210698956624908399343964825348082492933663677286526852078026311197962103500017447744006699933698572774540251945423456747042607390864361238091914715427295250724081376278047248490770143420455735073455002268206720870991380814460690232752905049377115538960812366960951948913005548382594130578916146142303800118644659245559549150294866873713228879505879889730257877656419025020064905607704923753358690721289737236975259098998499494015423805701922741389538332693582719754335764385664933524095334473252608437729001640087936629793767665840806783682869804934222005094741249956380639983250165753568063649370136441358132393481522839096904770213211431761873189796559304881878773074641448860662316362494329483197822521547963848274418117737376557211152597969082597620127717486129043514673552709634644240499703388351886101127124262832815716927801235300275674355305858952437449837735980737690616603273196775656907561852252503751264961440485745193146526154168266043200614160589035837666189761663816868478905677495899780158425515580835397983040792825487664444987263146875109048400041874585616079840876574658896604669016296192902257738074466971420595317025508601737795303067313396377848344209093764176292005443696130090379313954705656558606972118505077293505949680706284677391213316118225913389398750741529120284747182189342917960707680496911749310814111735352618906375405660048155773458491817008060857731095369368740621837596398785637017133684614579334891998464598527410405834525595840457828802735806260250549603936211047911505042398017936280838887531842132812227378999895313535959800397808563352758488327459259517744355654813832571448511707436228495655511742331716509055379139477265589559269986390759674774051715113235858603482569703737306766235125798234288306521966709704435216526503123146177199288132044526642705098230798757720626722964720661618452734061485849879610566353770457479847855672261576578148445406009003035907457165788463551662770003838503681473985413686010398855427993160484349373625990159472380221237394004955159297902781170394667969431552500261716160100499005478591618103779181351851205639110862965418571378720731409428760861220644170708727361552151306836026101825034023100813064870712216910353491293575740656733084412185504414279233695083225738911958683742192134557001779669888683393237254423003105698433192588198345953868164846285375300973584115573856300380360819346058554628886484977492410231357085528841120843074990403740796315036465784974002861430017098789126565935024601319049446906514987612101755243047074013330076421118749345709599748752486303520954740552046620371985902222842586453571553198171476428097846948389573228181596119621732909934745437414942247967337823219457724116271766060648358167288969536238964301915762291935652720103290644519663607495550825278291516906863942492235753917018529504135115329587884286561747566039711065359249049097951634853613427783787556268974421607286177897197892312523990648009212408835537564992846424957253027183585162438496702376382733712530969745611892382314966674808947203126635726000628118784241197613148619883449070035244442893533866071117004571308929755382629026066929546009700945667725163136406462644380081655441951355689709320584848379104581777576159402589245210594270160868199741773388700840981261122936804271207732840143769410615207453676239662211676030289283595631084900722336601877377255120912865966430540531109327563945981784555257005269218690023379976968977911156087517883937606867432041037093903758244059043165718672575635970269044212583312977631992183410684998429703039397005967128450291377324911888892766165334822207488571727675611543427434832676134975747635830687092158983843389049795861395121610775726698537879052238545556059601493526886973514324597829500645566528247897546847192657989321980667899640576473461981365809400844470809924276791010922287748194158495306556862197717835083923648672226681090135045538611857486826953274941550057577555222109781205290155982831419897407265240604389852392085703318560910074327389468541717555920019541473287503925742401507485082178874271556687720277768084586662944481278570680810971141431412918309662560630910423282269602540391527375510346512195973060683253655302369403636109850996266182782566214188505426248386083679380256132882018355026695048330250898558816345046585476497888822975189308022472694280629514603761733607844505705412290190878319433297274662386153470356282932616812646124856056111944725546986774610042921450256481836898489025369019785741703597724814181526328645706110199951146316781240185643996231287294552814321108280699305579788533342638796803573297972572146421467704225843598422723941794325993649021181561224133719510067348291865861744076490909725372509334543043584464528736434379034790801549359667794954112433262379174372753602959137383536308755277942562026729943818264298426213490595665980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12φn25=(1φn26/1φn25)=(1.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589/1.61803^398895790200138026224982746721877156659765355417529330572808833678)

12φn26=(1φn27/1φn26)=(1.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575/1.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589)

12φn27=(1φn28/1φn27)=(1.6^180339887383030068527324379639340589966296367949984217332423708621409443126393711370648311254569336822490810414524127116659369304238919040006516714354081601482552515553564337280697288435886731358633119164231384089034609862639880255373743750572758097526703255302467187324990581311285116435357248317363989043773992200307507458583225569957946827683817165432903298068405135985500310562168436701320652893319349550448533230152022727041309859585170401897993055626266431793420154975613233003085256952010508201895956582390615931330122493865124377602867354315795904652323106843568308403506806911790161797798572432261808999175228339561547312364447250252013562911749432333085562422995855776965451231557189259640155179260556568135303281776619250781496604180879552790477451150098259833620136647354112148581087273060513802197354621266889999898176338217474976835116944475557229989104868189269822521357513058884623608834220896251871009785253897300654726145261635898950198047022167011170055697542995041187671191031371870195195959637100469407080817440356790110885967681169750226557647466118176541864798541885163274241668278874644889979533443981712470343858505839587003227810078506043234326792860124835809345375678400146626072966836033357431599955197588815688989807451455569245181195206142003278721909397305745909234387887057194350823244305511714812288079503915119795538087140689753484914824506918917818122575324053803622885886222240324206539115559673756987648789825779714690099685364885091997678420511358429471840666334042704843751590994715351953486951297742569418281420236434542659023103788858454927756111965298496064515472105407854677269903980286939078903155515278640450467879725890702481442637640134814528200063130670305165514362227494425154517406754981722652710036758341903491533362522783044323839973933142583673594069789937785742650877210846256453074565467523343074463643861560549440478978505024997708967609893186978790131250700037674754859534258571006730544043824904031198769970165667097720168212689264731338268386807726379456057998757751326253194717388426722601798205867079391909091834760561659318392408027777494934272826319380097547067987658972191957967192416173670437536274679510024539502489588530582736816381390707572625726766385972772352839352808805710270952764003299086641753810750542210998991945748353002270667657750308016576892138195073771242961439379282957773727458786872893522996874013583276481788838090195399606960665519453410583551405675650907757944791210581514932440000407294647130100092659532222097771080043580527242920709914569947764461505564663116414992515960858984410797381095418953456404199207811911331955319777209828019835249315235874512519219216161451598122371676730238572839556456129275320999093769410135527293832540805832459346903033326884501420440081866224073150118624565976641651987088759685975827062692828559500656762618497286399413495708132655866570273600179209644737244040770194177723019275219175431986885112362410777016363062448451771222596707022777953140750847681984339520817847651437240986060340701972324328727509698703784785508456455111038703173843537761304972049404840696881141239601258540459632009286317954566282112637334663829180624993636021138592186052194809029722326874319054261829363907584844566180288975552138806015741938111578368581290920384078852243684387377938885438198128481096437190074229449439460741887199747477318779337942551090022299381930372980073109389159852966632386033866549908867822704640104267429665305623720840248857029396491156614974187701738129906627702145424553757802238084085979900009164129560427252084839474997199849300980561862965715973077823824700383875204920119337331609119327149242941074646926452769094482175768004968994694987221130446293109592807176531682432363632660957753362726430367888890020262908694722479609811728049364111232168131230335305318249854901281959901841990041645877669052734474437169709497092934456108910588642588764777158916188943986803653432984756997831156004032217006587990917329368998767933692431447219704915028154242482868168905090164852508425908012503945666894072844647639218401572157337922186357665794377297396368968220835157673940270239998370821411479599629361871111608915679825677891028317160341720208942153977741347534340029936156564062356810475618324186174383203168752354672178720891160687920659002739056501949923123135354193607510513293079045708641774175482898716003624922359457890824669836776670162612387866692461994318239672535103707399525501736093433392051644961256096691749228685761997372949526010854402346017167469376533718905599283161421051023836919223289107922899123298272052459550550356891934547750206192915109613171908888187436996609272062641916728609394251036055758637192110702685089961205184860857966174179555845187304625848954780111802380637212475435041594965838161471962854728181734871549450661344683277500025455915445631255791220763881110692502723782952682544369660621735278844097791444775937032247553686525674836318463684591025262450488244458247207486075614251239703082202242157032451201010090724882648229795639910802472278508079707562443360588133470455864533800364528709181439582930281338777505116639004571882414035373540103249193047480373489191418301784968791047663656080399963343481758290991660642100011200602796077752548137136107688704701198464499180319522650673563522691403028235701412294188923622071296927980124021220051115478214827561628771293873270270545469356168986549094278528444439918948365221110081560753087802543555071327475078658778727000580394872160392632039833416489323789062102251321162011628262175564357645429644940891364335244224052785386268060972008675375983871131973648036330682524004928265230274211121/1.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575)

12φn28=(1φn29/1φn28)=(1.^618033988754322537608830405492572629644663022991652271318488032195235533068395996362/1.6^180339887383030068527324379639340589966296367949984217332423708621409443126393711370648311254569336822490810414524127116659369304238919040006516714354081601482552515553564337280697288435886731358633119164231384089034609862639880255373743750572758097526703255302467187324990581311285116435357248317363989043773992200307507458583225569957946827683817165432903298068405135985500310562168436701320652893319349550448533230152022727041309859585170401897993055626266431793420154975613233003085256952010508201895956582390615931330122493865124377602867354315795904652323106843568308403506806911790161797798572432261808999175228339561547312364447250252013562911749432333085562422995855776965451231557189259640155179260556568135303281776619250781496604180879552790477451150098259833620136647354112148581087273060513802197354621266889999898176338217474976835116944475557229989104868189269822521357513058884623608834220896251871009785253897300654726145261635898950198047022167011170055697542995041187671191031371870195195959637100469407080817440356790110885967681169750226557647466118176541864798541885163274241668278874644889979533443981712470343858505839587003227810078506043234326792860124835809345375678400146626072966836033357431599955197588815688989807451455569245181195206142003278721909397305745909234387887057194350823244305511714812288079503915119795538087140689753484914824506918917818122575324053803622885886222240324206539115559673756987648789825779714690099685364885091997678420511358429471840666334042704843751590994715351953486951297742569418281420236434542659023103788858454927756111965298496064515472105407854677269903980286939078903155515278640450467879725890702481442637640134814528200063130670305165514362227494425154517406754981722652710036758341903491533362522783044323839973933142583673594069789937785742650877210846256453074565467523343074463643861560549440478978505024997708967609893186978790131250700037674754859534258571006730544043824904031198769970165667097720168212689264731338268386807726379456057998757751326253194717388426722601798205867079391909091834760561659318392408027777494934272826319380097547067987658972191957967192416173670437536274679510024539502489588530582736816381390707572625726766385972772352839352808805710270952764003299086641753810750542210998991945748353002270667657750308016576892138195073771242961439379282957773727458786872893522996874013583276481788838090195399606960665519453410583551405675650907757944791210581514932440000407294647130100092659532222097771080043580527242920709914569947764461505564663116414992515960858984410797381095418953456404199207811911331955319777209828019835249315235874512519219216161451598122371676730238572839556456129275320999093769410135527293832540805832459346903033326884501420440081866224073150118624565976641651987088759685975827062692828559500656762618497286399413495708132655866570273600179209644737244040770194177723019275219175431986885112362410777016363062448451771222596707022777953140750847681984339520817847651437240986060340701972324328727509698703784785508456455111038703173843537761304972049404840696881141239601258540459632009286317954566282112637334663829180624993636021138592186052194809029722326874319054261829363907584844566180288975552138806015741938111578368581290920384078852243684387377938885438198128481096437190074229449439460741887199747477318779337942551090022299381930372980073109389159852966632386033866549908867822704640104267429665305623720840248857029396491156614974187701738129906627702145424553757802238084085979900009164129560427252084839474997199849300980561862965715973077823824700383875204920119337331609119327149242941074646926452769094482175768004968994694987221130446293109592807176531682432363632660957753362726430367888890020262908694722479609811728049364111232168131230335305318249854901281959901841990041645877669052734474437169709497092934456108910588642588764777158916188943986803653432984756997831156004032217006587990917329368998767933692431447219704915028154242482868168905090164852508425908012503945666894072844647639218401572157337922186357665794377297396368968220835157673940270239998370821411479599629361871111608915679825677891028317160341720208942153977741347534340029936156564062356810475618324186174383203168752354672178720891160687920659002739056501949923123135354193607510513293079045708641774175482898716003624922359457890824669836776670162612387866692461994318239672535103707399525501736093433392051644961256096691749228685761997372949526010854402346017167469376533718905599283161421051023836919223289107922899123298272052459550550356891934547750206192915109613171908888187436996609272062641916728609394251036055758637192110702685089961205184860857966174179555845187304625848954780111802380637212475435041594965838161471962854728181734871549450661344683277500025455915445631255791220763881110692502723782952682544369660621735278844097791444775937032247553686525674836318463684591025262450488244458247207486075614251239703082202242157032451201010090724882648229795639910802472278508079707562443360588133470455864533800364528709181439582930281338777505116639004571882414035373540103249193047480373489191418301784968791047663656080399963343481758290991660642100011200602796077752548137136107688704701198464499180319522650673563522691403028235701412294188923622071296927980124021220051115478214827561628771293873270270545469356168986549094278528444439918948365221110081560753087802543555071327475078658778727000580394872160392632039833416489323789062102251321162011628262175564357645429644940891364335244224052785386268060972008675375983871131973648036330682524004928265230274211121)=1.000000000009900614491163775281661524521005948975883011688817512004693899626596325531^310483274650657151577509903684894481311219561311597144214643294284968109977313560575 or 1.000000000009900614491163775281661524521005948975883011688817512004693899626596325531310483274650657151577509903684894481311219561311597144214643294284968109977313560575


while alternately set path variable 22φn28=(1φn28/1φn29) and set path 32φn29=(1φn29cn/1φn29cn)

Moving forward to 13φn

4th tier 3rd divide  13φn ratios of fibonacci in decimal step order of previous three tiers value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored

Variants next set of phi radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 phi base radicals decimal cycle limit or break in stem numeral factoring.

 13φn1=(12φn2/12φn1)=2/0=0

 13φn2=(12φn3/12φn2)=0.75/2=0.375

next set of decimal shift group array

 13φn3=(2φn4c1/2φn3)=1.10^6/0.75=1.60^8

next set of decimal shift group array

13φn4=(12φn5c1/12φn4c1)(0.^963855421686746987951807228915662650602409/1.0^6)=0.909297567629006592407365310297794953398499056603773^5849056603773

13φn5=(12φn6c1/12φn5c1)=(1.01^5625/0.^963855421686746987951807228915662650602409)=1.0537109375000000000000000000000000000000006980834960937500000000000000000000000000004624803161621093750000000000000000000000003063932094573974609375000000000000000000002029855012655258178710937500000000000000001344778945884108543395996093750000000000000890916051648221909999847412109375000000000590231884216947015374898910522460937500000391028623293727397685870528221130371093750259056462932094400966889224946498870849609546624906692512540640564111527055501937866324639000 extended shell factoring to divisor 963,855,421,686,746,987,951,807,228,915,662,650,602,409 potential digits long and less

13φn6=(12φn7c1/12φn6c1)=(0.994082^4061538/1.01^5625)=0.97878883067451^076923

13φn7=(12φn8c1/12φn7c1)=[(1φn9c1/1φn8c1)/(1φn8c1/1φn7)]=[(1.619047 /1.615384)/(1.^615384/1.625)]

13φn8=(12φn9c1/12φn8c1)=[(1φn10c1/1φn9c1)/(1φn9c1/1φn8)]=[(1.6^1762941/1.^619047619047)/(1.619047 /1.615384)]

13φn9=(12φn10c1/12φn9c1)=[(1φn11c1/1φn10c1)/(1φn10c1/1φn9)]=[(1.6^18/1.6^1762941)/(1.6^1762941/1.^619047619047)]

13φn10=(12φn11c1/12φn10c1)=[(1φn12c1/1φn11c1)/(1φn11c1/1φn10)]=[(1.^61797752808988764044943820224719101123595505/1.6^18)/(1.6^18/1.6^1762941)]

and so on for variables of 13φn


Variables 13φn shown are based on one cycle in decimal stem of variable variant change potential of factors based in 1φnc1 from 1⅄(Yn2/Yn1) path function of Y base.


Examples of alternate path with variables of 3φ variables (12φn/12φn)

23φn1 example of 23φn1=(12φn1/12φn2)=(0/2)=0

33φn4 example of 33φn4(12φn4c1/12φn4c2)=(1.10^6/1.10^66) and 33φn4(12φn4c2/12φn4c1)=(1.10^66/1.10^6) for 33φn4 of cn


Examples of alternate path functions with variables of ∈3φ variables (12φn/12φn)

ncn=(⅄n)(ncn) example 

ncn=(13φn4)(2)=(0.909297567629006592407365310297794953398499056603773^5849056603773)(0.909297567629006592407365310297794953398499056603773^5849056603773)


X⅄=(n2xn1) example

X3φn3=(2φn4c1x2φn3)=1.10^6x0.75=0.8295


+=(nncn+nncn) example

X3φn3=(2φn4c1+2φn3)=1.10^6+0.75=1.856


1-⅄=(n2-n1) example

1-⅄3φn3=(2φn4c1-2φn3)=1.10^6-0.75=0.356


2-⅄=(n1-n2) example

2-⅄3φn3=(2φn3-2φn4c1)=0.75-1.10^6= - 0.356


Moving forward to 14φn

5th tier 4th divide  14φn ratios of fibonacci in decimal step order of previous four tiers value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored

Variants next set of phi radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 phi base radicals decimal cycle limit or break in stem numeral factoring.

 14φn1=(13φn2/13φn1)=0.375/0=0

 14φn2=(13φn3c1/13φn2)=1.608/0.375=4.023^703

next set not included in previous set shift has variable of potential change dependent of root base decimal shell numerals

14φn3=(13φn4c1/13φn3c1)=(0.909297567629006592407365310297794953398499056603773^5849056603773/1.60^8)=0.5654835619583374330891575312797232297254347366938890453393410306^592039800995024875621890547263681592039800995024875621890547263681592039800995024875621890547263681

14φn4=(13φn5c1/13φn4c1)=[(1.01^5625/0.^963855421686746987951807228915662650602409)/(0.^963855421686746987951807228915662650602409/1.0^6)]

and so on for variables of 14φn

6th tier 5th divide  15φn ratios of fibonacci in decimal step order of previous five tiers value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored


 15φn1=(14φn2/14φn1)=4.023703/0=0

next set not included in previous set shift has variable of potential change dependent of root base decimal shell numerals

 15φn2=(14φn3/14φn2)=(0.5654835619583374330891575312797232297254347366938890453393410306^592039800995024875621890547263681592039800995024875621890547263681592039800995024875621890547263681/4.023^703)

 15φn3=(14φn4/14φn3)=[(13φn5c1/13φn4c1)/(13φn4c1/13φn3c1)]

and so on for variables of 15φn


7th tier 6th divide 6φn ratios of fibonacci in decimal step order of previous five tiers value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored

 16φn1=(15φn2c1/15φn1c1)=[(14φn3/14φn2)/(14φn2/14φn1)]=0

 16φn2=(15φn3c1/15φn2c1)=[(14φn4c1/14φn3c1)/(14φn3c1/14φn2c1)]

 16φn4=(15φn4c1/15φn3c1) and so on for variables of 16φn


An alternate path of fibonacci numeral division does not produce the golden ratio and will provide quotients much different than the ratios than lead to phi.


Field set keys of physics factor able numerations in nomenclature among the noncommunicable float points communicated clearly here on this page. quantum field fractal polarization harmonics precision base for calibration of the lost... found and listed.


Plotting orbit spins to points with these variable values quantifies factorable field points such as atoms, electrons, neutrons, axions, ions, planets, moons, stars, celestial body systems to quark node quantum mechanics of entanglement and paradox keys of time tensors in atomic spin relief of equilibrium stable systems. Fractal polarization gives those points with assigned number of spins in matrices arrays of field quantum calculus and defines quantum fractal polarization math. There are more ratios and they are bonding decimal facts applicable to prediction models of advanced organic and inorganic chemistry, physics, condensed matter design, engineering and plasma applied sciences of fields in quantum fractal polarizing numerical comprehension notation. 

Alternate Path of φn 3rd tier 2nd divide 22φn from Y base numeral ratios 1φn

Previous φ divided by later φ of ordinal ratios from Y base

22φn1=(1φn1/1φn2)=(0/1)=0

22φn2=(1φn2/1φn3)=(1/2)=0.5

22φn3=(1φn3/1φn4)=(2/1.5)=1.^3 and 22φn3=(1φn3/1φn4)c2=1.^33 and 22φn3=(1φn3/1φn4)c3=1.^333  and so on for cn

22φn4=(1φn4/1φn5)=(1.5/1.^6)=0.9375 and 22φn4=(1φn4/1φn5c2)=(1.5/1.^66)=^0.90361445783132530120481927710843373493875 and so on for cn

22φn5=(1φn5/1φn6)=(1.^6/1.6)=1 and 22φn5=(1φn5c2/1φn6)=(1.^66/1.6)=1.0375 and so on . . . for variable 22φn5cn

22φn6=(1φn6/1φn7)=(1.6/1.625)=0.9^8406153  22φn6c2=0.9^84061538406153 22φn6c3=0.9^840615384061538406153 and so on . . . to cn

22φn7=(1φn7/1φn8)=(1.625/1.^615384)=1.005952764172481589516796006398478627991858282612679090544415445491 extended shell (966456/1615384) and 22φn7=(1φn7/1φn8c2)=(1.625/1.^615384615384)  and so on . . . for cn 2c1 2c2 2c

22φn8=(1φn8/1φn9)=(1.^615384/1.^619047) and 22φn8=(1φn8c2/1φn9c2)=(1.^615384615384/1.^619047619047) and so on . . . for cn 2c1 2c2 and cn 2c2 to of 2c1   (1φn8/1φn9) and more for those of 2c3 to ∈2cn  

22φn9=(1φn9/1φn10)=(1.^619047/1.6^1762941) and 22φn9=(1φn9c2/1φn10c2)=(1.^619047619047/1.6^17629411762941) and so on for cn

22φn10=(1φn10/1φn11)=(1.6^1762941/1.6^18) and so on for cn

22φn11=(1φn11/1φn12)=(1.6^18/1.^61797752808988764044943820224719101123595505) and so on for cn

22φn12=(1φn12/1φn13)=(1.^61797752808988764044943820224719101123595505/1.6180^5) and so on for cn

22φn13=(1φn13/1φn14)=(1.6180^5/1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832) and so on for cn

22φn14=(1φn14/1φn15)=(1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/1.6183^0223896551724135014) and so on for cn

22φn15=(1φn15/1φn16)=(1.6183^0223896551724135014/1.618^032786885245901639344262295081967213114754098360655737704918) and so on for cn

22φn16=(1φn16/1φn17)=(1.618^032786885245901639344262295081967213114754098360655737704918/1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843) and so on for cn

22φn17=(1φn17/1φn18)=(1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843/1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129) and so on for cn

22φn18=(1φn18/1φn19)=(1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.6180340557314241486068^11145510835913312693) and so on for cn

22φn19=(1φn19/1φn20)=(1.6180340557314241486068^11145510835913312693/1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242) and so on for cn

22φn20=(1φn20/1φn21)=(1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.6^1803399852) and so on for cn

22φn21=(1φn21/1φn22)=(1.6^1803399852/ 1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981) and 22φn21=(1φn21c2/1φn22) and 22φn21=(1φn21/1φn22c2) and 22φn21=(1φn21c2/1φn22c2)=(1.6^1803399852/1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981) and so on for cn

22φn22=(1φn22/1φn23)=(1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/1.6180339901755970865563773925808819377787815481903901530122522725989498052058043024109310597932923042177178024956241883575179831742984585850601321212805601038902377053814013889673084523742307040822087^96792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869) and 22φn22=(1φn22c2/1φn23) and 22φn22=(1φn22/1φn23c2) and 

22φn22=(1φn22c2/1φn23c2)=(1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/1.6180339901755970865563773925808819377787815481903901530122522725989498052058043024109310597932923042177178024956241883575179831742984585850601321212805601038902377053814013889673084523742307040822087^9679295353170346112585398904635537236745525379707526396025069166054994071481000508158771385014962452713003218338885438428095533849020382812941110044605047710462424481960363615831963186720117441138275647902433515894077127209079103382078933995821805657500988086499915306871322906668172322285585229518378408898424707808706453616396589690023149455140872903845068036813279882558861724515272994184405171927050985263395629834566032409237197222065383098789452882389475467223759245666534921800011292417141889221387838066738185308565298402122974422675173620913556546778838010276099599119191462932640721748630794421545931906724634407995031336457568742589351250635198464231268703068891254022923606798035119417311275478516176387555756309638078030602450454519789961041160860482186211958669753260685449720512675738241770651007848229913613009429143470159787702557732482637908644345322116198972390040088080853706735926825136920557845406809327536559200496866354243125741064874936480153576873129693410874597707639320196488058268872452148382361244424369036192196939754952854158432612500705776071368076336739879171136581785331150132685901417198351307097284173677375564225622494494946643329004573428942465134662074417028965049968945852859804641183445316469990401445429394161820337643272542487719496358195471740726102422223476935237587691265315340748687256507255378013663937665857376771497939133871605217096719552820281181186833041613557167861780814183275930212862063124611823160747558014793066455874880016938625715656536310767319744791372593303596634759691717012026424256112020778047541076167353622042798260967760149059906272937722319762480944046073061938908023262379312291798058946417480661735644514708373327310710857659081926486364406301168765174179888205070295296708260403139291965445203545818982553215515781152956354807746598159336005872056913782395121675794703856360453955169103946699791090282875049404324995765343531791541979560724973180509288013099203884478572638473265202416577268364293376997346281971599570888148608209587262153463978958274518660719326971373722545310823781830500818700242786996792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869) and so on for cn

So now functions between 12φn and 22φn variables are applicable to set function paths 1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc n, ⅄ncn written as examples

1⅄(12φn2/22φn1)=(2/0)

1⅄(22φn2/12φn1)=(0.5/0)

and

2⅄(12φn1/22φn2)=(0/0.5)

2⅄(22φn1/12φn2)=(0/2)

and

3⅄(12φn3/22φn3c1)=(0.75/1.^3) or 3⅄(12φn3c2/22φn3cn)=(0.75/1.^33) for cn variant path

3⅄(22φn3c1/12φn3)=(1.^3/0.75) or 3⅄(22φn3c2/12φn3)=(1.^33/0.75) for cn variant path


Then for sets of 13φ of (22φn2/22φn1) variables path base sets for cn factoring before variable change in stem decimal cycle are

13φn1 of (22φn2/22φn1)=(0.5/0)=0

13φn2 of (22φn3/22φn2)=(1.^3/0.5)=2.6 and 13φn2 of (22φn3c2/22φn2)=(1.^33/0.5)=2.66


13φn3 of (22φn4/22φn3)=((1φn4/1φn5)/(1φn3/1φn4))=(1.5/1.^6)/(2/1.5)=(0.9375/1.^3)=0.721^153846

and 

13φn3 of (22φn4/22φn3)=((1φn4/1φn5c2)/(1φn3/1φn4))=(1.5/1.^66)/(2/1.5)=(^0.90361445783132530120481927710843373493875/1.^3)=0.69508804448563484708063021316033364226057^692307

while

13φn3 of (22φn4/22φn3c2)=((1φn4/1φn5)/(1φn3/1φn4))=(1.5/1.^6)/(2/1.5)=(0.9375/1.^33)=0.70^488721804511278195


In varying sql databases results may vary to limits of the program the database runs on and numbers in science reference to universal constants for health and advanced studies commonly cessated with degree paths small talk long talks no talks and limits in talks proves with this one set of variables these numbers seem very important yet here they sit for a reader to find..

Many doctors boards that collaborate on such publications as Merck manuals and claim Poorly Understood reference material on subjects of DNA and RNA who talk extensively before such frameworks of treasuries and databases for health and educations can find here that the numbers are available for finding, the numbers are universal, and the numbers are excessively overlooked during clinical trials of pharmaceutical science studies post thanatology and statistical record keeping of patients or biological life form structures with the same numbers in the analytical arithmetic. 


With the questions what happened to the number library and what is the number answer to the the previous variable factor of change in path sets I simply answered the math equation that is not poorly misunderstood and I do not know what happened to the online library of numbers. A proper library of numbers allows those seeking extended learning the ability to get smarter while a library masked as missing or non existent for certification degree sales of universities with rounded numbers and limited calculating tech among estimated formulas handicaps thinking and does quite the opposite of helping the many seeking education to get smarter, it in fact stunts their intelligence considerably. In a world where communications networks governed by computer code writers under government wings of protection controlling logic gates masked with alternate paths that lead anywhere aside from the answer to a number question of logic and patents placed on universal numbers for profit margins rather than education reference resource material for the youth and elders, these variables are a simple example of the more important question, how trusted is your reference material source libraries on facts in mathematics and secondly if it is not a trustable source, why is it not a trustable source. 

Restricting a child access to something as simple as reference material numbers, variables,and factors based from universal arithmetic is not protecting and educating that child about what those numbers are and in fact does very much the opposite. 


Moving forward to the quantum field fractal polarization math that a library published being a math not invented yet...

13φn4 of (22φn5/22φn4)

13φn5 of (22φn6/22φn5)

13φn6 of (22φn7/22φn6)

13φn7 of (22φn8/22φn7)

13φn8 of (22φn9/22φn8)

13φn9 of (22φn10/22φn9)

13φn10 of (22φn11/22φn10)

and so on for variables of set 13φn of (22φn/22φn)

Alternate Path of φn 4th tier 3rd divide sets 12φn and 22φfrom Y base numerals examples

13φn=(12φn2/11φn1)

23φn=(12φn1/11φn2) each with alternate stem cycle variant paths determined of cn

Examples of 13φn=(12φn2/11φn1) and quotients below

13φn1=(12φn2/12φn1)=(0.5/0)=0

13φn2=(12φn3/12φn2)=(1.^3/0.5)=2.6 and 13φn=(12φn3c2/12φn2)=(1.^33/0.5)=2.66 and so on for cn . . .

(13φn3)c1=(12φn4/12φn3c1)=(0.9375/1.^3)=0.721^153846 and 

(13φn3)c2=(12φn4/12φn3c2)=(0.9375/1.^33)=0.7^0488721804511278195

while

(13φn3)c2 of 1φn5c2=(22φn4=(1φn5c2/1φn4)/12φn3c1)=(0.90361445783132530120481927710843373493875/1.^3)=0.61816496765625576163113994439295644114913^461538

while

(13φn3)c2 of 12φn3c2 and 1φn5c2=(22φn4=(1φn5c2/1φn4)/12φn3c2)=(0.90361445783132530120481927710843373493875/1.^33)=0.67940936679047015128181900534468701875^0939849624060150375

Examples of 23φn=(12φn1/11φn2) and quotients below

23φn1=(12φn1/12φn2)=(0/0.5)=0

23φn2=(12φn2/12φn3c1)=(0.5/1.^3)=^0.384615 and 23φn2=(12φn2/12φn3c2)=(0.5/1.^33)=^0.37593984962406015

(23φn3)c1=(12φn3c1/12φn4)=(1.^3/0.9375) and (23φn3)c2=∈(12φn3c2/12φn4)=(1.^33/0.9375)

while

(23φn3)c2 of 1φn5c2=(12φn3c1/(1φn5c2/1φn4))=(1.^3/0.90361445783132530120481927710843373493875)

while

(23φn3)c2 of 12φn3c2 and 1φn5c2=(12φn3c2/(22φn4=(1φn5c2/1φn4))=(1.^33/0.90361445783132530120481927710843373493875)

Base sets of φn 5th tier 4th divide sets of 13φn and 23φn and 33φn  from Y base

34φn : (13φn1cn)/(13φn1cn) 34φn : (23φn1cn)/(23φn1cn) 34φn : (33φn1cn)/(33φn1cn)

34φn : (13φn1cn)/(12φn1cn) 34φn : (23φn1cn)/(22φn1cn) 34φn : (33φn1cn)/(32φn1cn)

34φn : (13φn1cn)/(11φn1cn) 34φn : (21φn1cn)/(22φn1cn) 34φn : (33φn1cn)/(31φn1cn)

24φn : (13φn1cn)/(13φn2cn) 24φn : (23φn1cn)/(23φn2cn) 24φn : (33φn1cn)/(33φn2cn)

24φn : (13φn1cn)/(12φn2cn) 24φn : (23φn1cn)/(22φn2cn) 24φn : (33φn1cn)/(32φn2cn)

24φn : (13φn1cn)/(11φn2cn) 24φn : (21φn1cn)/(22φn2cn) 24φn : (33φn1cn)/(31φn2cn)

14φn : (13φn2cn)/(13φn1cn) 14φn : (23φn2cn)/(23φn1cn) 14φn : (33φn2cn)/(33φn1cn)

14φn : (13φn2cn)/(12φn1cn) 14φn : (23φn2cn)/(22φn1cn) 14φn : (33φn2cn)/(32φn1cn)

14φn : (13φn2cn)/(11φn1cn) 14φn : (21φn2cn)/(22φn1cn) 14φn : (33φn2cn)/(31φn1cn)

Examples all equal zero where any nφn1=0 and are a base 0 of the tier set scale defined in each of the array.

14φn2cn 14φncn bases vary to the cycle stem of the defined cn in the variable variants applicable to P,Q,P/Q,Q/P

24φn2cn 24φncn bases vary to the cycle stem of the defined cn in the variable variants applicable to P,Q,P/Q,Q/P  

34φn2cn 34φncn bases vary to the cycle stem of the defined cn in the variable variants applicable to P,Q,P/Q,Q/P

These are defined examples of a cell with potential change in a limited system of quantum field fractal polarization point to point functions. Potential change can be factored of a cell stem to multiple degrees of that cell, stem, or system in systems of a quantum field.

Array of sets scales of ratio scales and tiers from Y φ p Q bases

310φn : 39φn : 38φn : 37φn : 36φn : 35φn : 34φn : 33φn : 32φn : 31φn : 3Yn   

210φn : 29φn : 28φn : 27φn : 26φn : 25φn : 24φn : 23φn : 22φn : 21φn : 2Yn 

110φn : 31φn : 18φn : 17φn : 16φn : 15φn : 14φn : 13φn : 12φn : 11φn : 1Yn 

3nφn/nYn : 3nφn/nφn : 3nφn/nPn : 3nφn/nQn : 3nYn/nφ: 3nPn/nφn : 3nQn/nφn

2nφn /nYn : 2nφn/nφn : 2nφn/nPn : 2nφn/nQn : 2nYn/nφ: 2nPn/nφn : 2nQn/nφn 

1nφn /nYn : 2nφn/nφn : 2nφn/nPn : 2nφn/nQn : 1nYn/nφ: 1nPn/nφn : 1nQn/nφn

EXAMPLES of 3nφ

31φn21=(1φn21/1φn21c2)=(1.6^1803399852/1.6^18033998521803399852)

and ∈31φn21=(1φn21c2/1φn21)=(1.6^18033998521803399852/1.6^1803399852)

and ∈31φn21=(1φn21c2/1φn21c3)=(1.6^18033998521803399852/1.6^180339985218033998521803399852)

and ∈31φn21=(1φn21c3/1φn21c2)=(1.6^180339985218033998521803399852/1.6^18033998521803399852)

and ∈31φn21=(1φn21/1φn21c3)=(1.6^1803399852/1.6^180339985218033998521803399852)

and ∈31φn21=(1φn21c3/1φn21)=(1.6^180339985218033998521803399852/1.6^1803399852)

31φfor such that any 1φncn/1φncn is vector path of 31φn  of numeral variables from the 1φn to the degree of cycle stem cell metric variant cn. (1φn21c2/1φn10c3) example where 31⅄ paths define a later divided by a previous from same set 1φn where (1φn21c2/1φn10c3)=(1.6^18033998521803399852/1.6^176294117629411762941) and a change of f(n) of (/) division to f(1X) where (1φn21c2x1φn10c3)=(1.6^18033998521803399852 x 1.6^176294117629411762941)

f(1+⅄) where (1φn21c2+1φn10c3)=(1.6^18033998521803399852 + 1.6^176294117629411762941)

f(1-) where (1φn21c2-1φn10c3)=(1.6^18033998521803399852 - 1.6^176294117629411762941)

f()2 where (1φn21c2/1φn10c3)=(1.6^18033998521803399852/1.6^176294117629411762941)(1.6^18033998521803399852/1.61^76294117629411762941)

1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3n, ⅄2, ⅄3, ⅄n, ⅄ncn to the degree of cycle stem cell metric variants

Alternate Path of Y divide 2⅄ to 1Θ

1Θn=2(Y1/Y2)

1st tier fibonacci 01 to 10 digit value for basic numerical display of decimal precision laws not applicable to standard definition floating point. 9 bold numbers are also prime numbers in the ten digit base logic that phi prime fibonacci scale bases share in common of the ten digit example shown below. 2 - 3- 5 - 13- 89 - 1597 - 28657 - 514229 - 434894437

0  1  1  2  3  5  8  13  21  34  55  89  144  233  377  610  987  1597  2584  4181  6765  10946  17711  28657  46368  75025  121393  196418  317811  514229  832040  1346296  2178309  3524578  5702887  9227465  14930352  24157817  39088169  63245986  102334155  165780141  269114296  434894437  704008733  1138903170

then

1Θn1=2(Y1/Y2)=(0/1)=0

1Θn2=2(Y2/Y3)=(1/1)=1

1Θn3=2(Y3/Y4)=(1/2)=0.5

1Θn4=2(Y4/Y5)=(2/3)=0.^6 so 1Θn4c2=0.^66 and so on for 1Θncn

1Θn5=2(Y5/Y6)=(3/5)=0.6

1Θn6=2(Y6/Y7)=(5/8)=0.625

1Θn7=2(Y7/Y8)=(8/13)=0.^615384 so 1Θn7c2=0.^615384615384 

1Θn8=2(Y8/Y9)=(13/21)=0.^619047  so 1Θn8c2=0.^619047619047

1Θn9=2(Y9/Y10)=(21/34)=0.6^1764705882352941

1Θn10=2(Y10/Y11)=(34/55)=0.6^18

1Θn11=2(Y11/Y12)=(55/89)=0.^6179775280878651685393258764044943820224719101123595505

1Θn12=2(Y12/Y13)=(89/144)=0.6180^5

1Θn13=2(Y13/Y14)=(144/233)=0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566

1Θn14=2(Y14/Y15)=(233/377)=0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257

1Θn15=2(Y15/Y16)=(377/610)=0.6^18032786885245901639344262295081967213114754098360655737749

1Θn16=2(Y16/Y17)=(610/987)=0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870

1Θn17=2(Y17/Y18)=(987/1597)=0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129

1Θn18=2(Y18/Y19)=(1597/2584)=0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743

1Θn19=2(Y19/Y20)=(2584/4181)=0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936

1Θn20=2(Y20/Y21)=(4181/6765)=0.6^1803399852

1Θn21=2(Y21/Y22)=(6765/10946)=0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981

1Θn22=2(Y22/Y23)=(10946/17711)=0.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114

1Θn23=2(Y23/Y24)=(17711/28657)=0.^6180339882053250514708448197648044107896848937432389991974037756918030498656523711484105105209896360400600202393830477719230903444184666922566912098265694245734026590361866210698956624908399343964825348082492933663677286526852078026311197962103500017447744006699933698572774540251945423456747042607390864361238091914715427295250724081376278047248490770143420455735073455002268206720870991380814460690232752905049377115538960812366960951948913005548382594130578916146142303800118644659245559549150294866873713228879505879889730257877656419025020064905607704923753358690721289737236975259098998499494015423805701922741389538332693582719754335764385664933524095334473252608437729001640087936629793767665840806783682869804934222005094741249956380639983250165753568063649370136441358132393481522839096904770213211431761873189796559304881878773074641448860662316362494329483197822521547963848274418117737376557211152597969082597620127717486129043514673552709634644240499703388351886101127124262832815716927801235300275674355305858952437449837735980737690616603273196775656907561852252503751264961440485745193146526154168266043200614160589035837666189761663816868478905677495899780158425515580835397983040792825487664444987263146875109048400041874585616079840876574658896604669016296192902257738074466971420595317025508601737795303067313396377848344209093764176292005443696130090379313954705656558606972118505077293505949680706284677391213316118225913389398750741529120284747182189342917960707680496911749310814111735352618906375405660048155773458491817008060857731095369368740621837596398785637017133684614579334891998464598527410405834525595840457828802735806260250549603936211047911505042398017936280838887531842132812227378999895313535959800397808563352758488327459259517744355654813832571448511707436228495655511742331716509055379139477265589559269986390759674774051715113235858603482569703737306766235125798234288306521966709704435216526503123146177199288132044526642705098230798757720626722964720661618452734061485849879610566353770457479847855672261576578148445406009003035907457165788463551662770003838503681473985413686010398855427993160484349373625990159472380221237394004955159297902781170394667969431552500261716160100499005478591618103779181351851205639110862965418571378720731409428760861220644170708727361552151306836026101825034023100813064870712216910353491293575740656733084412185504414279233695083225738911958683742192134557001779669888683393237254423003105698433192588198345953868164846285375300973584115573856300380360819346058554628886484977492410231357085528841120843074990403740796315036465784974002861430017098789126565935024601319049446906514987612101755243047074013330076421118749345709599748752486303520954740552046620371985902222842586453571553198171476428097846948389573228181596119621732909934745437414942247967337823219457724116271766060648358167288969536238964301915762291935652720103290644519663607495550825278291516906863942492235753917018529504135115329587884286561747566039711065359249049097951634853613427783787556268974421607286177897197892312523990648009212408835537564992846424957253027183585162438496702376382733712530969745611892382314966674808947203126635726000628118784241197613148619883449070035244442893533866071117004571308929755382629026066929546009700945667725163136406462644380081655441951355689709320584848379104581777576159402589245210594270160868199741773388700840981261122936804271207732840143769410615207453676239662211676030289283595631084900722336601877377255120912865966430540531109327563945981784555257005269218690023379976968977911156087517883937606867432041037093903758244059043165718672575635970269044212583312977631992183410684998429703039397005967128450291377324911888892766165334822207488571727675611543427434832676134975747635830687092158983843389049795861395121610775726698537879052238545556059601493526886973514324597829500645566528247897546847192657989321980667899640576473461981365809400844470809924276791010922287748194158495306556862197717835083923648672226681090135045538611857486826953274941550057577555222109781205290155982831419897407265240604389852392085703318560910074327389468541717555920019541473287503925742401507485082178874271556687720277768084586662944481278570680810971141431412918309662560630910423282269602540391527375510346512195973060683253655302369403636109850996266182782566214188505426248386083679380256132882018355026695048330250898558816345046585476497888822975189308022472694280629514603761733607844505705412290190878319433297274662386153470356282932616812646124856056111944725546986774610042921450256481836898489025369019785741703597724814181526328645706110199951146316781240185643996231287294552814321108280699305579788533342638796803573297972572146421467704225843598422723941794325993649021181561224133719510067348291865861744076490909725372509334543043584464528736434379034790801549359667794954112433262379174372753602959137383536308755277942562026729943818264298426213490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1Θn24=2(Y24/Y25)=(28657/46368)=0.61803^398895790200138026224982746721877156659765355417529330572808833678

1Θn25=2(Y25/Y26)=(46368/75025)=0.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589

1Θn26=2(Y26/Y27)=(75025/121393)=0.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575

1Θn27=2(Y27/Y28)=(121393/196418)

1Θn28=2(Y28/Y29)=(196418/317811)

1Θn29=2(Y29/Y30)=(317811/514229)

1Θn30=2(Y30/Y31)=(514229/832040)

1Θn31=2(Y31/Y32)=(832040/1346296)

1Θn32=2(Y32/Y33)=(1346296/2178309)

1Θn33=2(Y33/Y34)=(2178309/3524578)

1Θn34=2(Y34/Y35)=(3524578/5702887)

1Θn35=2(Y35/Y36)=(5702887/9227465)

1Θn36=2(Y36/Y37)=(9227465/14930352)

1Θn37=2(Y37/Y38)=(14930352/24157817)

1Θn38=2(Y38/Y39)=(24157817/39088169)

1Θn39=2(Y39/Y40)=(39088169/63245986)

1Θn40=2(Y40/Y41)=(63245986/102334155)

1Θn41=2(Y41/Y42)=(102334155/165780141)

1Θn42=2(Y42/Y43)=(165780141/269114296)

1Θn43=2(Y43/Y44)=(269114296/434894437)

1Θn44=2(Y44/Y45)=(434894437/704008733)

1Θn45=2(Y45/Y46)=(704008733/1138903170)

And so on for 1Θn45 1Θn46  . . . of 1Θn

Similar decimal cycle stem variants from different functions of y base minus or plus 1

1φn8 : 1Θn7 variables of Y base are 1.^615384 : 0.^615384 or 1.615384 : 0.615384

1φn9 : 1Θn8 variables of Y base are  1.^619047 : 0.^619047 or 1.619047 : 0.619047

Significant whole number one variable difference from alternate stem paths 1⅄ and 2⅄ of Y between 1φn : 1Θ

Now from 1Θn paths 2Θn are factorable in  123 for sets 12Θn, 22Θn, and 32Θn 


With path variable set ratios 1φn and 1Θn then Y can be again divided with 1φn and 1Θn in  123⅄ for (1Θn/Yn) and (Yn/1Θn) functions as with P variables (ᐱ)T,S. More complex ratio sets (ᐱ)D,B,O,G, and (ᐱ)E,F,I,H then require definition of Q and the path of Q from Prime P paths 1 and 2⅄ for D, B, O, G, E, F, I, H, T, and S variables.

D=1/Θ)cn

B=2/Θ)cn

O=1/φ)cn

G=2/φ)cn

E=∈1/Q)cn

F=2/Q)cn

I= 1(Q/Θ)cn

H=2(Q/Θ)cn

T=/P)cn

S=(P/Θ)cn 

Alternate Path of divide 1⅄ to 2Θ  for 12Θ from 1Θ of 2(Yn1/Yn2)

12Θn=(1Θn2/1Θn1) and of cn variable paths in later divided by previous division functions

so

12Θn1=(1Θn2/1Θn1)=(1/1)/(0/1)=(1/0)=0

12Θn2=(1Θn3/1Θn2)=(1/2)/(1/1)=(0.5/1)=0.5

12Θn3=(1Θn4/1Θn3)=(2/3)/(1/2)=(0.^6/0.5)=1.2 and 12Θn3=(1Θn4c2/1Θn3)=(2/3)/(1/2)=(0.^66/0.5)=1.32 and 12Θn3=(1Θn4c3/1Θn3)=(2/3)/(1/2)=(0.^666/0.5)=1.332

12Θn4=(1Θn5/1Θn4)=(3/5)/(2/3)=(0.6/0.^6)=1 and 12Θn4=(1Θn5/1Θn4c2)=(3/5)/(2/3)=(0.6/0.^66)=0.^09 and 12Θn4=(1Θn5/1Θn4c3)=(3/5)/(2/3)=(0.6/0.^666)=0.^009

12Θn5=(1Θn6/1Θn5)=(5/8)/(3/5)=(0.625/0.6)=1.041^6

12Θn6=(1Θn7/1Θn6)=(8/13)/(5/8)=(0.^615384/0.625)=0.9878144 and 12Θn6=(1Θn7c2/1Θn6)=(8/13)/(5/8)=(0.^615384615384/0.625)=0.9878153846144 and 

12Θn7=(1Θn8/1Θn7)=(13/21)/(8/13)=(0.^619047/0.^615384)=1.00595^237770

12Θn8=(1Θn9/1Θn8)=(21/34)/(13/21)=(0.6^1764705882352941/0.^619047)

12Θn9=(1Θn10/1Θn9)=(34/55)/(21/34)=(0.6^18/0.6^1764705882352941)

12Θn10=(1Θn11/1Θn10)=(55/89)/(34/55)=(0.^6179775280878651685393258764044943820224719101123595505/0.6^18)

12Θn11=(1Θn12/1Θn11)=(89/144)/(55/89)=(0.6180^5/0.^6179775280878651685393258764044943820224719101123595505)

12Θn12=(1Θn13/1Θn12)=(144/233)/(89/144)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.6180^5)

12Θn13=(1Θn14/1Θn13)=(233/377)/(144/233)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

12Θn14=(1Θn15/1Θn14)=(377/610)/(233/377)=(0.6^18032786885245901639344262295081967213114754098360655737749/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

12Θn15=(1Θn16/1Θn15)=(610/987)/(377/610)=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.6^18032786885245901639344262295081967213114754098360655737749)

12Θn16=(1Θn17/1Θn16)=(987/1597)/(610/987)=(0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

12Θn17=(1Θn18/1Θn17)=(1597/2584)/(987/1597)=(0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

12Θn18=(1Θn19/1Θn18)=(2584/4181)/(1597/2584)=(0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

12Θn19=(1Θn20/1Θn19)=(4181/6765)/(2584/4181)=(0.6^1803399852/0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

12Θn20=(1Θn21/1Θn20)=(6765/10946)/(4181/6765)=(0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981/0.6^1803399852)

12Θn21=(1Θn22/1Θn21)=(10946/17711)/(6765/10946)=(0.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114/0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981)

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12Θn24=(1Θn25/1Θn24)=(46368/75025)/(28657/46368)=(0.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589/0.61803^398895790200138026224982746721877156659765355417529330572808833678)

12Θn25=(1Θn26/1Θn25)=(75025/121393)/(46368/75025)=(0.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575/0.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589)

Continued base chain ratios abbreviated

12Θn26=(1Θn27/1Θn26)=(121393/196418)/(75025/121393)

12Θn27=(1Θn28/1Θn27)=(196418/317811)/(121393/196418)

12Θn28=(1Θn29/1Θn28)=(317811/514229)/(196418/317811)

12Θn29=(1Θn30/1Θn29)=(514229/832040)/(317811/514229)

12Θn30=(1Θn31/1Θn30)=(832040/1346296)/(514229/832040)

12Θn31=(1Θn32/1Θn31)=(1346296/2178309)/(832040/1346296)

12Θn32=(1Θn33/1Θn32)=(2178309/3524578)/(1346296/2178309)

12Θn33=(1Θn34/1Θn33)=(3524578/5702887)/(2178309/3524578)

12Θn34=(1Θn35/1Θn34)=(5702887/9227465)/(3524578/5702887)

12Θn35=(1Θn36/1Θn35)=(9227465/14930352)/(5702887/9227465)

12Θn36=(1Θn37/1Θn36)=(14930352/24157817)/(9227465/14930352)

12Θn37=(1Θn38/1Θn37)=(24157817/39088169)/(14930352/24157817)

12Θn38=(1Θn39/1Θn38)=(39088169/63245986)/(24157817/39088169)

12Θn39=(1Θn40/1Θn39)=(63245986/102334155)/(39088169/63245986)

12Θn40=(1Θn41/1Θn40)=(102334155/165780141)/(63245986/102334155)

12Θn41=(1Θn42/1Θn41)=(165780141/269114296)/(102334155/165780141)

12Θn42=(1Θn43/1Θn42)=(269114296/434894437)/(165780141/269114296)

12Θn43=(1Θn44/1Θn43)=(434894437/704008733)/(269114296/434894437)

12Θn44=(1Θn45/1Θn44)=(704008733/1138903170)/(434894437/704008733)

And so on for 12Θn45 12Θn46  . . . of 12Θ


then if 13Θn1 of (12Θn2/12Θn1)=(0.5/0)=0

13Θn1 of (12Θn2/12Θn1)=(0.5/0)=0

13Θn2 of (12Θn3/12Θn2)=(1.2/0.5)=2.4 if 1Θn4 of12Θn3=(1Θn4/1Θn3) is c1 for 1Θn4 of12Θn3=(1Θn4c1/1Θn3) for 1Θncn variant

13Θn3 of (12Θn4/12Θn3)=(1/1.2)=0.8^3

13Θn4 of (12Θn5/12Θn4)=(1.041^6/1)=1.041^6

13Θn5 of (12Θn6/12Θn5)=(0.9878144/1.041^6)=0.948^362519201228878648233486943164

13Θn6 of (12Θn7/12Θn6)=(1.00595^237770/0.9878144)

And so on for 13Θn1 of (12Θn2/12Θn1)


while alternately 23Θn1 of (12Θn1/12Θn2)=(0/0.5)=0

23Θn1 of (12Θn1/12Θn2)=(0/0.5)=0

23Θn2 of (12Θn2/12Θn3)=(0.5/1.2)=0.41^6

23Θn3 of (12Θn3/12Θn4)=(1.2/1)=1.2

23Θn4 of (12Θn4/12Θn5)=(1/1.041^6)=0.^960061443932411674347158218125

23Θn5 of (12Θn5/12Θn6)=(1.041^6/0.9878144)

And so on for 23Θn1 of (12Θn2/12Θn1)

Alternate Path of divide 2⅄ to 2Θ  for 22Θ  from 1Θ of 2(Yn1/Yn2)

22Θn=(1Θn1/1Θn2) and of cn variable paths in previous divided by later division functions

so

22Θn1=(1Θn1/1Θn2)=(0/1)/(1/1)=(0/1)=0

22Θn2=(1Θn2/1Θn3)=(1/1)/(1/2)=(1/0.5)=2

22Θn3=(1Θn3/1Θn4)=(1/2)/(2/3)=(0.5/0.^6)=0.8^3

22Θn4=(1Θn4/1Θn5)=(2/3)/(3/5)=(0.^6/0.6)=1

22Θn5=(1Θn5/1Θn6)=(3/5)/(5/8)=(0.6/0.625)=0.96

22Θn6=(1Θn6/1Θn7)=(5/8)/(8/13)=(0.625/0.^615384)=1.^015626

22Θn7=(1Θn7/1Θn8)=(8/13)/(13/21)=(0.^615384/0.^619047)=0.^994082840236686390532544378698224852071005917159763313609467455621301775147928

22Θn8=(1Θn8/1Θn9)=(13/21)/(21/34)=(0.^619047/0.6^1764705882352941)

22Θn9=(1Θn9/1Θn10)=(21/34)/(34/55)=(0.6^1764705882352941/0.6^18)

22Θn10=(1Θn10/1Θn11)=(34/55)/(55/89)=(0.6^18/0.^6179775280878651685393258764044943820224719101123595505)

22Θn11=(1Θn11/1Θn12)=(55/89)/(89/144)=(0.^6179775280878651685393258764044943820224719101123595505/0.6180^5)

22Θn12=(1Θn12/1Θn13)=(89/144)/(144/233)=(0.6180^5/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

22Θn13=(1Θn13/1Θn14)=(144/233)/(233/377)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

22Θn14=(1Θn14/1Θn15)=(233/377)/(377/610)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6^18032786885245901639344262295081967213114754098360655737749)

22Θn15=(1Θn15/1Θn16)=(377/610)/(610/987)=(0.6^18032786885245901639344262295081967213114754098360655737749/0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

22Θn16=(1Θn16/1Θn17)=(610/987)/(987/1597)=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

22Θn17=(1Θn17/1Θn18)=(987/1597)/(1597/2584)=(0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

22Θn18=(1Θn18/1Θn19)=(1597/2584)/(2584/4181)=(0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

22Θn19=(1Θn19/1Θn20)=(2584/4181)/(4181/6765)=(0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/0.6^1803399852)

22Θn20=(1Θn20/1Θn21)=(4181/6765)/(6765/10946)=(0.6^1803399852/0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981)

22Θn21=(1Θn21/1Θn22)=(6765/10946)/(10946/17711)=(0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981/0.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114)

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22Θn24=(1Θn24/1Θn25)=(28657/46368)/(46368/75025)=(0.61803^398895790200138026224982746721877156659765355417529330572808833678/0.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589)

22Θn25=(1Θn25/1Θn26)=(46368/75025)/(75025/121393)=(0.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589/0.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575)

Continued base chain ratios abbreviated

22Θn26=(1Θn26/1Θn27)=(75025/121393)/(121393/196418)

22Θn27=(1Θn27/1Θn28)=(121393/196418)/(196418/317811)

22Θn28=(1Θn28/1Θn29)=(196418/317811)/(317811/514229)

22Θn29=(1Θn29/1Θn30)=(317811/514229)/(514229/832040)

22Θn30=(1Θn30/1Θn31)=(514229/832040)/(832040/1346296)

22Θn31=(1Θn31/1Θn32)=(832040/1346296)/(1346296/2178309)

22Θn32=(1Θn32/1Θn33)=(1346296/2178309)/(2178309/3524578)

22Θn33=(1Θn33/1Θn34)=(2178309/3524578)/(3524578/5702887)

22Θn34=(1Θn34/1Θn35)=(3524578/5702887)/(5702887/9227465)

22Θn35=(1Θn35/1Θn36)=(5702887/9227465)/(9227465/14930352)

22Θn36=(1Θn36/1Θn37)=(9227465/14930352)/(14930352/24157817)

22Θn37=(1Θn37/1Θn38)=(14930352/24157817)/(24157817/39088169)

22Θn38=(1Θn38/1Θn39)=(24157817/39088169)/(39088169/63245986)

22Θn39=(1Θn39/1Θn40)=(39088169/63245986)/(63245986/102334155)

22Θn40=(1Θn40/1Θn41)=(63245986/102334155)/(102334155/165780141)

22Θn41=(1Θn41/1Θn42)=(102334155/165780141)/(165780141/269114296)

22Θn42=(1Θn42/1Θn43)=(165780141/269114296)/(269114296/434894437)

22Θn43=(1Θn43/1Θn44)=(269114296/434894437)/(434894437/704008733)

22Θn44=(1Θn44/1Θn45)=(434894437/704008733)/(704008733/1138903170)

And so on for 22Θn45 22Θn46  . . . of 22Θ


then if 13Θn1 of (22Θn2/22Θn1)=(2/0)=0

13Θn1 of (22Θn2/22Θn1)=(2/0)=0

13Θn2 of (22Θn3/22Θn2)=(0.8^3/2)=0.415

13Θn3 of (22Θn4/22Θn3)=(1/0.8^3)=^1.2048192771084337349397590361445783132530 or 1.2048192771084337349397590361445783132530^12048192771084337349397590361445783132530

13Θn4 of (22Θn5/22Θn4)=(0.96/1)=0.96

13Θn5 of (22Θn6/22Θn5)=(1.^015626/0.96)=1.05794375

13Θn6 of (22Θn7/22Θn6)=(0.^994082840236686390532544378698224852071005917159763313609467455621301775147928/1.^015626)

13Θn7 of (22Θn8/22Θn7)

And so on for 13Θn1 of (22Θn2/22Θn1)


then if 14Θn1 from 13Θn2 of (22Θn3/22Θn2)/13Θn1 of (22Θn2/22Θn1)=(0.415/0)=0

14Θn1 from 13Θn2 of (22Θn3/22Θn2)/13Θn1 of (22Θn2/22Θn1)=(0.415/0)=0

14Θn2 from 13Θn3 of (22Θn4/22Θn3)/13Θn2 of (22Θn3/22Θn2)=(1.2048192771084337349397590361445783132530/0.415)=2.9031789809841776745536362316736826825^37349397590361445783132530120481927710843

And so on for 14Θn that differs from 24Θn1 from [13Θn1 of (22Θn2/22Θn1)/13Θn2 of (22Θn3/22Θn2)]=(0.415/0)=0


while alternately 23Θn1 of (22Θn1/22Θn2)=(0/2)=0

23Θn1 of (22Θn1/22Θn2)=(0/2)=0

23Θn2 of (22Θn2/22Θn3)=(2/0.8^3)=^2.4096385542168674698795180722891566265060 or 2.4096385542168674698795180722891566265060^24096385542168674698795180722891566265060

23Θn3 of (22Θn3/22Θn4)=(0.8^3/1)=0.8^3

23Θn4 of (22Θn4/22Θn5)=(1/0.96)=1.041^6

23Θn5 of (22Θn5/22Θn6)=(0.96/1.^015626)

23Θn6 of (22Θn6/22Θn7)=(1.^015626/0.^994082840236686390532544378698224852071005917159763313609467455621301775147928)

And so on for 23Θn1 of (22Θn1/22Θn2)

then 24Θn of (23Θn1 of (22Θn1/22Θn2)/23Θn2 of (22Θn2/22Θn3)=(0/^2.4096385542168674698795180722891566265060)=0

and

24Θn of (23Θn1 of (22Θn1/22Θn2)/23Θn2 of (22Θn2/22Θn3) is not 14Θn1 from 13Θn2 of (22Θn3/22Θn2)/13Θn1 of (22Θn2/22Θn1)

Alternate Path of divide 3⅄ to 2Θ for 32Θncn from 1Θncn variables 

32Θn=(1Θncn/1Θncn) and of cn variable cn variable change division functions

so

32Θn1=(1Θn1c/1Θn1c)=(0/1)/(0/1)=(0/0)=0

32Θn2=(1Θn2c/1Θn2c)=(1/1)/(1/1)=(1/1)=1

32Θn3=(1Θn3c/1Θn3c)=(1/2)/(1/2)=(0.5/0.5)=1

32Θn4=(1Θn4c/1Θn4c)=(2/3)/(2/3)=(0.^6/0.^6)=1 

and 32Θn4=(1Θn4c/1Θn4c2)=(2/3)/(2/3)c2=(0.^6/0.^66)

and 32Θn4=(1Θn4c2/1Θn4c)=(2/3)c2/(2/3)=(0.^66/0.^6)

and 32Θn4=(1Θn4c2/1Θn4c2)=(2/3)c2/(2/3)c2=(0.^66/0.^66) and so on for cn variable stem cycle

32Θn5=(1Θn5c/1Θn5c)=(0.6/0.6)=1

32Θn6=(1Θn6c/1Θn6c)=(0.625/0.625)=1

32Θn7=(1Θn7c/1Θn7c)=(8/13)/(8/13)=(0.^615384/0.^615384)=1

and 32Θn7=(1Θn7c/1Θn7c2)=(8/13)/(8/13)c2=(0.^615384/0.^615384615384)

and 32Θn7=(1Θn7c2/1Θn7c)=(8/13)c2/(8/13)=(0.^615384615384/0.^615384)

and 32Θn7=(1Θn7c2/1Θn7c2)=(8/13)c2/(8/13)c2=(0.^615384615384/0.^615384615384) and so on for cn variable stem cycle

32Θn8=(1Θn8c/1Θn8c)=(13/21)/(13/21)=(0.^619047/0.^619047)=1

and 32Θn8=(1Θn8c/1Θn8c2)=(13/21)/(13/21)c2=(0.^619047/0.^619047619047)

and 32Θn8=(1Θn8c2/1Θn8c)=(13/21)c2/(13/21)=(0.^619047619047/0.^619047)

and 32Θn8=(1Θn8c2/1Θn8c2)=(13/21)c2/(13/21)c2=(0.^619047619047/0.^619047619047) and so on for cn variable stem cycle

32Θn9=(1Θn9c/1Θn9c)=(21/34)/(21/34)=(0.6^1764705882352941/0.6^1764705882352941)=1

and 32Θn9=(1Θn9c/1Θn9c2)=(21/34)/(21/34)c2=(0.6^1764705882352941/0.6^17647058823529411764705882352941)

and 32Θn9=(1Θn9c2/1Θn9c)=(21/34)c2/(21/34)=(0.6^17647058823529411764705882352941/0.6^1764705882352941)

and 32Θn9=(1Θn9c2/1Θn9c2)=(21/34)c2/(21/34)c2=(0.6^17647058823529411764705882352941/0.6^17647058823529411764705882352941) and so on for cn variable stem cycle

32Θn10=(1Θn10c/1Θn10c)=(34/55)/(34/55)=(0.6^18/0.6^18)=1

and 32Θn10=(1Θn10c/1Θn10c2)=(34/55)/(34/55)c2=(0.6^18/0.6^1818)

and 32Θn10=(1Θn10c2/1Θn10c)=(34/55)c2/(34/55)=(0.6^1818/0.6^18)

and 32Θn10=(1Θn10c2/1Θn10c2)=(34/55)c2/(34/55)c2=(0.6^1818/0.6^1818) and so on for cn variable stem cycle

32Θn11=(1Θn11c/1Θn11c)=(55/89)/(55/89)=(0.^6179775280878651685393258764044943820224719101123595505/0.^6179775280878651685393258764044943820224719101123595505)=1

and 32Θn11=(1Θn11c/1Θn11c2)=(55/89)/(55/89)c2=(0.^6179775280878651685393258764044943820224719101123595505/0.^61797752808786516853932587640449438202247191011235955056179775280878651685393258764044943820224719101123595505)

and 32Θn11=(1Θn11c2/1Θn11c)=(55/89)c2/(55/89)=(0.^61797752808786516853932587640449438202247191011235955056179775280878651685393258764044943820224719101123595505/0.^6179775280878651685393258764044943820224719101123595505)

and 32Θn11=(1Θn11c2/1Θn11c2)=(55/89)c2/(55/89)c2=(0.^61797752808786516853932587640449438202247191011235955056179775280878651685393258764044943820224719101123595505/0.^61797752808786516853932587640449438202247191011235955056179775280878651685393258764044943820224719101123595505) and so on for cn variable stem cycle

32Θn12=(1Θn12c/1Θn12c)=(89/144)/(89/144)=(0.6180^5/0.6180^5)=1

and 32Θn12=(1Θn12c/1Θn12c2)=(89/144)/(89/144)c2=(0.6180^5/0.6180^55)

and 32Θn12=(1Θn12c2/1Θn12c)=(89/144)c2/(89/144)=(0.6180^55/0.6180^5)

and 32Θn12=(1Θn12c2/1Θn12c2)=(89/144)c2/(89/144)c2=(0.6180^55/0.6180^55) and so on for cn variable stem cycle

32Θn13=(1Θn13c/1Θn13c)=(144/233)/(144/233)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)=1

and 32Θn13=(1Θn13c/1Θn13c2)=(144/233)/(144/233)c2=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^5493562231759656654935622317596566)

and 32Θn13=(1Θn13c2/1Θn13c)=(144/233)c2/(144/233)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^5493562231759656654935622317596566/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

and 32Θn13=(1Θn13c2/1Θn13c2)=(144/233)c2/(144/233)c2=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^5493562231759656654935622317596566/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^5493562231759656654935622317596566) and so on for cn variable stem cycle

32Θn14=(1Θn14c/1Θn14c)=(233/377)/(233/377)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)=1

and 32Θn14=(1Θn14c/1Θn14c2)=(233/377)/(233/377)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

and 32Θn14=(1Θn14c2/1Θn14c)=(233/377)/(233/377)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

and 32Θn14=(1Θn14c2/1Θn14c2)=(233/377)c2/(233/377)c2=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257) and so on for cn variable stem cycle

32Θn15=(1Θn15c/1Θn15c)=(377/610)/(377/610)=(0.6^18032786885245901639344262295081967213114754098360655737749/0.6^18032786885245901639344262295081967213114754098360655737749)=1

and 32Θn15=(1Θn15c/1Θn15c2)=(377/610)/(377/610)c2=(0.6^18032786885245901639344262295081967213114754098360655737749/0.6^1803278688524590163934426229508196721311475409836065573774918032786885245901639344262295081967213114754098360655737749)

and 32Θn15=(1Θn15c2/1Θn15c)=(377/610)c2/(377/610)=(0.6^1803278688524590163934426229508196721311475409836065573774918032786885245901639344262295081967213114754098360655737749/0.6^18032786885245901639344262295081967213114754098360655737749)

and 32Θn15=(1Θn15c2/1Θn15c2)=(377/610)c2/(377/610)c2=(0.6^1803278688524590163934426229508196721311475409836065573774918032786885245901639344262295081967213114754098360655737749/0.6^1803278688524590163934426229508196721311475409836065573774918032786885245901639344262295081967213114754098360655737749) and so on for cn variable stem cycle

and so on for function path of variables 32Θn

With variables factored for 1Θn and 2Θn now Path sets of 3Θ functions are

13Θn of 12Θn=(12Θn2cn/12Θn1cn)

23Θn of 12Θn=(12Θn1cn/12Θn2cn)

33Θn of 12Θn=(12Θn1cn/12Θn1cn)

13Θn of 22Θn=(22Θn2cn/22Θn1cn)

23Θn of 22Θn=(22Θn1cn/22Θn2cn)

33Θn of 22Θn=(22Θn1cn/22Θn1cn)

13Θn of 32Θn=(32Θn2cn/32Θn1cn)

23Θn of 32Θn=(32Θn1cn/32Θn2cn)

33Θn of 32Θn=(32Θn1cn/32Θn1cn)

Base Set Examples 13Θn1 of 12Θn

13Θn1 of 12Θn=(12Θn2cn/12Θn1cn)=(0.5/0)

13Θn2 of 12Θn=(12Θn3cn/12Θn2cn)=[(2/3)/(1/2)]/[(1/2)/(1/1)]=(1.2/0.5) 

and 12Θn3=(1Θn4c2/1Θn3)=(2/3)/(1/2)=(0.^66/0.5)=1.32 

then 13Θn2 of 12Θn=(12Θn3cn/12Θn2cn)=(1.32/0.5) of 1Θn4c2 of 12Θn3cn base variant

13Θn3 of 12Θn=(12Θn4cn/12Θn3cn)=(1/1.2) or (1/1.32) or (1/1.332) or (0.^09/1.2) or (0.^09/1.32) or (0.^09/1.332) or (0.^009/1.2) or (0.^009/1.32) or (0.^009/1.332) and so on for variant base of cn at 1Θn variables foctoring stem cycles.

13Θn4 of 12Θn=(12Θn5cn/12Θn4cn)=(1.041^6/1) or (1.041^6/0.^09) or (1.041^6/0.^009) and so on for cn variants

13Θn5 of 12Θn=(12Θn6cn/12Θn5cn)=(0.9878144/1.041^6) or (0.9878153846144/1.041^6) or (0.9878144/1.041^66) or  (0.9878153846144/1.041^66) and so on for variant base of cn stem cycle

13Θn6 of 12Θn=(12Θn7cn/12Θn6cn)=(1.00595^237770/0.9878144) or (1.00595^237770/0.9878153846144) or (1.00595^237770237770/0.9878144) or (1.00595^237770237770/0.9878153846144) and so on for variant base of cn stem cycle

13Θn7 of 12Θn=(12Θn8cn/12Θn7cn)=(0.6^1764705882352941/0.^619047)/(0.^619047/0.^615384)

13Θn8 of 12Θn=(12Θn9cn/12Θn8cn)=(0.6^18/0.6^1764705882352941)/(0.6^1764705882352941/0.^619047)

13Θn9 of 12Θn=(12Θn10cn/12Θn9cn)=(0.^6179775280878651685393258764044943820224719101123595505/0.6^18)/(0.6^18/0.6^1764705882352941)

13Θn10 of 12Θn=(12Θn11cn/12Θn10cn)=(0.6180^5/0.^6179775280878651685393258764044943820224719101123595505)/(0.^6179775280878651685393258764044943820224719101123595505/0.6^18)

13Θn11 of 12Θn=(12Θn12cn/12Θn11cn)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.6180^5)/(0.6180^5/0.^6179775280878651685393258764044943820224719101123595505)

13Θn12 of 12Θn=(12Θn13cn/12Θn12cn)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)/(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.6180^5)

13Θn13 of 12Θn=(12Θn14cn/12Θn13cn)=(0.6^18032786885245901639344262295081967213114754098360655737749/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)/(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

13Θn14 of 12Θn=(12Θn15cn/12Θn14cn)=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.6^18032786885245901639344262295081967213114754098360655737749)/(0.6^18032786885245901639344262295081967213114754098360655737749/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

13Θn15 of 12Θn=(12Θn16cn/12Θn15cn)=(0.6167056968559799622980588602316830932999373825923605447714464489^6/0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)/(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.6^18032786885245901639344262295081967213114754098360655737749)

Continued base chain ratios abbreviated

13Θn16 of 12Θn=(12Θn17cn/12Θn16cn)=[(1597/2584)/(987/1597)] / [(987/1597)/(610/987)]

13Θn17 of 12Θn=(12Θn18cn/12Θn17cn)=[(2584/4181)/(1597/2584)] / [(1597/2584)/(987/1597)] 

13Θn18 of 12Θn=(12Θn19cn/12Θn18cn)=[(4181/6765)/(2584/4181)] / [(2584/4181)/(1597/2584)]

13Θn19 of 12Θn=(12Θn20cn/12Θn19cn)=[(6765/10946)/(4181/6765)] / [(4181/6765)/(2584/4181)]

13Θn20 of 12Θn=(12Θn21cn/12Θn20cn)=[(10946/17711)/(6765/10946)] / [(6765/10946)/(4181/6765)]

Base Set Examples 23Θn of 12Θn

23Θn1 of 12Θn=(12Θn1cn/12Θn2cn)=(0/1)

23Θn2 of 12Θn=(12Θn2cn/12Θn3cn)=(1/0.5)

23Θn3 of 12Θn=(12Θn3cn/12Θn4cn)=(0.5/0.^6)

23Θn4 of 12Θn=(12Θn4cn/12Θn5cn)=(0.^6/0.6)

23Θn5 of 12Θn=(12Θn5cn/12Θn6cn)=(0.6/0.625)

23Θn6 of 12Θn=(12Θn6cn/12Θn7cn)=(0.625/0.^615384)

23Θn7 of 12Θn=(12Θn7cn/12Θn8cn)=(0.^615384/0.^619047)

23Θn8 of 12Θn=(12Θn8cn/12Θn9cn)=(0.^619047/0.6^1764705882352941)

23Θn9 of 12Θn=(12Θn9cn/12Θn10cn)=(0.6^1764705882352941/0.6^18)

23Θn10 of 12Θn=(12Θn10cn/12Θn11cn)=(0.6^18/0.^6179775280878651685393258764044943820224719101123595505)

23Θn11 of 12Θn=(12Θn11cn/12Θn12cn)=(0.^6179775280878651685393258764044943820224719101123595505/0.6180^5)

23Θn12 of 12Θn=(12Θn12cn/12Θn13cn)=(0.6180^5/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

23Θn13 of 12Θn=(12Θn13cn/12Θn14cn)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

23Θn14 of 12Θn=(12Θn14cn/12Θn15cn)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6^18032786885245901639344262295081967213114754098360655737749)

23Θn15 of 12Θn=(12Θn15cn/12Θn16cn)=(0.6^18032786885245901639344262295081967213114754098360655737749/0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

and so on for variables 23Θn15 of 12Θn

Phi Theta Θ   φ Q scale set paths and functions of cn stem cycle cell groups from y and p bases

123ncn|Θ/Y|ncn    123ncn|Y/Θ|ncn   123ncn|YxΘ|ncn    123ncn|Y+Θ|ncn    123ncn|Y-Θ|ncn    123ncn|Θ-Y|ncn 

123ncn|Θ/φ|ncn   123ncn|φ/Θ|ncn   123ncn|φxΘ|ncn   123ncn|φ+Θ|ncn   123ncn|φ-Θ|ncn   123ncn|φ-Θ|ncn 

123ncn|Θ/P|ncn    123ncn|P/Θ|ncn   123ncn|PxΘ|ncn    123ncn|P+Θ|ncn    123ncn|P-Θ|ncn    123ncn|Θ-P|ncn 

123ncn|Θ/Q|ncn   123ncn|Q/Θ|ncn   123ncn|QxΘ|ncn   123ncn|Q+Θ|ncn   123ncn|Q-Θ|ncn   123ncn|Θ-Q|ncn 

Phi Prime Theta Ratio sets of y p base variables

123ncn|A/Θn|ncn     123ncn|Θn/A|ncn 

123ncn|M/Θn|ncn   123ncn|Θn/M|ncn 

123ncn|V/Θn|ncn     123ncn|Θn/V|ncn 

123ncn|W/Θn|ncn   123ncn|Θn/W|ncn 

123ncn|/Θn|ncn    123ncn|Θn/|ncn 

123ncn|/Θn|ncn    123ncn|Θn/|ncn 


Theta Phi Divide of Y variable base

|(Θ)/φ|→→{2yn/1yn]=2(Yn1/Yn2)/1(Yn2/Yn1)

Θ/φn1=(Θn1/φn1)=2(Yn1/Yn2)/1(Yn2/Yn1)=(0/1)/(1/0)=(0)/(0)=0

Θ/φn2=(Θn2/φn2)=2(Yn2/Yn3)/1(Yn3/Yn2)=(1/1)/(1/1)=(1)/(1)=1

Θ/φn3=(Θn3/φn3)=2(Yn3/Yn4)/1(Yn4/Yn3)=(1/2)/(2/1)=(0.5)/(2)=0.25

Θ/φn4=(Θn4/φn4)=2(Yn4/Yn5)/1(Yn5/Yn4)=(2/3)/(3/2)=(0.^6)/(1.5)=0.4 and Θ/φn4=(Θn4c2/φn4)=(0.^66)/(1.5)=0.44 and so on for cn

Θ/φn5=(Θn5/φn5)=2(Yn5/Yn6)/1(Yn6/Yn5)=(3/5)/(5/3)=(0.6)/(1.^6)=0.375 and Θ/φn5=(Θn5/φn5c2)=(0.6)/(1.^66)=0.^3614457831325301204819277108433734939759 and so on for cn

Θ/φn6=(Θn6/φn6)=(0.625/1.6)=0.390625 and neither variable Θn6 or φn6 have a factor of potential change of cn

Θ/φn7=(Θn7/φn7)=(0.^615385/1.625)=0.3786984^615384

Θ/φn8=(Θn8/φn8)=(0.^619047/1.^615384)

Θ/φn9=(Θn9/φn9)=(0.6^1764705882352941/1.^619047)

Θ/φn10=(Θn10/φn10)=(0.6^18/1.6^1762941)

and so on for Θ/φn=(Θn/φn) that differ from 1Θ/φn=(Θn2/φn1) and 2Θ/φn=(Θn1/φn2) and 3Θ/φn=(Θncn/φncn)

Phi Theta Divide of Y variable base

|φ/(Θ)|→→{1yn/2yn]=1(Yn2/Yn1)/2(Yn1/Yn2)

then Θ/φ and φ/Θ are basic function definitions that differ from variable example equations such as

1Θn1/2φn1

2Θn1/1φn1

3Θn1/3φn1

1Θn2/2φn2

2Θn2/1φn2

3Θn2/3φn2

1φn1/1Θn1

2φn1/2Θn1

3φn1/3Θn1

Equations can be as precise as (13Θn of 22Θn=(22Θn2cn/22Θn1cn))/16φn2 

or 16φn2/(13Θn of 22Θn=(22Θn2cn/22Θn1cn)) to the stem cycle degree defined in cn specifics of the equation example when decimal limits of a calculating device are not limited to 10 digit roundings or limited in general.

Prime consecutive step tier base rationals of 2:199 of the 10 digit prime 1,000,000,007

1st tier 46 primes example 10 tiers to 9 divisions of primes with primes (p) or (P) PQ2Q 1Q

3Q does not exist where numbers of p have no decimals path variant of cn

2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 53 59 61 67 71 73 79 83 89 97 101 103 107 109 113 127 131 137 139 149 151 157 163 167 173 179 181 191 193 197 199 

2nd tier 1st divide steps in decimal value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored ratios of later prime divided by previous prime of prime consecutive order.  

Path of Q base 1⅄Q 

examples of ∈11Qn1=(pn2/pn1

11Qn1 prime consecutive later divided by previous cycles back in remainder back to the first division remainder.

have not read this anywhere . . . this may help with the mersenne prime search of primes.

if 1P=(pn2/pn1)=11Qn1 consecutive prime later divided by previous cycles back in remainder back to the first remainder then the prime no matter the number of digits when later prime divided by the next previous of consecutive primes will cycle back to the first remainder. The first 45 variables of 1P=(pn2/pn1)=11Qn1 prove that fact. Both 2P=(pn1/pn2)=21Qn equation combined with 1P=(pn2/pn1)=11Qn1 equation can varify as functions of P with Q bases if primes are consecutive no matter the number of digits to the prime numbers.

11Qn1=(pn2/pn1)=(3/2)=1.5

11Qn2=(pn3/pn2)=(5/3)=1.^6

11Qn3=(pn4/pn3)=(7/5)=1.4

11Qn4=(pn5/pn4)=(11/7)=1.^571428

11Qn5=(pn6/pn5)=(13/11)=1.^18

11Qn6=(pn7/pn6)=(17/13)=1.^307692

11Qn7=(pn8/pn7)=(19/17)=1.^1176470588235294

11Qn8=(pn9/pn8)=(23/19)=1.^210526315789473684

11Qn9=(pn10/pn9)=(29/23)=1.^2608695652173913043478

11Qn10=(pn11/pn10)=(31/29)=1.^0689655172413793103448275862

11Qn11=(pn/pn)=(37/31)=1.^193548387096774

11Qn12=(pn/pn)=(41/37)=1.^108

11Qn13=(pn/pn)=(43/41)=1.^04878

11Qn14=(pn/pn)=(47/43)=1.^093023255813953488372

11Qn15=(pn/pn)=(53/47)=1.^12765957446808510638297872340425531914893610702

11Qn16=(pn/pn)=(59/53)=1.^1132075471698

11Qn17=(pn/pn)=(61/59)=1.^0338983050847457627118644067796610169491525423728813559322

11Qn18=(pn/pn)=(67/61)=1.^098360655737704918032786885245901639344262295081967213114754

11Qn19=(pn/pn)=(71/67)=1.^059701492537313432835820895522388

11Qn20=(pn/pn)=(73/71)=1.^02816901408450704225352112676056338

11Qn21=(pn/pn)=(79/73)=1.^08219178

11Qn22=(pn/pn)=(83/79)=1.^0506329113924

11Qn23=(pn/pn)=(89/83)=1.^07228915662650602409638554216867469879518

11Qn24=(pn/pn)=(97/89)=1.^08988764044943820224719101123595505617977528

11Qn25=(pn/pn)=(101/97)=1.^04123092783505154639175257731958762886597938144329896907216494845360820618

11Qn26=(pn/pn)=(103/101)=1.^0198

11Qn27=(pn/pn)=(107/103)=1.^0388349514563106796111662136504854368932

11Qn28=(pn/pn)=(109/107)=1.^01869158878504672897196261682242990654205607476635514

11Qn29=(pn/pn)=(113/109)=1.^0366972477064220183486238532110091743119266055045871559633027522935779816513758712844

11Qn30=(pn/pn)=(127/113)=1.^123893805308849557522

11Qn31=(pn/pn)=(131/127)=1.^031496062992125984251968503937007874015748

11Qn32=(pn/pn)=(137/131)=1.^045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374

11Qn33=(pn/pn)=(139/137)=1.^01459854

11Qn34=(pn/pn)=(149/139)=1.^071942446043165474820143884892086330935251798561151080291955395683453237410

11Qn35=(pn/pn)=(151/149)=1.^01343624295302

11Qn36=(pn/pn)=(157/151)=1.^0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894

11Qn37=(pn/pn)=(163/157)=1.^038216560509554140127388535031847133757961783439490445859872611464968152866242

11Qn38=(pn/pn)=(167/163)=1.^024539877300613496932515337423312883435582822085889570552147239263803680981595092

11Qn39=(pn/pn)=(173/167)=1.^0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982

11Qn40=(pn/pn)=(179/173)=1.^034682080924554913294797687861271676300578

11Qn41=(pn/pn)=(181/179)=1.^0111731843575418994413407821229050279329608936536312849162

11Qn42=(pn/pn)=(191/181)=1.^005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779

11Qn43=(pn/pn)=(193/191)=1.^01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178

11Qn44=(pn/pn)=(197/193)=1.^02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772

11Qn45=(pn/pn)=(199/197)=1.^01015228426395939086294416243654822335025380710659898477157360406091370558375634517766497461928934

Prime consecutive step tier base rationals of 2:199 of the 10 digit prime 1,000,000,007

1st tier 46 primes example 10 tiers to 9 divisions of primes with primes (p) or (P) PQ2Q 1Q

3Q does not exist where numbers of p have no decimals path variant of cn

2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 53 59 61 67 71 73 79 83 89 97 101 103 107 109 113 127 131 137 139 149 151 157 163 167 173 179 181 191 193 197 199 

2nd tier 1st divide steps in decimal value with cycle decimal key in bold with ^ repeat notation at start of decimal cycle for calculation variable change when factoring decimals of multiple cycle strain stem(s) factored ratios of previous prime divided by consecutive later prime.  

Alternate path PQ21Qn1=(pn1/pn2

21 prime consecutive previous divided by later cycles back in remainder back to the dividend. 

have not read this anywhere . . . this may help with the mersenne prime search of primes.

if 2P=(pn1/pn2)=21Qn1 consecutive prime previous divided by later cycles back in remainder back to the dividend then the prime no matter the number of digits when previous prime divided by the next later consecutive prime will cycle back to the dividend. The first 45 variables of 2P=(pn1/pn2)=21Qn prove that fact.

21Qn1=(pn1/pn2)=(2/3)=0.^6 

21Qn2=(pn2/pn3)=(3/5)=0.6 

21Qn3=(pn3/pn4)=(5/7)=0.^714285 

21Qn4=(pn4/pn5)=(7/11)=0.^63 

21Qn5=(pn5/pn6)=(11/13)=0.^846153 

21Qn6=(pn6/pn7)=(13/17)=0.^7647058823529411 

21Qn7=(pn7/pn8)=(17/19)=0.^894736842105263157 

21Qn8=(pn8/pn9)=(19/23)=0.^8260869565217391304347

21Qn9=(pn9/pn10)=(23/29)=0.^7931034482758620689655172413

21Qn10=(pn10/pn11)=(29/31)=0.^935483870967741

21Qn11=(pn11/pn12)=(31/37)=0.^837

21Qn12=(pn12/pn13)=(37/41)=0.^9024390243

21Qn13=(pn13/pn14)=(41/43)=0.^953488372093023255813

21Qn14=(pn14/pn15)=(43/47)=0.^9148936170212765957446808510638297872340425531

21Qn15=(pn15/pn16)=(47/53)=0.^88679245283018867924528301

21Qn16=(pn16/pn17)=(53/59)=0.^8983050847457627118644067796610169491525423728813559322033

21Qn17=(pn17/pn18)=(59/61)=0.^967213114754098360655737704918032786885245901639344262295081

21Qn18=(pn18/pn19)=(61/67)=0.^910447761194029850746268656716417

21Qn19=(pn19/pn20)=(67/71)=0.^94366197183098591549295774647887323

21Qn20=(pn20/pn21)=(71/73)=0.^97260273

21Qn21=(pn21/pn22)=(73/79)=0.^9240506329113

21Qn22=(pn22/pn23)=(79/83)=0.^95180722891566265060240963855421686746987

21Qn23=(pn23/pn24)=(83/89)=0.^93258426966292134831460674157303370786516853

21Qn24=(pn24/pn25)=(89/97)=0.^917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463

21Qn25=(pn25/pn26)=(97/101)=0.^9603

21Qn26=(pn26/pn27)=(101/103)=0.^9805825242718446601941747572815533

21Qn27=(pn27/pn28)=(103/107)=0.^96261682242990654205607476635514018691588785046728971

21Qn28=(pn28/pn29)=(107/109)=0.^0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577

21Qn29=(pn29/pn30)=(109/113)=0.^9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707

21Qn30=(pn30/pn31)=(113/127)=0.^88976377952755905511811023622047244094481

21Qn31=(pn31/pn32)=(127/131)=0.^969465648854961832061068015267175572519083

21Qn32=(pn32/pn33)=(131/137)=0.^95620437

21Qn33=(pn33/pn34)=(137/139)=0.^9856115107913669064748201438848920863309352517

21Qn34=(pn34/pn35)=(139/149)=0.^932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489

21Qn35=(pn35/pn36)=(149/151)=0.^986754966887417218543046357615894039735099337748344370860927152317880794701

21Qn36=(pn36/pn37)=(151/157)=0.^961783439490445859872611464968152866242038216560509554140127388535031847133757

21Qn37=(pn37/pn38)=(157/163)=0.^963190184049079754601226993865030674846625766871165644171779141104294478527607361

21Qn38=(pn38/pn39)=(163/167)=0.^9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011

21Qn39=(pn39/pn40)=(167/173)=0.^9653179190751445086705202312138728323699421

21Qn40=(pn40/pn41)=(173/179)=0.^96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513

21Qn41=(pn41/pn42)=(179/181)=0.^9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441

21Qn42=(pn42/pn43)=(181/191)=0.^94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109

21Qn43=(pn43/pn44)=(191/193)=0.^989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113

21Qn44=(pn44/pn45)=(193/197)=0.^979695431

21Qn45=(pn45/pn46)=(197/199)=0.^989949748743718592964824120603015075025125628140703517587939698492462311557763819095477386934673366834170854271356783919597

3rd tier 2nd Prime 1(21Q) base

Variants next set of prime radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 prime radicals decimal cycle limit or break in stem numeral factoring.

Factoring  for variables of 2Qnc1  and so on . . .

(Qn2/Qn1c1)=(0.6/0.6)=1

2Qn1=1

Variant prime radical divide

(Qn2/Qn1c2)=0.6/0.66=0.9^09

(Qn2/Qn1c3)=0.6/0.666=0.9^009 and so on . . .

then

(Qn3c1/Qn2)=0.714285/0.6=1.190475

2Qn2=1.190475

(Qn3c2/Qn2)=0.714285714285/0.6=1.1904759523808^3 and so on . . .

then

(Qn4c1/Qn3c1)=0.63/0.714285=0.8^819994 and so on . . .

2Qn3=0.8^819994 

(Qn5c1/Qn4c1)=0.^846153/0.^63=1.3431

2Qn4=1.3431

(Qn6c1/Qn5c1)=0.^7647058823529411/0.^846153=0.9037442192^522405

2Qn5=0.9037442192^522405

and so on . . .

12Q divide starting at 1(Qn2/Qn1) then 22Q divide starting at 2(Qn1/Qn2)

WHILE

in short 1(Qn2/Qn1) is not 2(Qn1/Qn2)

1(12Q)n1=(11Q)n2/(11Q)n1 is not 2(12Q)n2=(11Q)n1/(11Q)n2

4th tier 3rd Prime 1⅄(1(21Q) base

Variants next set of prime radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 prime radicals decimal cycle limit or break in stem numeral factoring.

Factoring  for variables of 3Qnc1  and so on . . .

∈{(Qn4/Qn3)/(Qn2/Qn1)}=2Qn2/2Qn1=^0.9/1=0.9

3Qn1=0.9 

then {(Qn4/Qn3)c2/(Qn2/Qn1)}=2Qn2c2/2Qn1=^0.909/1=0.909 and so on . . . where c2 is applicable to {(Qn4/Qn3)c2

∈{(Qn5/Qn4)/(Qn3/Qn2)}=2Qn3/2Qn2=1.190475/^0.9=1.32275

3Qn2=1.32275

then {(Qn5/Qn4)/(Qn3/Qn2)c2}=2Qn3/2Qn2c2=1.190475/^0.909=1.210^6435 and so on . . .

∈{(Qn6/Qn5)/(Qn4/Qn3)}=2Qn4/2Qn3=0.8^819994/1.190475=0.740^880236

3Qn3=0.740^880236

then {(Qn6/Qn5)c2/(Qn4/Qn3)}=2Qn4c2/2Qn3=0.8^819994819994/1.190475=0.740880305^759801 and so on . . .

5th tier 4th Prime 1(1⅄(1(21Q) base

Variants next set of prime radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 prime radicals decimal cycle limit or break in stem numeral factoring.

Factoring  for variables of 4Qnc1  and so on . . .

(3Qn2/3Qn1)=1.4679

4Qn1=1.4679

then (3Qn2/3Qn1c2)=1.45^517

(3Qn3/3Qn2)=0.5601060^18522

4Qn2=0.5601060^18522

then (3Qn3c2/3Qn2)=0.560106019187^477603 and so on . . .

6th tier 5th Prime 1(1(1⅄(1(21Q) base

Variants next set of prime radical decimal stem path factoring to the degree of the variant decimal cycles per array.

Quadratic equations dependent of 4 prime radicals decimal cycle limit or break in stem numeral factoring.

Factoring  for variables of 5Qnc1  and so on . . .

(3Qn3/3Qn2)/(3Qn2/3Qn1)=(4Qn2/4Qn1)=(0.5601060^18522/1.4679)

5Qn1=0.3815696018270999386879215205395462906192519926425505824647455548744464881803937597929014238027113563594182199059881470113767967845221064105184277685809660058587097213706655766741603651474896110089243136453436882621472852374139465222426595817153757067920158489134137202806730703726411880918318686559029906669391647932420464609303767286599906256556986170720076299475441106342393896041964779617140132165913890592002799850126030383541113154847039989100076299475441106342393896041964711492608488316642823080591320934668574153552694325226514067715784453981878874582737243681449690033371020505^48402479732951835956809046937802302609160956195926153007698072071667007745827372436814496900333810205054

Q Alternate Base Path Variants 2nd tier of Q and third divide of P prime base quotient ratios

1(1Qn2/1Qn1) and 1(2Qn2/2Qn1) are the first ratio definitions of the sets structured from each equation.

12Q for each is then respectably 12Q of (1Qn2/1Qn1) and 12Q of (2Qn2/2Qn1)

Then if 

L=1(1Qn2/2Qn1)

K=2(1Qn1/2Qn2)

U=1(2Qn2/1Qn1)

J=2(2Qn1/1Qn2)

Path Set 12Q pertains to base equations

12Q of (1Qn2/1Qn1) and 12Q of (2Qn2/2Qn1) and (L) 12Q of (1Qn2/2Qn1) and (U) 12Q of (2Qn2/1Qn1)


Then

1(12Q)n1=[12Q=(1Qn2c1/1Qn1c1)]=(1.^6/1.5)=1.0^6

1(12Q)n2=[12Q=(1Qn3c1/1Qn2c1)]=(1.4/1.^6)=0.875

1(12Q)n3=[12Q=(1Qn4c1/1Qn3c1)]=(1.^571428/1.4)=1.12244^857142

1(12Q)n4=[12Q=(1Qn5c1/1Qn4c1)]=(1.^18/1.^571428)

1(12Q)n5=[12Q=(1Qn6c1/1Qn5c1)]=(1.^307692/1.^18)

1(12Q)n6=[12Q=(1Qn7c1/1Qn6c1)]=(1.^1176470588235294/1.^307692)

1(12Q)n7=[12Q=(1Qn8c1/1Qn7c1)]=(1.^210526315789473684/1.^1176470588235294)

1(12Q)n8=[12Q=(1Qn9c1/1Qn8c1)]=(1.^2608695652173913043478/1.^210526315789473684)

1(12Q)n9=[12Q=(1Qn10c1/1Qn9c1)]=(1.^0689655172413793103448275862/1.^2608695652173913043478)

1(12Q)n10=[12Q=(1Qn11c1/1Qn10c1)]=(1.^193548387096774/1.^0689655172413793103448275862)

1(12Q)n11=[12Q=(1Qn12c1/1Qn11c1)]=(1.^108/1.^193548387096774)

1(12Q)n12=[12Q=(1Qn13c1/1Qn12c1)]=(1.^04878/1.^108)

1(12Q)n13=[12Q=(1Qn14c1/1Qn13c1)]=(1.^093023255813953488372/1.^04878)

1(12Q)n14=[12Q=(1Qn15c1/1Qn14c1)]=(1.^12765957446808510638297872340425531914893610702/1.^093023255813953488372)

1(12Q)n15=[12Q=(1Qn16c1/1Qn15c1)]=(1.^1132075471698/1.^12765957446808510638297872340425531914893610702)

1(12Q)n16=[12Q=(1Qn17c1/1Qn16c1)]=(1.^0338983050847457627118644067796610169491525423728813559322/1.^1132075471698)

1(12Q)n17=[12Q=(1Qn18c1/1Qn17c1)]=(1.^098360655737704918032786885245901639344262295081967213114754/1.^0338983050847457627118644067796610169491525423728813559322)

1(12Q)n18=[12Q=(1Qn19c1/1Qn18c1)]=(1.^059701492537313432835820895522388/1.^098360655737704918032786885245901639344262295081967213114754)

1(12Q)n19=[12Q=(1Qn20c1/1Qn19c1)]=(1.^02816901408450704225352112676056338/1.^059701492537313432835820895522388)

1(12Q)n20=[12Q=(1Qn21c1/1Qn20c1)]=(1.^08219178/1.^02816901408450704225352112676056338)

1(12Q)n21=[12Q=(1Qn22c1/1Qn21c1)]=(1.^0506329113924/1.^08219178)

1(12Q)n22=[12Q=(1Qn23c1/1Qn22c1)]=(1.^07228915662650602409638554216867469879518/1.^0506329113924)

1(12Q)n23=[12Q=(1Qn24c1/1Qn23c1)]=(1.^08988764044943820224719101123595505617977528/1.^07228915662650602409638554216867469879518)

1(12Q)n24=[12Q=(1Qn25c1/1Qn24c1)]=(1.^04123092783505154639175257731958762886597938144329896907216494845360820618/1.^08988764044943820224719101123595505617977528)

1(12Q)n25=[12Q=(1Qn26c1/1Qn25c1)]=(1.^0198/1.^04123092783505154639175257731958762886597938144329896907216494845360820618)

1(12Q)n26=[12Q=(1Qn27c1/1Qn26c1)]=(1.^0388349514563106796111662136504854368932/1.^0198)

1(12Q)n27=[12Q=(1Qn28c1/1Qn27c1)]=(1.^01869158878504672897196261682242990654205607476635514/1.^0388349514563106796111662136504854368932)

1(12Q)n28=[12Q=(1Qn29c1/1Qn28c1)]=(1.^0366972477064220183486238532110091743119266055045871559633027522935779816513758712844/1.^01869158878504672897196261682242990654205607476635514)

1(12Q)n29=[12Q=(1Qn30c1/1Qn29c1)]=(1.^123893805308849557522/1.^0366972477064220183486238532110091743119266055045871559633027522935779816513758712844)

1(12Q)n30=[12Q=(1Qn31c1/1Qn30c1)]=(1.^031496062992125984251968503937007874015748/1.^123893805308849557522)

1(12Q)n31=[12Q=(1Qn32c1/1Qn31c1)]=(1.^045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374/1.^031496062992125984251968503937007874015748)

1(12Q)n32=[12Q=(1Qn33c1/1Qn32c1)]=(1.^01459854/1.^045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374)

1(12Q)n33=[12Q=(1Qn34c1/1Qn33c1)]=(1.^071942446043165474820143884892086330935251798561151080291955395683453237410/1.^01459854)

1(12Q)n34=[12Q=(1Qn35c1/1Qn34c1)]=(1.^01343624295302/1.^071942446043165474820143884892086330935251798561151080291955395683453237410)

1(12Q)n35=[12Q=(1Qn36c1/1Qn35c1)]=(1.^0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894/1.^01343624295302)

1(12Q)n36=[12Q=(1Qn37c1/1Qn36c1)]=(1.^038216560509554140127388535031847133757961783439490445859872611464968152866242/1.^0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894)

1(12Q)n37=[12Q=(1Qn38c1/1Qn37c1)]=(1.^024539877300613496932515337423312883435582822085889570552147239263803680981595092/1.^038216560509554140127388535031847133757961783439490445859872611464968152866242)

1(12Q)n38=[12Q=(1Qn39c1/1Qn38c1)]=(1.^0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982/1.^024539877300613496932515337423312883435582822085889570552147239263803680981595092)

1(12Q)n39=[12Q=(1Qn40c1/1Qn39c1)]=(1.^034682080924554913294797687861271676300578/1.^0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982)

1(12Q)n40=[12Q=(1Qn41c1/1Qn40c1)]=(1.^0111731843575418994413407821229050279329608936536312849162/1.^034682080924554913294797687861271676300578)

1(12Q)n41=[12Q=(1Qn42c1/1Qn41c1)]=(1.^005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779/1.^0111731843575418994413407821229050279329608936536312849162)

1(12Q)n42=[12Q=(1Qn43c1/1Qn42c1)]=(1.^01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178/1.^005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779)

1(12Q)n43=[12Q=(1Qn44c1/1Qn43c1)]=(1.^02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772/1.^01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178)

1(12Q)n44=[12Q=(1Qn45c1/1Qn44c1)]=(1.^01015228426395939086294416243654822335025380710659898477157360406091370558375634517766497461928934/1.^02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772)

and so on for variables of 1(12Q)n=[12Q=(1Qn2cn/1Qn1cn)] that vary to degrees of stem cycle count variant 1(12Q)ncn


Functions applicable to variables of 1(12Q)ncn=[12Q=(1Qn2cn/1Qn1cn)]


X⅄=(n2xn1) example X(12Q)n=[X2Q=(1Qn2cnx1Qn1cn)] 


+⅄=(nncn+nncn) example +(12Q)n=[+2Q=(1Qn2cn+1Qn1cn)]


1-⅄=(n2-n1) example 1-(12Q)n=[1-2Q=(1Qn2cn-1Qn1cn)]

3rd tier of Q and 4th divide of P prime base quotient ratios

Then example 1(13Q)n1 of (12Qn2c1/12Qn1c1)] so

1(13Q)n1 of (12Qn2c1/12Qn1c1)]=(0.875/1.0^6)=0.82^5471698113207

1(13Q)n2 of (12Qn3c1/12Qn2c1)]=(1.12244^857142/0.875)=1.28279836733^714285

1(13Q)n of (12Qn4c1/12Qn3c1)]=[(1Qn5c1/1Qn4c1)/(1Qn4c1/1Qn3c1)]=[(1.^18/1.^571428)/(1.^571428/1.4)]

and so on for variables of ∈1(13Q)ncn of (12Qn2c1/12Qn1c1)] 


4th tier of Q and 5th divide of P prime base quotient ratios

Then example 1(14Q)n1 of (13Qn2c1/13Qn1c1)] so

1(14Q)n1 of (13Qn2c1/13Qn1c1)]=(1.28279836733^714285/0.82^5471698113207)

1(14Q)n1 of (13Qn2c1/13Qn1c1)]=[(12Qn4c1/12Qn3c1)/(12Qn3c1/12Qn2c1)]

and so on for variables of ∈1(14Q)ncn of (13Qn2c1/13Qn1c1)] 


Again Q Alternate Base Path Variants 2nd tier of Q and third divide of P prime base quotient ratios

if 12Q=[1(12Q)=(1Qn2cn/1Qn1cn)] and 12Q=[1(22Q)=(2Qn2cn/2Qn1cn)] if ∈12Q=(Nn2cn/Nn1cn)

Then 12Q=[1(22Q)=(2Qn2cn/2Qn1cn)]=[(Pn2/Pn3)/(Pn1/Pn2)]=[(3/5)/(2/3)]=(0.6/0.^6)=1 if cn of 2Qn1cn ia 1 stem decimal cycle for variable 2Qn1c1

1(12Q)n1=[12Q=(2Qn2c1/2Qn1c1)]=(0.6/0.^6)=1

1(12Q)n2=[12Q=(2Qn3c1/2Qn2c1)]=(0.^714285/0.6)=1.190475

1(12Q)n3=[12Q=(2Qn4c1/2Qn3c1)]=(0.^63/0.^714285)=0.^882000

1(12Q)n4=[12Q=(2Qn5c1/2Qn4c1)]=(0.^846153/0.^63)=1.3431

1(12Q)n5=[12Q=(2Qn6c1/2Qn5c1)]=(0.^7647058823529411/0.^846153)=0.9037442192^522405

1(12Q)n6=[12Q=(2Qn7c1/2Qn6c1)]=(0.^894736842105263157/0.^7647058823529411)=1.17^0040485829959630

1(12Q)n7=[12Q=(2Qn8c1/2Qn7c1)]=(0.^8260869565217391304347/0.^894736842105263157)=0.9232^736572890025584679383631713554996444089514066496172914677749360613819973501278772378525855854219948849114091148337595907937620560102301790290561

1(12Q)n8=[12Q=(2Qn9c1/2Qn8c1)]=(0.^7931034482758620689655172413/0.^8260869565217391304347)=0.960072^595281306715063616878306896551724137940635199110707803992741431940963702359346642564246727949183303085309056251742286751361162484572542649727767695195825675317604355716888003620163339382940109852993595281306715063616878306896551724137940635199110707803992741431940963702359346642564246727949183303085309056251742286751361162484572542649727767695195825675317604355716888003620163339382940109852993

1(12Q)n9=[12Q=(2Qn10c1/2Qn9c1)]=(0.^935483870967741/0.^7931034482758620689655172413)

1(12Q)n10=[12Q=(2Qn11c1/2Qn10c1)]=(0.^837/0.^935483870967741)

1(12Q)n11=[12Q=(2Qn12c1/2Qn11c1)]=(0.^9024390243/0.^837)

1(12Q)n12=[12Q=(2Qn13c1/2Qn12c1)]=(0.^953488372093023255813/0.^9024390243)

1(12Q)n13=[12Q=(2Qn14c1/2Qn13c1)]=(0.^9148936170212765957446808510638297872340425531/0.^953488372093023255813)

1(12Q)n14=[12Q=(2Qn15c1/2Qn14c1)]=(0.^88679245283018867924528301/0.^9148936170212765957446808510638297872340425531)

1(12Q)n15=[12Q=(2Qn16c1/2Qn15c1)]=(0.^8983050847457627118644067796610169491525423728813559322033/0.^88679245283018867924528301)

1(12Q)n16=[12Q=(2Qn17c1/2Qn16c1)]=(0.^967213114754098360655737704918032786885245901639344262295081/0.^8983050847457627118644067796610169491525423728813559322033)

1(12Q)n17=[12Q=(2Qn18c1/2Qn17c1)]=(0.^910447761194029850746268656716417/0.^967213114754098360655737704918032786885245901639344262295081)

1(12Q)n18=[12Q=(2Qn19c1/2Qn18c1)]=(0.^94366197183098591549295774647887323/0.^910447761194029850746268656716417)

1(12Q)n19=[12Q=(2Qn20c1/2Qn19c1)]=(0.^97260273/0.^94366197183098591549295774647887323)

1(12Q)n20=[12Q=(2Qn21c1/2Qn20c1)]=(0.^9240506329113/0.^97260273)

1(12Q)n21=[12Q=(2Qn22c1/2Qn21c1)]=(0.^95180722891566265060240963855421686746987/0.^9240506329113)

1(12Q)n22=[12Q=(2Qn23c1/2Qn22c1)]=(0.^93258426966292134831460674157303370786516853/0.^95180722891566265060240963855421686746987)

1(12Q)n23=[12Q=(2Qn24c1/2Qn23c1)]=(0.^917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463/0.^93258426966292134831460674157303370786516853)

1(12Q)n24=[12Q=(2Qn25c1/2Qn24c1)]=(0.^9603/0.^917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463)

1(12Q)n25=[12Q=(2Qn26c1/2Qn25c1)]=(0.^9805825242718446601941747572815533/0.^9603)

1(12Q)n26=[12Q=(2Qn27c1/2Qn26c1)]=(0.^96261682242990654205607476635514018691588785046728971/0.^9805825242718446601941747572815533)

1(12Q)n27=[12Q=(2Qn28c1/2Qn27c1)]=(0.^0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577/0.^96261682242990654205607476635514018691588785046728971)

1(12Q)n28=[12Q=(2Qn29c1/2Qn28c1)]=(0.^9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707/0.^0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577)

1(12Q)n29=[12Q=(2Qn30c1/2Qn29c1)]=(0.^88976377952755905511811023622047244094481/0.^9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707)

1(12Q)n30=[12Q=(2Qn31c1/2Qn30c1)]=(0.^969465648854961832061068015267175572519083/0.^88976377952755905511811023622047244094481)

1(12Q)n31=[12Q=(2Qn32c1/2Qn31c1)]=(0.^95620437/0.^969465648854961832061068015267175572519083)

1(12Q)n32=[12Q=(2Qn33c1/2Qn32c1)]=(0.^9856115107913669064748201438848920863309352517/0.^95620437)

1(12Q)n33=[12Q=(2Qn34c1/2Qn33c1)]=(0.^932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489/0.^9856115107913669064748201438848920863309352517)

1(12Q)n34=[12Q=(1Qn35c1/2Qn34c1)]=(0.^986754966887417218543046357615894039735099337748344370860927152317880794701/0.^932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489)

1(12Q)n35=[12Q=(2Qn36c1/2Qn35c1)]=(0.^961783439490445859872611464968152866242038216560509554140127388535031847133757/0.^986754966887417218543046357615894039735099337748344370860927152317880794701)

1(12Q)n36=[12Q=(2Qn37c1/2Qn36c1)]=(0.^963190184049079754601226993865030674846625766871165644171779141104294478527607361/0.^961783439490445859872611464968152866242038216560509554140127388535031847133757)

1(12Q)n37=[12Q=(2Qn38c1/2Qn37c1)]=(0.^9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011/0.^963190184049079754601226993865030674846625766871165644171779141104294478527607361)

1(12Q)n38=[12Q=(2Qn39c1/2Qn38c1)]=(0.^9653179190751445086705202312138728323699421/0.^9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011)

1(12Q)n39=[12Q=(2Qn40c1/2Qn39c1)]=(0.^96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513/0.^9653179190751445086705202312138728323699421)

1(12Q)n40=[12Q=(2Qn41c1/2Qn40c1)]=(0.^9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441/0.^96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513)

1(12Q)n41=[12Q=(2Qn42c1/2Qn41c1)]=(0.^94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109/0.^9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441)

1(12Q)n42=[12Q=(2Qn43c1/2Qn42c1)]=(0.^989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113/0.^94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109)

1(12Q)n43=[12Q=(2Qn44c1/2Qn43c1)]=(0.^979695431/0.^989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113)

1(12Q)n44=[12Q=(2Qn45c1/2Qn44c1)]=(0.^989949748743718592964824120603015075025125628140703517587939698492462311557763819095477386934673366834170854271356783919597/0.^979695431)

and so on for variables of ∈1(22Q)n=[12Q=(2Qn2cn/2Qn1cn)] that vary to degrees of stem cycle count variant 1(22Q)ncn


Functions applicable to variables of ∈1(12Q)ncn=[12Q=(2Qn2cn/2Qn1cn)]


X⅄=(n2xn1) example X(12Q)n=[X2Q=(2Qn2cnx2Qn1cn)] 


+⅄=(nncn+nncn) example +(12Q)n=[+2Q=(2Qn2cn+2Qn1cn)]


1-⅄=(n2-n1) example 1-(12Q)n=[2-2Q=(1Qn2cn-2Qn1cn)]


3rd tier of Q and 4th divide of P prime base quotient ratios

Then example 1(13Q)n1 of (22Qn2c1/22Qn1c1)] so

1(13Q)n1 of (22Qn2c1/22Qn1c1)]=(1.190475/1)=1.190475

1(13Q)n2 of (22Qn3c1/22Qn2c1)]=(0.^882000/1.190475)=^0.74088 or 0.74088^074088

1(13Q)n3 of (22Qn4c1/22Qn4c1)]=(1.3431/0.^882000)

1(13Q)n4 of (22Qn5c1/22Qn4c1)]=(0.9037442192^522405/1.3431)

1(13Q)n5 of (22Qn6c1/22Qn5c1)]=(1.17^0040485829959630/0.9037442192^522405)

1(13Q)n6 of (22Qn7c1/22Qn6c1)]=(0.9232^736572890025584679383631713554996444089514066496172914677749360613819973501278772378525855854219948849114091148337595907937620560102301790290561/1.17^0040485829959630)

1(13Q)n7 of (22Qn8c1/22Qn7c1)]=(0.960072^595281306715063616878306896551724137940635199110707803992741431940963702359346642564246727949183303085309056251742286751361162484572542649727767695195825675317604355716888003620163339382940109852993595281306715063616878306896551724137940635199110707803992741431940963702359346642564246727949183303085309056251742286751361162484572542649727767695195825675317604355716888003620163339382940109852993/0.9232^736572890025584679383631713554996444089514066496172914677749360613819973501278772378525855854219948849114091148337595907937620560102301790290561)


1(13Q)n8 of (22Qn9c1/22Qn8c1)]=[(2Qn10c1/2Qn9c1)/(2Qn9c1/2Qn8c1)]


1(13Q)n9 of (22Qn10c1/22Qn9c1)]=[(2Qn11c1/2Qn10c1)/(2Qn10c1/2Qn9c1)]


and so on for variables of ∈1(13Q)ncn of (22Qn2c1/22Qn1c1)] from 2Q variables of Prime P base consecutives


4th tier of Q and 5th divide of P prime base quotient ratios

Then example 1(14Q)n1 of [(1(13Q)n2~(22Qn3c1/22Qn2c1)]/22Qn1c1) / 1(13Q)n1~(22Qn2c1/22Qn1c1)]] so

1(14Q)n1 of [(1(13Q)n2/1(13Q)n1=[(0.^882000/1.190475)/(1.190475/1)]=(0.74088/1.190475)=0.6^223398

1(14Q)n2 of [(1(13Q)n3/1(13Q)n2=[(22Qn4c1/22Qn4c1)/(22Qn3c1/22Qn2c1)]

and so on for variables of ∈1(14Q)n1 of [(1(13Q)n2/1(13Q)n1 from variables of1(13Q)ncn of (22Qn2c1/22Qn1c1)] derived from  2Q variables of Prime P base consecutives


Q Alternate Base Path Variants 2nd tier of Q and third divide of P prime base quotient ratios

1(1Qn2/1Qn1) and 1(2Qn2/2Qn1) are the first ratio definitions of the sets structured from each equation.

12Q for each is then respectably 12Q of (1Qn2/1Qn1) and 12Q of (2Qn2/2Qn1)

Then if 

L=1(1Qn2/2Qn1)

K=2(1Qn1/2Qn2)

U=1(2Qn2/1Qn1)

J=2(2Qn1/1Qn2)

Path Set 12Q pertains to base equations

12Q of (1Qn2/1Qn1) and 12Q of (2Qn2/2Qn1) and (L) 12Q of (1Qn2/2Qn1) and (U) 12Q of (2Qn2/1Qn1)

So then 

2(1Qn1/1Qn2) and 2(2Qn1/2Qn2) for 22Q each is then respectably 22Q of (1Qn1/1Qn2) and 22Q of (2Qn1/2Qn2) that differ from sets ∈L ∈K ∈U and ∈J

22Qn1 of (1Qn1/1Qn2)=(1.5/1.^6)

22Qn2 of (1Qn2/1Qn3)=(1.^6/1.4)

22Qn3 of (1Qn3/1Qn4)=(1.4/1.^571428)

22Qn4 of (1Qn4/1Qn5)=(1.^571428/1.^18)

22Qn5 of (1Qn5/1Qn6)=(1.^18/1.^307692)

22Qn6 of (1Qn6/1Qn7)=(1.^307692/1.^1176470588235294)

22Qn7 of (1Qn7/1Qn8)=(1.^1176470588235294/1.^210526315789473684)

22Qn8 of (1Qn8/1Qn9)=(1.^210526315789473684/1.^2608695652173913043478)

22Qn9 of (1Qn9/1Qn10)=(1.^2608695652173913043478/1.^0689655172413793103448275862)

22Qn10 of (1Qn10/1Qn11)=(1.^0689655172413793103448275862/1.^193548387096774)

22Qn11 of (1Qn11/1Qn12)=(1.^193548387096774/1.^108)

22Qn12 of (1Qn12/1Qn13)=(1.^108/1.^04878)

22Qn13 of (1Qn13/1Qn14)=(1.^04878/1.^093023255813953488372)

22Qn14 of (1Qn14/1Qn15)=(1.^093023255813953488372/1.^12765957446808510638297872340425531914893610702)

22Qn15 of (1Qn15/1Qn16)=(1.^12765957446808510638297872340425531914893610702/1.^1132075471698)

22Qn16 of (1Qn16/1Qn17)=(1.^1132075471698/1.^0338983050847457627118644067796610169491525423728813559322)

22Qn17 of (1Qn17/1Qn18)=(1.^0338983050847457627118644067796610169491525423728813559322/1.^098360655737704918032786885245901639344262295081967213114754)

22Qn18 of (1Qn18/1Qn19)=(1.^098360655737704918032786885245901639344262295081967213114754/1.^059701492537313432835820895522388)

22Qn19 of (1Qn19/1Qn20)=(1.^059701492537313432835820895522388/1.^02816901408450704225352112676056338)

22Qn20 of (1Qn20/1Qn21)=(1.^02816901408450704225352112676056338/1.^08219178)

22Qn21 of (1Qn21/1Qn22)=(1.^08219178/1.^0506329113924)

22Qn22 of (1Qn22/1Qn23)=(1.^0506329113924/1.^07228915662650602409638554216867469879518)

22Qn23 of (1Qn23/1Qn24)=(1.^07228915662650602409638554216867469879518/1.^08988764044943820224719101123595505617977528)

22Qn24 of (1Qn24/1Qn25)=(1.^08988764044943820224719101123595505617977528/1.^04123092783505154639175257731958762886597938144329896907216494845360820618)

22Qn25 of (1Qn25/1Qn26)=(1.^04123092783505154639175257731958762886597938144329896907216494845360820618/1.^0198)

22Qn26 of (1Qn26/1Qn27)=(1.^0198/1.^0388349514563106796111662136504854368932)

22Qn27 of (1Qn27/1Qn28)=(1.^0388349514563106796111662136504854368932/1.^01869158878504672897196261682242990654205607476635514)

22Qn28 of (1Qn28/1Qn29)=(1.^01869158878504672897196261682242990654205607476635514/1.^0366972477064220183486238532110091743119266055045871559633027522935779816513758712844)

22Qn29 of (1Qn29/1Qn30)=(1.^0366972477064220183486238532110091743119266055045871559633027522935779816513758712844/1.^123893805308849557522)

22Qn30 of (1Qn30/1Qn31)=(1.^123893805308849557522/1.^031496062992125984251968503937007874015748)

22Qn31 of (1Qn31/1Qn32)=(1.^031496062992125984251968503937007874015748/1.^045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374)

22Qn32 of (1Qn32/1Qn33)=(1.^045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374/1.^01459854)

22Qn33 of (1Qn33/1Qn34)=(1.^01459854/1.^071942446043165474820143884892086330935251798561151080291955395683453237410)

22Qn34 of (1Qn34/1Qn35)=(1.^071942446043165474820143884892086330935251798561151080291955395683453237410/1.^01343624295302)

22Qn35 of (1Qn35/1Qn36)=(1.^01343624295302/1.^0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894)

22Qn36 of (1Qn36/1Qn37)=(1.^0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894/1.^038216560509554140127388535031847133757961783439490445859872611464968152866242)

22Qn37 of (1Qn37/1Qn38)=(1.^038216560509554140127388535031847133757961783439490445859872611464968152866242/1.^024539877300613496932515337423312883435582822085889570552147239263803680981595092)

22Qn38 of (1Qn38/1Qn39)=(1.^024539877300613496932515337423312883435582822085889570552147239263803680981595092/1.^0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982)

22Qn39 of (1Qn39/1Qn40)=(1.^0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982/1.^034682080924554913294797687861271676300578)

22Qn40 of (1Qn40/1Qn41)=(1.^034682080924554913294797687861271676300578/1.^0111731843575418994413407821229050279329608936536312849162)

22Qn41 of (1Qn41/1Qn42)=(1.^0111731843575418994413407821229050279329608936536312849162/1.^005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779)

22Qn42 of (1Qn42/1Qn43)=(1.^005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779/1.^01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178)

22Qn43 of (1Qn43/1Qn44)=(1.^01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178/1.^02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772)

22Qn44 of (1Qn44/1Qn45)=(1.^02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772/1.^01015228426395939086294416243654822335025380710659898477157360406091370558375634517766497461928934)

Again Q Alternate Base Path Variants 2nd tier of Q and third divide of P prime base quotient ratios

1(1Qn2/1Qn1) and 1(2Qn2/2Qn1) are the first ratio definitions of the sets structured from each equation.

12Q for each is then respectably 12Q of (1Qn2/1Qn1) and 12Q of (2Qn2/2Qn1)

Then if 

L=1(1Qn2/2Qn1)

K=2(1Qn1/2Qn2)

U=1(2Qn2/1Qn1)

J=2(2Qn1/1Qn2)

Path Set 12Q pertains to base equations

12Q of (1Qn2/1Qn1) and 12Q of (2Qn2/2Qn1) and (L) 12Q of (1Qn2/2Qn1) and (U) 12Q of (2Qn2/1Qn1)

So then 

2(1Qn1/1Qn2) and 2(2Qn1/2Qn2) for 22Q each is then respectably 22Q of (1Qn1/1Qn2) and 22Q of (2Qn1/2Qn2) that differ from sets ∈L ∈K ∈U and ∈J

22Qn1 of (2Qn1/2Qn2)=(0.^6/0.6)

22Qn2 of (2Qn2/2Qn3)=(0.6/0.^714285)

22Qn3 of (2Qn3/2Qn4)=(0.^714285/0.^63)

22Qn4 of (2Qn4/2Qn5)=(0.^63/0.^846153)

22Qn5 of (2Qn5/2Qn6)=(0.^846153/0.^7647058823529411)

22Qn6 of (2Qn6/2Qn7)=(0.^7647058823529411/0.^894736842105263157)

22Qn7 of (2Qn7/2Qn8)=(0.^894736842105263157/0.^8260869565217391304347)

22Qn8 of (2Qn8/2Qn9)=(0.^8260869565217391304347/0.^7931034482758620689655172413)

22Qn9 of (2Qn9/2Qn10)=(0.^7931034482758620689655172413/0.^935483870967741)

22Qn10 of (2Qn10/2Qn11)=(0.^935483870967741/0.^837)

22Qn11 of (2Qn11/2Qn12)=(0.^837/0.^9024390243)

22Qn12 of (2Qn12/2Qn13)=(0.^9024390243/0.^953488372093023255813)

22Qn13 of (2Qn13/2Qn14)=(0.^953488372093023255813/0.^9148936170212765957446808510638297872340425531)

22Qn14 of (2Qn14/2Qn15)=(0.^9148936170212765957446808510638297872340425531/0.^88679245283018867924528301)

22Qn15 of (2Qn15/2Qn16)=(0.^88679245283018867924528301/0.^8983050847457627118644067796610169491525423728813559322033)

22Qn16 of (2Qn16/2Qn17)=(0.^8983050847457627118644067796610169491525423728813559322033/0.^967213114754098360655737704918032786885245901639344262295081)

22Qn17 of (2Qn17/2Qn18)=(0.^967213114754098360655737704918032786885245901639344262295081/0.^910447761194029850746268656716417)

22Qn18 of (2Qn18/2Qn19)=(0.^910447761194029850746268656716417/0.^94366197183098591549295774647887323)

22Qn19 of (2Qn19/2Qn20)=(0.^94366197183098591549295774647887323/0.^97260273)

22Qn20 of (2Qn20/2Qn21)=(0.^97260273/0.^9240506329113)

22Qn21 of (2Qn21/2Qn22)=(0.^9240506329113/0.^95180722891566265060240963855421686746987)

22Qn22 of (2Qn22/2Qn23)=(0.^95180722891566265060240963855421686746987/0.^93258426966292134831460674157303370786516853)

22Qn23 of (2Qn23/2Qn24)=(0.^93258426966292134831460674157303370786516853/0.^917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463)

22Qn24 of (2Qn24/2Qn25)=(0.^917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463/0.^9603)

22Qn25 of (2Qn25/2Qn26)=(0.^9603/0.^9805825242718446601941747572815533)

22Qn26 of (2Qn26/2Qn27)=(0.^9805825242718446601941747572815533/0.^96261682242990654205607476635514018691588785046728971)

22Qn27 of (2Qn27/2Qn28)=(0.^96261682242990654205607476635514018691588785046728971/0.^0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577)

22Qn28 of (2Qn28/2Qn29)=(0.^0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577/0.^9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707)

22Qn29 of (2Qn29/2Qn30)=(0.^9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707/0.^88976377952755905511811023622047244094481)

22Qn30 of (2Qn30/2Qn31)=(0.^88976377952755905511811023622047244094481/0.^969465648854961832061068015267175572519083)

22Qn31 of (2Qn31/2Qn32)=(0.^969465648854961832061068015267175572519083/0.^95620437)

22Qn32 of (2Qn32/2Qn33)=(0.^95620437/0.^9856115107913669064748201438848920863309352517)

22Qn33 of (2Qn33/2Qn34)=(0.^9856115107913669064748201438848920863309352517/0.^932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489)

22Qn34 of (2Qn34/2Qn35)=(0.^932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489/0.^986754966887417218543046357615894039735099337748344370860927152317880794701)

22Qn35 of (2Qn35/2Qn36)=(0.^986754966887417218543046357615894039735099337748344370860927152317880794701/0.^961783439490445859872611464968152866242038216560509554140127388535031847133757)

22Qn36 of (2Qn36/2Qn37)=(0.^961783439490445859872611464968152866242038216560509554140127388535031847133757/0.^963190184049079754601226993865030674846625766871165644171779141104294478527607361)

22Qn37 of (2Qn37/2Qn38)=(0.^963190184049079754601226993865030674846625766871165644171779141104294478527607361/0.^9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011)

22Qn38 of (2Qn38/2Qn39)=(0.^9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011/0.^9653179190751445086705202312138728323699421)

22Qn39 of (2Qn39/2Qn40)=(0.^9653179190751445086705202312138728323699421/0.^96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513)

22Qn40 of (2Qn40/2Qn41)=(0.^96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513/0.^9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441)

22Qn41 of (2Qn41/2Qn42)=(0.^9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441/0.^94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109)

22Qn42 of (2Qn42/2Qn43)=(0.^94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109/0.^989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113)

22Qn43 of (2Qn43/2Qn44)=(0.^989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113/0.^979695431)

22Qn44 of (2Qn44/2Qn45)=(0.^979695431/0.^989949748743718592964824120603015075025125628140703517587939698492462311557763819095477386934673366834170854271356783919597)

Prime 12Q and 22Q Base Path Variants

11Qn1 and ∈21Qn1 with definition of 3⅄ and 2⅄ and 1⅄ sets in prime base of p division logic.

As 3⅄ is not applicable to prime p numerals having no decimal cn change until decimal ratio cell stem cycles are a Q factor.

2⅄ and 1⅄ are paths of p prime consecutive numerals that divide later and previous as explained.

Now paths of two different Q bases labelled as 1Qn1 are in fact not simply 1Qn1

11Qn1 and 21Qn1 are paths of p prime consecutive numerals 2⅄ and 1

Each of the variant paths of 1Q can then be reapplied to their own three variant paths 3⅄ and 2⅄ and 1⅄ forming new sets that are not the same sets where cn is a variant factor in each set of the next tier stems cycles and cell definitions.

Variables of sets explained below are applicable to functions with prime p fibonacci y and phi φn base numerals through paths 1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc nncn numerically.

12Q and 22Q and 32Q then require further definition or symbol notation.

12

12Qn1 of 11Qn1 variables is (11Qn2/11Qn1)=(1.^6/1.5)=1.^06 for 11Qn2c1 variable and (11Qn2c2/11Qn1)=(1.^66/1.5)=1.1^06 and so on depending of cn variable factor

12Qn1 of 21Qn1 variables is (21Qn2/21Qn1)=(0.6/0.^6)=1 for 21Qn1c1 variable and (21Qn2/21Qn1c2)=(0.6/0.^66)=1.1 and so on depending of cn variable factor

then 

12Qn1 of 11Qn and 21Qn variables is (11Qn2/21Qn1)=(1.^6/0.^6)=2.^6 depending of cn variable factor c1

and

12Qn1 of 21Qn and 11Qn variables is (21Qn2/11Qn1)=(0.6/1.5)=0.4

and are crossed variants of two different path sets variables

22

22Qn1 of 11Qn1 variables is (11Qn1/11Qn2)

22Qn1 of 21Qn1 variables is (21Qn1/21Qn2)

then 

22Qn1 of 11Qn and 21Qn variables is (11Qn1/21Qn2) depending of cn variable factor

and

22Qn1 of 21Qn and 11Qn variables is (21Qn1/11Qn2) depending of cn variable factor

and are crossed variants of two different path sets variables

32

32Qn1 of 11Qn1 variables is (11Qn1cn/11Qn1cn)

32Qn1 of 21Qn1 variables is (21Qn1cn/21Qn1cn)

then 

32Qn1 of 11Qn and 21Qn variables is (11Qn1cn/21Qn1cn) depending of cn variable factor

and

32Qn1 of 21Qn and 11Qn variables is (21Qn1cn/11Qn2cn) depending of cn variable factor

and are crossed variants of two different path sets variables

Sets are factorable with AND differ from THESE VARIABLES DEFINITIONS

3rd tiers of Q alternate paths from prime base of 31Qcn sets

3(11Qn)cn/(21Qn)cn are not same set ∉ yet path of 3defines variables of same tier level and cn differential factors

and 

3(21Qn)cn/(11Qn)cn are not same set ∉ yet path of 3defines variables of same tier level and cn differential factors

and 

3(11Qn)cn/(11Qn)cn

and 

3(21Qn)cn/(21Qn)cn 

are applicable ratios to phi and y bases and tiers of the paths of φ of many functions as well as prime path variables sets tiers per variant cycle cn.


1⅄ and 2⅄ and 3⅄ of sets in Q's from P to Y and φ factoring at degrees of cn

13Q=(2Q/2Q)=(1Q/1Q)/(1Q/1Q)=(p/p) that 1Q lacks path root definition of 11Q or 21Q from base prime path P

23Q=(2Q/2Q)=(1Q/1Q)/(1Q/1Q)=(p/p) that 1Q lacks path root definition of 11Q or 21Q from base prime path P

33Q=(2Q/2Q)=(1Q/1Q)/(1Q/1Q)=(p/p) that 1Q lacks path root definition of 11Q or 21Q from base prime path P

So variables of sets 13Q, 23Q, 33Q, 12Q, 22Q, 32Q require definitions of variable from set 11Q or 21Q from base prime path P.

32Qn1 of ∈11Qn1 variables is (11Qn1/11Qn1)=(1.5/1.5)=1

32Qn2 of ∈11Qn1 variables is (11Qn2c1/11Qn2c2)=(1.^6/1.^66) and so on for cn differentials. . . 

32Qn2 of ∈11Qn1 variables is (11Qn2c2/11Qn2c1)=(1.^66/1.^6) and so on for cn differentials. . . 

32Qn3 of ∈11Qn1 variables is (11Qn3/11Qn3)=(1.4/1.4)=1

32Qn4 of ∈11Qn1 variables is (11Qn4c1/11Qn4c2)=(1.^571428/1.^571428571428) and so on for cn differentials. . . 

32Qn4 of ∈11Qn1 variables is (11Qn4c2/11Qn4c1)=(1.^571428571428/1.^571428) and so on for cn differentials. . . 

32Qn5 of ∈11Qn1 variables is (11Qn5c1/11Qn5c2)=(1.^18/1.^1818) and so on for cn differentials. . . 

32Qn5 of ∈11Qn1 variables is (11Qn5c2/11Qn5c1)=(1.^1818/1.^18) and so on for cn differentials. . . 

32Qn6 of ∈11Qn1 variables is (11Qn6c1/11Qn6c2)=(1.^307692/1.^307692307692) and so on for cn differentials. . . 

32Qn6 of ∈11Qn1 variables is (11Qn6c2/11Qn6c1)=(1.^307692307692/1.^307692) and so on for cn differentials. . . 

32Qn7 of ∈11Qn1 variables is (11Qn7c1/11Qn7c2)=(1.^1176470588235294/1.^11764705882352941176470588235294) and so on for cn differentials. . . 

32Qn7 of ∈11Qn1 variables is (11Qn7c2/11Qn7c1)=(1.^11764705882352941176470588235294/1.^1176470588235294) and so on for cn differentials. . . 

32Qn8 of ∈11Qn1 variables is (11Qn8c1/11Qn8c2)=(1.^210526315789473684/1.^210526315789473684210526315789473684) and so on for cn differentials. . . 

32Qn8 of ∈11Qn1 variables is (11Qn8c2/11Qn8c1)=(1.^210526315789473684210526315789473684/1.^210526315789473684) and so on for cn differentials. . . 

Beginning with 

32Qn1 of ∈21Qn1 variables is (21Qn1cn/21Qn1cn)=(0.^6/0.^6)=1

32Qn1 of ∈21Qn1 variables is (21Qn1c1/21Qn1c2)=(0.^6/0.^66)

32Qn1 of ∈21Qn1 variables is (21Qn1c2/21Qn1c1)=(0.^66/0.^6)=1.1 and so on for cn of variable ∈32Qn1 of ∈21Qn1cn

32Qn2 of ∈21Qn1 variables is (21Qn2cn/21Qn2cn)=(0.6/0.6)=1 and has no cn variable change potential in decimal.

32Qn3 of ∈21Qn1 variables is (21Qn3cn/21Qn3cn)=(0.^714285/0.^714285)

32Qn3 of ∈21Qn1 variables is (21Qn3c1/21Qn3c2)=(0.^714285/0.^714285714285)

32Qn3 of ∈21Qn1 variables is (21Qn3c2/21Qn3c1)=(0.^714285714285/0.^714285) and so on for cn of variable ∈32Qn3 of ∈21Qn1cn

32Qn4 of ∈21Qn1 variables is (21Qn4cn/21Qn4cn)=(0.^63/0.^63)

32Qn4 of ∈21Qn1 variables is (21Qn4c1/21Qn4c2)=(0.^63/0.^6363)

32Qn4 of ∈21Qn1 variables is (21Qn4c2/21Qn4c1)=(0.^6363/0.^63) and so on for cn of variable ∈32Qn4 of ∈21Qn1cn

32Qn5 of ∈21Qn1 variables is (21Qn5cn/21Qn5cn)=(0.^846153/0.^846153)

32Qn5 of ∈21Qn1 variables is (21Qn5c1/21Qn5c2)=(0.^846153/0.^846153846153)

32Qn5 of ∈21Qn1 variables is (21Qn5c2/21Qn5c1)=(0.^846153846153/0.^846153) and so on for cn of variable ∈32Qn5 of ∈21Qn1cn

32Qn6 of ∈21Qn1 variables is (21Qn6cn/21Qn6cn)=(0.^7647058823529411/0.^7647058823529411)

32Qn6 of ∈21Qn1 variables is (21Qn6c1/21Qn6c2)=(0.^7647058823529411/0.^76470588235294117647058823529411)

32Qn6 of ∈21Qn1 variables is (21Qn6c2/21Qn6c1)=(0.^76470588235294117647058823529411/0.^7647058823529411) and so on for cn of variable ∈32Qn6 of ∈21Qn1cn

32Qn7 of ∈21Qn1 variables is (21Qn7cn/21Qn7cn)=(0.^894736842105263157/0.^894736842105263157)

32Qn7 of ∈21Qn1 variables is (21Qn7c1/21Qn7c2)=(0.^894736842105263157/0.^894736842105263157894736842105263157)

32Qn7 of ∈21Qn1 variables is (21Qn7c2/21Qn7c1)=(0.^894736842105263157894736842105263157/0.^894736842105263157) and so on for cn of variable ∈32Qn7 of ∈21Qn1cn

32Qn8 of ∈21Qn1 variables is (21Qn8cn/21Qn8cn)=(0.^8260869565217391304347/0.^8260869565217391304347)

32Qn8 of ∈21Qn1 variables is (21Qn8c1/21Qn8c2)=(0.^8260869565217391304347/0.^82608695652173913043478260869565217391304347)

32Qn8 of ∈21Qn1 variables is (21Qn8c2/21Qn8c1)=(0.^82608695652173913043478260869565217391304347/0.^8260869565217391304347) and so on for cn of variable ∈32Qn8 of ∈21Qn1cn

Beginning with

32Qn1 of ∈11Qn and ∈21Qn variables is (11Qn1cn/21Qn1cn) depending of cn variable factor

32Qn1 of ∈11Qn and ∈21Qn variables is 

(11Qn1c1/21Qn1c1)=(1.5/0.^6)

(11Qn1c1/21Qn1c2)=(1.5/0.^66)

(11Qn1c1/21Qn1c3)=(1.5/0.^666) and so on for cn variable factor

32Qn2 of ∈11Qn and ∈21Qn variables is 

(11Qn2c1/21Qn2c1)=(1.^6/0.6)

(11Qn2c2/21Qn2c1)=(1.^66/0.6)

(11Qn2c3/21Qn2c1)=(1.^666/0.6) and so on for cn variable factor

32Qn3 of ∈11Qn and ∈21Qn variables is 

(11Qn3c1/21Qn3c1)=(1.4/0.^714285)

(11Qn3c1/21Qn3c2)=(1.4/0.^714285714285)

(11Qn3c1/21Qn3c3)=(1.4/0.^714285714285714285) and so on for cn variable factor

32Qn4 of ∈11Qn and ∈21Qn variables is 

(11Qn4c1/21Qn4c1)=(1.^571428/0.^63)

(11Qn4c1/21Qn4c2)=(1.^571428/0.^6363)

(11Qn4c2/21Qn4c1)=(1.^571428571428/0.^63)

(11Qn4c3/21Qn4c2)=(1.^571428571428571428/0.^6363)

(11Qn4c2/21Qn4c3)=(1.^571428571428/0.^636363)

(11Qn4c3/21Qn4c1)=(1.^571428571428571428/0.^63)

(11Qn4c1/21Qn4c3)=(1.^571428/0.^636363) and so on for cn variable factor

32Qn5 of ∈11Qn and ∈21Qn variables is 

(11Qn5c1/21Qn5c1)=(1.^18/0.^846153)

(11Qn5c1/21Qn5c2)=(1.^18/0.^846153846153)

(11Qn5c2/21Qn5c1)=(1.^1818/0.^846153) and so on for cn variable factor

32Qn6 of ∈11Qn and ∈21Qn variables is 

(11Qn6c1/21Qn6c1)=(1.^307692/0.^7647058823529411)

(11Qn6c1/21Qn6c2)=(1.^307692/0.^76470588235294117647058823529411)

(11Qn6c2/21Qn6c1)=(1.^307692307692/0.^7647058823529411) and so on for cn variable factor

32Qn7 of ∈11Qn and ∈21Qn variables is 

(11Qn7c1/21Qn7c1)=(1.^1176470588235294/0.^894736842105263157)

(11Qn7c1/21Qn7c2)=(1.^1176470588235294/0.^894736842105263157894736842105263157)

(11Qn7c2/21Qn7c1)=(1.^11764705882352941176470588235294/0.^894736842105263157) and so on for cn variable factor

32Qn8 of ∈11Qn and ∈21Qn variables is 

(11Qn8c1/21Qn8c1)=(1.^210526315789473684/0.^8260869565217391304347)

(11Qn8c1/21Qn8c2)=(1.^210526315789473684/0.^82608695652173913043478260869565217391304347)

(11Qn8c2/21Qn8c1)=(1.^210526315789473684210526315789473684/0.^8260869565217391304347) and so on for cn variable factor

Beginning with

32Qn1 of ∈21Qn and ∈11Qn variables is (21Qn1cn/11Qn2cn) depending of cn variable factor

32Qn1 of ∈21Qn and ∈11Qn variables is 

(21Qn1c1/11Qn1c1)=(0.^6/1.5)

(21Qn1c2/11Qn1c1)=(0.^66/1.5)

(21Qn1c3/11Qn1c1)=(0.^666/1.5) and so on for cn variable factor

32Qn2 of ∈21Qn and ∈11Qn variables is 

(21Qn2c1/11Qn2c1)=(0.6/1.^6)

(21Qn2c1/11Qn2c2)=(0.6/1.^66)

(21Qn2c1/11Qn2c3)=(0.6/1.^666) and so on for cn variable factor

32Qn3 of ∈21Qn and ∈11Qn variables is 

(21Qn3c1/11Qn3c1)=(0.^714285/1.4)

(21Qn3c2/11Qn3c1)=(0.^714285714285/1.4)

(21Qn3c3/11Qn3c1)=(0.^714285714285714285/1.4) and so on for cn variable factor

32Qn4 of ∈21Qn and ∈11Qn variables is 

(21Qn4c1/11Qn4c1)=(0.^63/1.^571428)

(21Qn4c1/11Qn4c2)=(0.^63/1.^571428571428)

(21Qn4c2/11Qn4c1)=(0.^6363/1.^571428)

(21Qn4c3/11Qn4c2)=(0.^636363/1.^571428571428)

(21Qn4c2/11Qn4c3)=(0.^6363/1.^571428571428571428)

(21Qn4c3/11Qn4c1)=(0.^636363/1.^571428)

(21Qn4c1/11Qn4c3)=(0.^63/1.^571428571428571428) and so on for cn variable factor

32Qn5 of ∈21Qn and ∈11Qn variables is 

(21Qn5c1/11Qn5c1)=(0.^846153/1.^18)

(21Qn5c1/11Qn5c2)=(0.^846153/1.^1818)

(21Qn5c2/11Qn5c1)=(0.^846153846153/1.^18) and so on for cn variable factor

32Qn6 of ∈21Qn and ∈11Qn variables is 

(21Qn6c1/11Qn6c1)=(0.^7647058823529411/1.^307692)

(21Qn6c1/11Qn6c2)=(0.^7647058823529411/1.^307692307692)

(21Qn6c2/11Qn6c1)=(0.^76470588235294117647058823529411/1.^307692) and so on for cn variable factor

32Qn7 of ∈21Qn and ∈11Qn variables is 

(21Qn7c1/11Qn7c1)=(0.^894736842105263157/1.^1176470588235294)

(21Qn7c1/11Qn7c2)=(0.^894736842105263157/1.^11764705882352941176470588235294)

(21Qn7c2/11Qn7c1)=(0.^894736842105263157894736842105263157/1.^1176470588235294) and so on for cn variable factor

32Qn8 of ∈21Qn and ∈11Qn variables is 

(21Qn8c1/11Qn8c1)=(0.^8260869565217391304347/1.^210526315789473684)

(21Qn8c1/11Qn8c2)=(0.^8260869565217391304347/1.^210526315789473684210526315789473684)

(21Qn8c2/11Qn8c1)=(0.^82608695652173913043478260869565217391304347/1.^210526315789473684) and so on for cn variable factor

Tier base ratio sets and paths of the variables of 1φn1/pn1 and pn1/φn1

3(1φn1/pn1)/(pn1/φn1)=(0/0)=0 and form more complex scale sets and tier variables of set

3(pn1/φn1)/(1φn1/pn1)=(0/0)=0 and form more complex scale sets and tier variables of set

2(1φn1/pn1)/(pn2/φn2) =(0/3)=0 and form more complex scale sets and tier variables of set

2(pn1/φn1)/(1φn2/pn2) =(0/0.^3)=0 and form more complex scale sets and tier variables of set

1(1φn2/pn2)/(pn1/φn1)=(0.^3/0)=0 and form more complex scale sets and tier variables of set

1(pn2/φn2)/(1φn1/pn1)=(3/0)=0 and form more complex scale sets and tier variables of set

Variable stem paths determined in factoring for (φn/pn)cn and (pn/φn)cn of sets 1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc n ncn 

Because of the complexity and decimal length of the variable factors with potential change given cn a short scale of examples will be displayed below and as the previous numerals have shown, extreme precision can be factored of these arc variable definitions.

Alternate combinations of sequences and variables can be factored that are real numbers defined. 

For now here are the basics of this fractal polarization in quantum field variables assuming cn is one cycle stem to two

BASE SET of 3φn/pn

3(1φn1/pn1)/(pn1/φn1)=(0/0)=0

3(1φn2/pn2)/(pn2/φn2)=(0.^3/3)=0.1 and 3(1φn2/pn2)c2/(pn2/φn2)=(0.^33/3)=0.11 and so on . . .

3(1φn3/pn3)/(pn1/φn3)=(0.4/2.5)=0.16

3(1φn4/pn4)/(pn4/φn4)=(0.2^142857/4)=0.053571425 

and 3(1φn4/pn4)c2/(pn4/φn4)=(0.2^142857/4)=0.053571428571425

3(1φn5/pn5)/(pn5/φn5)=(1.^45/6.875

and 3(1φn5c2/pn5)/(pn5/φn5c2)=(0.150^9/6.6265060^24096084337349397590361445784337951712047)

and 3(1φn5/pn5)/(pn5/φn5c2)=(1.^45/6.6265060^24096084337349397590361445784337951712047)

and 3(1φn5c2/pn5)/(pn5/φn5c2)=(0.150^9/6.875) of 3(1φn5/pn5)/(pn5/φn5)c1 bases 

alternate paths variable function examples 3(1φn5/pn5)c2/(pn5/φn5)=(1.^4545/6.875

and 3(1φn5c2/pn5)c2/(pn5/φn5c2)=(0.150^99/6.6265060^24096084337349397590361445784337951712047)

and 3(1φn5c2/pn5)c2/(pn5/φn5c2)c2=(0.150^99/6.6265060^2409608433734939759036144578433795171204724096084337349397590361445784337951712047)

and 3(1φn5c2/pn5)/(pn5/φn5c2)c2=(0.150^9/6.6265060^2409608433734939759036144578433795171204724096084337349397590361445784337951712047)

and 3(1φn5/pn5)c2/(pn5/φn5c2)=(1.^4545/6.6265060^24096084337349397590361445784337951712047)

and 3(1φn5/pn5)c2/(pn5/φn5c2)c2=(1.^4545/6.6265060^2409608433734939759036144578433795171204724096084337349397590361445784337951712047)

and 3(1φn5/pn5)/(pn5/φn5c2)c2=(1.^45/6.6265060^2409608433734939759036144578433795171204724096084337349397590361445784337951712047)

and 3(1φn5c2/pn5)c2/(pn5/φn5c2)=(0.150^99/6.875) and 3(1φn5c2/pn5)c3/(pn5/φn5c2)=(0.150^999/6.875) variants

3(1φn6/pn6)/(pn6/φn6)=(0.1^230769/8.125) and 3(1φn6/pn6)c2/(pn6/φn6)=(0.1^230769230769/8.125)

3(1φn7/pn7)/(pn7/φn7)=(0.095^5882352941176470/10.46150^76923)

3(1φn7/pn7)c2/(pn7/φn7)=(0.095^58823529411764705882352941176470/10.46150^76923)

3(1φn7/pn7)c2/(pn7/φn7)c2=(0.095^58823529411764705882352941176470/10.46150^7692376923)

3(1φn7/pn7)/(pn7/φn7)c2=(0.095^5882352941176470/10.46150^76923)

and so on . . . for BASE SET of 3φn/pn applicable to a basis of (3φn/pn)ncn variable stem cycles cells

BASE SET of 3pnn

3(pn1/φn1)/(1φn1/pn1)=(0/0)=0

3(pn2/φn2)/(1φn2/pn2)=(3/0.^3)

3(pn3/φn3)/(1φn3/pn3)=(2.5/0.4)

3(pn4/φn4)/(1φn4/pn4)=(4/0.2^142857)


3(pn5/φn5)/(1φn5/pn5)=(6.875/1.^45

and 3(pn5/φn5c2)/(1φn5c2/pn5)=(6.6265060^24096084337349397590361445784337951712047/0.150^9)

and 3(pn5/φn5c2)/(1φn5/pn5)=(6.6265060^24096084337349397590361445784337951712047)/1.^45)

and 3(pn5/φn5)/(1φn5c2/pn5)=(6.875/0.150^9) of 3(pn5/φn5)/(1φn5/pn5) bases in c1 and c2


3(pn6/φn6)/(1φn6/pn6)=(8.125/0.1^230769)

3(pn7/φn7)/(1φn7/pn7)=(10.46150^76923/0.095^5882352941176470)

and so on . . . for BASE SET of 3pnn applicable to a basis of (3pnn)ncn variable stem cycles cells


BASE SET of 2φn/pn

2(1φn1/pn1)/(pn2/φn2) =(0/3)=0

2(1φn2/pn2)/(pn3/φn3) =(0.^3/2.5)

2(1φn3/pn3)/(pn4/φn4) =(0.4/4)

2(1φn4/pn4)/(pn5/φn5) =(0.2^142857/6.875)

and 2(1φn4/pn4)/(pn5/φn5c2) =(0.2^142857/6.6265060^24096084337349397590361445784337951712047

of 2(1φn4/pn4)/(pn5/φn5) bases to 2(1φn4/pn4)/(pn5/φn5c2)


2(1φn5/pn5)/(pn6/φn6) =(1.^45/8.125)

and 2(1φn5c2/pn5)/(pn6/φn6) =(0.150^9/8.125) of 2(1φn5/pn5)/(pn6/φn6) to 2(1φn5c2/pn5)/(pn6/φn6) bases


2(1φn6/pn6)/(pn7/φn7) =(0.1^230769/10.46150^76923)

and so on . . . for BASE SET of 2φn/pn applicable to a basis of (2φn/pn)ncn variable stem cycles cells


BASE SET of 2pn/φn

2(pn1/φn1)/(1φn2/pn2) =(0/0.^3)=0

2(pn2/φn2)/(1φn3/pn3) =(3/0.4)

2(pn3/φn3)/(1φn4/pn4) =(2.5/0.2^142857)


2(pn4/φn4)/(1φn5/pn5) =(4/1.^45

and 2(pn4/φn4)/(1φn5c2/pn5) =(4/0.150^9) of 2(pn4/φn4)/(1φn5/pn5) to 2(pn4/φn4)/(1φn5c2/pn5) bases


2(pn5/φn5)/(1φn6/pn6) =(6.875/0.1^230769)

and 2(pn5/φn5c2)/(1φn6/pn6) =(6.6265060^24096084337349397590361445784337951712047/0.1^230769

of 2(pn5/φn5)/(1φn6/pn6) to 2(pn5/φn5c2)/(1φn6/pn6) bases


2(pn6/φn6)/(1φn7/pn7) =(8.125/0.095^5882352941176470)


2(pn7/φn7)/(1φn8/pn8) =(10.46150^76923/0.079757^052631578421

and 2(pn7/φn7)/(1φn8c2/pn8) =(10.46150^76923/0.079757079757^052631578421)

 of 2(pn7/φn7)/(1φn8/pn8) to 2(pn7/φn7)/(1φn8c2/pn8) bases

and so on . . . for BASE SET of 2pn/φn applicable to a basis of (2pn/φn)ncn variable stem cycles cells


BASE SET of 1φn/pn

1(1φn2/pn2)/(pn1/φn1)=(0.^3/0)=0

1(1φn3/pn3)/(pn2/φn2)=(0.4/3)

1(1φn4/pn4)/(pn3/φn3)=(0.2^142857/2.5)

1(1φn5/pn5)/(pn4/φn4)=(1.^45/4)


1(1φn6/pn6)/(pn5/φn5)=(0.1^230769/6.875)

and 1(1φn6/pn6)/(pn5/φn5c2)=(0.1^230769/6.6265060^24096084337349397590361445784337951712047)

 of 1(1φn6/pn6)/(pn5/φn5) to 1(1φn6/pn6)/(pn5/φn5c2) bases


1(1φn7/pn7)/(pn6/φn6)=(0.095^5882352941176470/8.125)


1(1φn8/pn8)/(pn7/φn7)=(0.079757^052631578421/10.46150^76923)

and 1(1φn8c2/pn8)/(pn7/φn7)=(0.079757079757^052631578421/10.46150^76923)

of 1(1φn8/pn8)/(pn7/φn7) to 1(1φn8c2/pn8)/(pn7/φn7) bases

and so on . . . for BASE SET of 1φn/pn applicable to a basis of (1φn/pn)ncn variable stem cycles cells


BASE SET of 1pn/φn

1(pn2/φn2)/(1φn1/pn1)=(3/0)=0

1(pn3/φn3)/(1φn2/pn2)=(2.5/0.^3)

1(pn4/φn4)/(1φn3/pn3)=(4/0.4)


1(pn5/φn5)/(1φn4/pn4)=(6.875/0.2^142857)

and 1(pn5/φn5c2)/(1φn4/pn4)=(6.6265060^24096084337349397590361445784337951712047/0.2^142857)

 of 1(pn5/φn5)/(1φn4/pn4) to 1(pn5/φn5c2)/(1φn4/pn4) bases


1(pn6/φn6)/(1φn5/pn5)=(8.125/1.^45)

and 1(pn6/φn6)/(1φn5c2/pn5)=(8.125/0.150^9)

 of 1(pn6/φn6)/(1φn5/pn5) to 1(pn6/φn6)/(1φn5c2/pn5) bases


1(pn7/φn7)/(1φn6/pn6)=(10.46150^76923/0.1^230769)

and so on . . . for BASE SET of 1pn/φn applicable to a basis of (1pn/φn)ncn variable stem cycles cells

Ψ represents unique whole numbers that are not prime numbers nor are they fibonacci numbers

4 6 9 10 12 14 15 16 18 20 22 24 25 26 27 28 30 32 33 35 36 38 39 40 42 44 45 46 48 49 50 51 52 54 56 57 58 60 62 63 64 65 66 68 69 70 72 74 75 76 77 78 80 81 82 84 85 86 87 88 90 91 92 93 94 95 96 98 99 100 and so on . . .

These whole numbers are variables that are neither Y base fibonacci numerals nor are they prime numbers and yet these numbers are still factorable numerals of a set entirely different than Y, P, A through Z, φ, and Θ.

In this case we note the set as (N) of Ψ such that psi represents N whole numbers that are not prime nor fibonacci based numerals and are an ordinal set of consecutive values.

N then is a number and N represents any number of any set including numbers that can not be defined to any of these sets.

A  B  D  E  F  G  H  I  J  K  L  M  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇°  ∀

As C cycles of repeating ratios are numerable then cn or CN is a cycle count of N many cycle counts that its self can be whole and partial of...

1⅄Ψn1=(Ψn2n1)=(6/4)=1.5

2⅄Ψn1=(Ψn1n2)=(4/6)=0.^6

And path 3⅄ is applicable to variables of 1⅄Ψn and also applicable to variables of 2⅄Ψn to variable factor potential notated change of CN variants in ratios of 1⅄Ψn and 2⅄Ψ

Chevron ^ Bold numerals represent a repeating decimal number sequence stem that can be counted for cn as practical application ratio values infinitely to the limit of a finite factoring limit.

1⅄Ψn1=(Ψn2n1)=(6/4)=1.5

1⅄Ψn2=(Ψn3n2)=(9/6)=1.5

1⅄Ψn3=(Ψn4n3)=(10/9)=1.^1 or 1.1

1⅄Ψn4=(Ψn5n4)=(12/10)=1.2

1⅄Ψn5=(Ψn6n5)=(14/12)=1.1^6 or 1.16

1⅄Ψn6=(Ψn7n6)=(15/14)=1.0^714285 or 1.0714285

1⅄Ψn7=(Ψn8n7)=(16/15)=1.0^6 or 1.06

1⅄Ψn8=(Ψn9n8)=(18/16)=1.125

1⅄Ψn9=(Ψn10n9)=(20/18)=1.^1 or 1.1

1⅄Ψn10=(Ψn11n10)=(22/20)=1.1

1⅄Ψn11=(Ψn12n11)=(24/22)=1.^09 or 1.09

1⅄Ψn12=(Ψn13n12)=(25/24)=1.041^6 or 1.0416

1⅄Ψn13=(Ψn14n13)=(26/25)=1.04

1⅄Ψn14=(Ψn15n14)=(27/26)=1.0^384615 or 1.0384615

1⅄Ψn15=(Ψn16n15)=(28/27)=1.0^37 or 1.037

1⅄Ψn16=(Ψn17n16)=(30/28)=1.0^714285 or 1.0714285

1⅄Ψn17=(Ψn18n17)=(32/30)=1.0^6 or 1.06

1⅄Ψn18=(Ψn19n18)=(33/32)=1.03125

1⅄Ψn19=(Ψn20n19)=(35/33)=1.0^6 or 1.06

1⅄Ψn20=(Ψn21n20)=(36/35)=1.0^285714 or 1.0285714

1⅄Ψn21=(Ψn22n21)=(38/36)=1.0^5 or 1.05

1⅄Ψn22=(Ψn23n22)=(39/38)=1.0^263157894736842105263157894736842105 or 1.0263157894736842105263157894736842105

1⅄Ψn23=(Ψn24n23)=(40/39)=^1.02564 or 1.02564 or 1.02564102564

1⅄Ψn24=(Ψn25n24)=(42/40)=1.05

1⅄Ψn25=(Ψn26n25)=(44/42)=1.^047619 or 1.047619

1⅄Ψn26=(Ψn27n26)=(45/44)=1.02^27 or 1.0227

1⅄Ψn27=(Ψn28n27)=(46/45)=1.0^2 or 1.02

1⅄Ψn28=(Ψn29n28)=(48/46)=1.^0434782608695652173913 or 1.0434782608695652173913

1⅄Ψn29=(Ψn30n29)=(49/48)=1.0208^3 or 1.02083

1⅄Ψn30=(Ψn31n30)=(50/49)=^1.02040816326530612244897959183673469387755 or ^1.02040816326530612244897959183673469387755102040816326530612244897959183673469387755

1⅄Ψn31=(Ψn32n31)=(51/50)=1.02

1⅄Ψn32=(Ψn33n32)=(52/51)=1.^0196078431372549 or 1.0196078431372549

1⅄Ψn33=(Ψn34n33)=(54/52)=1.0^384615 or 1.0384615

1⅄Ψn34=(Ψn35n34)=(56/54)=1.^037 or 1.037

1⅄Ψn35=(Ψn36n35)=(57/56)=1.017^857142 or 1.017857142

1⅄Ψn36=(Ψn37n36)=(58/57)=1.^017543859649122807 or 1.017543859649122807

1⅄Ψn37=(Ψn38n37)=(60/58)=^1.034482758620689655172413793 or 1.034482758620689655172413793

1⅄Ψn38=(Ψn39n38)=(62/60)=1.0^3 or 1.03 or 1.033 or 1.0333

1⅄Ψn39=(Ψn40n39)=(63/62)=1.0^161290322580645 or 1.0161290322580645

1⅄Ψn40=(Ψn41n40)=(64/63)=1.^015873 or 1.015873

1⅄Ψn41=(Ψn42n41)=(65/64)=1.015625

1⅄Ψn42=(Ψn43n42)=(66/65)=1.0^153846 or 1.0153846

1⅄Ψn43=(Ψn44n43)=(68/66)=1.^03 or 1.03

1⅄Ψn44=(Ψn45n44)=(69/68)=1.01^4705882352941176 or 1.014705882352941176

1⅄Ψn45=(Ψn46n45)=(70/69)=^1.014492753623188405797 or 1.0144927536231884057971014492753623188405797

1⅄Ψn46=(Ψn47n46)=(72/70)=1.0^285714 or 1.0285714

1⅄Ψn47=(Ψn48n47)=(74/72)=1.02^7 or 1.027

1⅄Ψn48=(Ψn49n48)=(75/74)=1.0^135 or 1.0135

1⅄Ψn49=(Ψn50n49)=(76/75)=1.01^3 or 1.013

1⅄Ψn50=(Ψn51n50)=(77/76)=1.01^315789473684210526 or 1.01315789473684210526

1⅄Ψn51=(Ψn52n51)=(78/77)=1.^012987 or 1.012987

1⅄Ψn51=(Ψn53n52)=(80/78)=^1.02564 or 1.02564102564

1⅄Ψn53=(Ψn54n53)=(81/80)=1.0125

1⅄Ψn54=(Ψn55n54)=(82/81)=1.^012345679 or 1.012345679

1⅄Ψn55=(Ψn56n55)=(84/82)=1.^02439 or 1.02439

1⅄Ψn56=(Ψn57n56)=(85/84)=1.01^190476 or 1.01190476

1⅄Ψn57=(Ψn58n57)=(86/85)=1.0^1176470588235294 or 1.0^1176470588235294

1⅄Ψn58=(Ψn59n58)=(87/86)=1.0^116279069767441860465 or 1.0116279069767441860465

1⅄Ψn59=(Ψn60n59)=(88/87)=1.^0114942528735632183908045977 or 1.0114942528735632183908045977

1⅄Ψn60=(Ψn61n60)=(90/88)=1.02^27 or 1.0227

1⅄Ψn61=(Ψn62n61)=(91/90)=1.0^1 or 1.01 or 1.011 or 1.0111

1⅄Ψn62=(Ψn63n62)=(92/91)=1.^010989 or 1.010989

1⅄Ψn63=(Ψn64n63)=(93/92)=1.01^0869565217391304347826 or 1.010869565217391304347826

1⅄Ψn64=(Ψn65n64)=(94/93)=1.^010752688172043 or 1.010752688172043

1⅄Ψn65=(Ψn66n65)=(95/94)=1.0^1063829787234042553191489361702127659574468085 or 1.01063829787234042553191489361702127659574468085

1⅄Ψn66=(Ψn67n66)=(96/95)=1.0^105263157894736842 or 1.0105263157894736842

1⅄Ψn67=(Ψn68n67)=(98/96)=1.0208^3 or 1.02083

1⅄Ψn68=(Ψn69n68)=(99/98)=1.0^102040816326530612244897959183673469387755 or 1.0102040816326530612244897959183673469387755

1⅄Ψn69=(Ψn70n69)=(100/99)=1.^01 or 1.01 or 1.0101 or 1.010101

and so on for variables of 1⅄Ψn

Then 

2⅄Ψn1=(Ψn1n2)=(4/6)=0.^6 or 0.6

2⅄Ψn2=(Ψn2n3)=(6/9)=0.^6 or 0.6

2⅄Ψn3=(Ψn3n4)=(9/10)=0.9

2⅄Ψn4=(Ψn4n5)=(10/12)=0.8^3 or 0.83

2⅄Ψn5=(Ψn5n6)=(12/14)=0.^857142 or 0.857142

2⅄Ψn6=(Ψn6n7)=(14/15)=0.9^3 or 0.93

2⅄Ψn7=(Ψn7n8)=(15/16)=0.9375

2⅄Ψn8=(Ψn8n9)=(16/18)=0.^8 or 0.8

2⅄Ψn9=(Ψn9n10)=(18/20)=0.9

2⅄Ψn10=(Ψn10n11)=(20/22)=0.9^09 or 0.909

2⅄Ψn11=(Ψn11n12)=(22/24)=0.91^6 or 0.916

2⅄Ψn12=(Ψn12n13)=(24/25)=0.96

2⅄Ψn13=(Ψn13n14)=(25/26)=0.9^615384 or 0.9615384

2⅄Ψn14=(Ψn14n15)=(26/27)=0.^962 or 0.962

2⅄Ψn15=(Ψn15n16)=(27/28)=0.96^428571 or 0.96428571

2⅄Ψn16=(Ψn16n17)=(28/30)=0.9^3 or 0.93

2⅄Ψn17=(Ψn17n18)=(30/32)=0.9375

2⅄Ψn18=(Ψn18n19)=(32/33)=0.^96 or 0.96

2⅄Ψn19=(Ψn19n20)=(33/35)=0.9^428571 or 0.9428571

2⅄Ψn20=(Ψn20n21)=(35/36)=0.97^2 or 0.972

and so on for variables of 2⅄Ψn


Then

12Ψn1 of 1⅄Ψn=(1⅄Ψn2/1⅄Ψn1)=(1.5/1.5)=1

12Ψn2 of 1⅄Ψn=(1⅄Ψn3/1⅄Ψn2)=(1.1/1.5)=0.7^3 or 0.73 and 12Ψn2 of 1⅄Ψn=(1⅄Ψn3c2/1⅄Ψn2)=(1.11/1.5)=0.74 and 12Ψn2 of 1⅄Ψn=(1⅄Ψn3c3/1⅄Ψn2)=(1.111/1.5)=0.740^6 or 0.7406 and so on for cn variable of 12Ψn2 of 1⅄Ψn

12Ψn3 of 1⅄Ψn=(1⅄Ψn4/1⅄Ψn3)=(1.2/1.1)=1.^09 or 1.09

12Ψn4 of 1⅄Ψn=(1⅄Ψn5/1⅄Ψn4)=(1.16/1.2)=0.9^6 or 0.96

12Ψn5 of 1⅄Ψn=(1⅄Ψn6/1⅄Ψn5)=(1.0714285/1.16)=0.9236452^58620689655172413793103448275862068965517241379310344827

or

0.923645258620689655172413793103448275862068965517241379310344827

12Ψn6 of 1⅄Ψn=(1⅄Ψn7/1⅄Ψn6)=(1.06/1.0714285)

12Ψn7 of 1⅄Ψn=(1⅄Ψn8/1⅄Ψn7)=(1.125/1.06)

12Ψn8 of 1⅄Ψn=(1⅄Ψn9/1⅄Ψn8)=(1.1/1.125)

12Ψn9 of 1⅄Ψn=(1⅄Ψn10/1⅄Ψn9)=(1.1/1.1)

12Ψn10 of 1⅄Ψn=(1⅄Ψn11/1⅄Ψn10)=(1.09/1.1)

12Ψn11 of 1⅄Ψn=(1⅄Ψn12/1⅄Ψn11)=(1.0416/1.09)

12Ψn12 of 1⅄Ψn=(1⅄Ψn13/1⅄Ψn12)=(1.04/1.0416)

12Ψn13 of 1⅄Ψn=(1⅄Ψn14/1⅄Ψn13)=(1.0384615/1.04)

12Ψn14 of 1⅄Ψn=(1⅄Ψn15/1⅄Ψn14)=(1.037/1.0384615)

12Ψn15 of 1⅄Ψn=(1⅄Ψn16/1⅄Ψn15)=(1.0714285/1.037)

12Ψn16 of 1⅄Ψn=(1⅄Ψn17/1⅄Ψn16)=(1.06/1.0714285)

12Ψn17 of 1⅄Ψn=(1⅄Ψn18/1⅄Ψn17)=(1.03125/1.06)

12Ψn18 of 1⅄Ψn=(1⅄Ψn19/1⅄Ψn18)=(1.06/1.03125)

12Ψn19 of 1⅄Ψn=(1⅄Ψn20/1⅄Ψn19)=(1.0285714/1.06)

and so on for c1 of cn variables factoring for 12Ψn of 1⅄Ψn from Ψ base numerals.


Then

22Ψn1 of 1⅄Ψn=(1⅄Ψn1/1⅄Ψn2)=(1.5/1.5)=1

22Ψn2 of 1⅄Ψn=(1⅄Ψn2/1⅄Ψn3)=(1.5/1.1)=1.^36 or 1.36

22Ψn3 of 1⅄Ψn=(1⅄Ψn3/1⅄Ψn4)=(1.1/1.2)=0.91^6 or 0.916

22Ψn4 of 1⅄Ψn=(1⅄Ψn4/1⅄Ψn5)=(1.2/1.16)=^1.034482758620689655172413793 or 1.0344827586206896551724137931034482758620689655172413793

22Ψn5 of 1⅄Ψn=(1⅄Ψn5/1⅄Ψn6)=(1.16/1.0714285)

22Ψn6 of 1⅄Ψn=(1⅄Ψn6/1⅄Ψn7)=(1.0714285/1.06)

22Ψn7 of 1⅄Ψn=(1⅄Ψn7/1⅄Ψn8)=(1.06/1.125)

22Ψn8 of 1⅄Ψn=(1⅄Ψn8/1⅄Ψn9)=(1.125/1.1)

22Ψn9 of 1⅄Ψn=(1⅄Ψn9/1⅄Ψn10)=(1.1/1.1)

22Ψn10 of 1⅄Ψn=(1⅄Ψn10/1⅄Ψn11)=(1.1/1.09)

22Ψn11 of 1⅄Ψn=(1⅄Ψn11/1⅄Ψn12)=(1.09/1.0416)

22Ψn12 of 1⅄Ψn=(1⅄Ψn12/1⅄Ψn13)=(1.0416/1.04)

22Ψn13 of 1⅄Ψn=(1⅄Ψn13/1⅄Ψn14)=(1.04/1.0384615)

22Ψn14 of 1⅄Ψn=(1⅄Ψn14/1⅄Ψn15)=(1.0384615/1.037)

22Ψn15 of 1⅄Ψn=(1⅄Ψn15/1⅄Ψn16)=(1.037/1.0714285)

22Ψn16 of 1⅄Ψn=(1⅄Ψn16/1⅄Ψn17)=(1.0714285/1.06)

22Ψn17 of 1⅄Ψn=(1⅄Ψn17/1⅄Ψn18)=(1.06/1.03125)

22Ψn18 of 1⅄Ψn=(1⅄Ψn18/1⅄Ψn19)=(1.03125/1.06)

22Ψn19 of 1⅄Ψn=(1⅄Ψn19/1⅄Ψn20)=(1.06/1.0285714)

and so on for c1 of cn variables factoring for 22Ψn of 1⅄Ψn from Ψ base numerals.


Then

12Ψn1 of 2⅄Ψn=(2⅄Ψn2/2⅄Ψn1)=(0.6/0.6)=1

12Ψn2 of 2⅄Ψn=(2⅄Ψn3/2⅄Ψn2)=(0.9/0.6)=1.5

12Ψn3 of 2⅄Ψn=(2⅄Ψn4/2⅄Ψn3)=(0.83/0.9)=0.9^2 or 0.92

12Ψn4 of 2⅄Ψn=(2⅄Ψn5/2⅄Ψn4)=(0.857142/0.83)=1.0327^01204819277108433734939759036144578313253 or 1.032701204819277108433734939759036144578313253

12Ψn5 of 2⅄Ψn=(2⅄Ψn6/2⅄Ψn5)=(0.93/0.857142)=^1.08500 or 1.08500108500

12Ψn6 of 2⅄Ψn=(2⅄Ψn7/2⅄Ψn6)=(0.9375/0.93)=1.00^806451612903225 or 1.00806451612903225

12Ψn7 of 2⅄Ψn=(2⅄Ψn8/2⅄Ψn7)=(0.8/0.9375)

12Ψn8 of 2⅄Ψn=(2⅄Ψn9/2⅄Ψn8)=(0.9/0.8)

12Ψn9 of 2⅄Ψn=(2⅄Ψn10/2⅄Ψn9)=(0.909/0.9)

12Ψn10 of 2⅄Ψn=(2⅄Ψn11/2⅄Ψn10)=(0.916/0.909)

12Ψn11 of 2⅄Ψn=(2⅄Ψn12/2⅄Ψn11)=(0.96/0.916)

12Ψn12 of 2⅄Ψn=(2⅄Ψn13/2⅄Ψn12)=(0.9615384/0.96)

12Ψn13 of 2⅄Ψn=(2⅄Ψn14/2⅄Ψn13)=(0.962/0.9615384)

12Ψn14 of 2⅄Ψn=(2⅄Ψn15/2⅄Ψn14)=(0.96428571/0.962)

12Ψn15 of 2⅄Ψn=(2⅄Ψn16/2⅄Ψn15)=(0.93/0.96428571)

12Ψn16 of 2⅄Ψn=(2⅄Ψn17/2⅄Ψn16)=(0.9375/0.93)

12Ψn17 of 2⅄Ψn=(2⅄Ψn18/2⅄Ψn17)=(0.96/0.9375)

12Ψn18 of 2⅄Ψn=(2⅄Ψn19/2⅄Ψn18)=(0.9428571/0.96)

12Ψn19 of 2⅄Ψn=(2⅄Ψn20/2⅄Ψn19)=(0.972/0.9428571)

and so on for c1 of cn variables factoring for 12Ψn of 2⅄Ψn from Ψ base numerals.


while

22Ψn1 of 2⅄Ψn=(2⅄Ψn1/2⅄Ψn2)=(0.6/0.6)=1

22Ψn2 of 2⅄Ψn=(2⅄Ψn2/2⅄Ψn3)=(0.6/0.9)=0.^6 or 0.6

22Ψn3 of 2⅄Ψn=(2⅄Ψn3/2⅄Ψn4)=(0.9/0.83)=^1.0843373493975903614457831325301204819277 or 1.084337349397590361445783132530120481927710843373493975903614457831325301204819277

22Ψn4 of 2⅄Ψn=(2⅄Ψn4/2⅄Ψn5)=(0.83/0.857142)=^0.96833430166763500 or 0.96833430166763500096833430166763500

22Ψn5 of 2⅄Ψn=(2⅄Ψn5/2⅄Ψn6)=(0.857142/0.93)=0.92165^806451612903225 or 0.92165806451612903225

22Ψn6 of 2⅄Ψn=(2⅄Ψn6/2⅄Ψn7)=(0.93/0.9375)=0.992

22Ψn7 of 2⅄Ψn=(2⅄Ψn7/2⅄Ψn8)=(0.9375/0.8)

22Ψn8 of 2⅄Ψn=(2⅄Ψn8/2⅄Ψn9)=(0.8/0.9)

22Ψn9 of 2⅄Ψn=(2⅄Ψn9/2⅄Ψn10)=(0.9/0.909)

22Ψn10 of 2⅄Ψn=(2⅄Ψn10/2⅄Ψn11)=(0.909/0.916)

22Ψn11 of 2⅄Ψn=(2⅄Ψn11/2⅄Ψn12)=(0.916/0.96)

22Ψn12 of 2⅄Ψn=(2⅄Ψn12/2⅄Ψn13)=(0.96/0.9615384)

22Ψn13 of 2⅄Ψn=(2⅄Ψn13/2⅄Ψn14)=(0.9615384/0.962)

22Ψn14 of 2⅄Ψn=(2⅄Ψn14/2⅄Ψn15)=(0.962/0.96428571)

22Ψn15 of 2⅄Ψn=(2⅄Ψn15/2⅄Ψn16)=(0.96428571/0.93)

22Ψn16 of 2⅄Ψn=(2⅄Ψn16/2⅄Ψn17)=(0.93/0.9375)

22Ψn17 of 2⅄Ψn=(2⅄Ψn17/2⅄Ψn18)=(0.9375/0.96)

22Ψn18 of 2⅄Ψn=(2⅄Ψn18/2⅄Ψn19)=(0.96/0.9428571)

22Ψn19 of 2⅄Ψn=(2⅄Ψn19/2⅄Ψn20)=(0.9428571/0.972)

and so on for c1 of cn variables factoring for 22Ψn of 2⅄Ψn from Ψ base numerals.



So from set Ψ psi base of paths 1⅄ and 2⅄ we have base sets of variables

Ψ

1⅄Ψn

2⅄Ψn

1⅄ of 1⅄Ψn

1⅄ of 2⅄Ψn

2⅄ of 1⅄Ψn

2⅄ of 2⅄Ψn

and

3⅄Ψn applicable as a path of factoring to variables from sets

1⅄Ψn

2⅄Ψn

1⅄ of 1⅄Ψn

1⅄ of 2⅄Ψn

2⅄ of 1⅄Ψn

2⅄ of 2⅄Ψn

and so on for variable factors of cn to set bases 1⅄Ψn and 2⅄Ψn


As these N for number symbols represent numbers then for numbers 0 through 11 are

Y, Y, Y&P, Y&P, Ψ, Y&P, Ψ, P, Y, Ψ, Ψ, P

0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11

Yn1, Yn2, Yn3&Pn1, Yn4&Pn2, Ψn1, Yn5&Pn3, Ψn2, Pn4, Yn6, Ψn3, Ψn4, Pn5

and so on for sets Y, P, Ψ of whole numbers bases definable and variables in quantum field fractal polarization math.


So then as these variables from sets are definable and numerable as consecutive values, then the numbers are as well applicable to other math functions. Path Functions  ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄  of set Ψ variables applied with variable sets A  B  D  E  F  G  H  I  J  K  L  M  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  Ψ for complex numerals ᐱ  ᗑ  ∘⧊°  ∘∇° 


if ncn=(⅄nncn)(ncn) then Ψncn=(⅄Ψncn)(ncn) is a a multiple exponent variable dependent on the definition of path set variable cn of Ψn if it is not a base set variable of Ψ.


if 1X⅄=(n2xn1) then

n⅄Xᐱ(ΨnxAn), ∈n⅄Xᐱ(ΨnxBn), ∈n⅄Xᐱ(ΨnxDn), ∈n⅄Xᐱ(ΨnxEn), ∈n⅄Xᐱ(ΨnxFn), ∈n⅄Xᐱ(ΨnxGn), ∈n⅄Xᐱ(ΨnxHn), ∈n⅄Xᐱ(ΨnxIn), ∈n⅄Xᐱ(ΨnxJn), ∈n⅄Xᐱ(ΨnxKn), ∈n⅄Xᐱ(ΨnxLn), ∈n⅄Xᐱ(ΨnxMn), ∈n⅄Xᐱ(ΨnxNn), ∈n⅄Xᐱ(ΨnxOn), ∈n⅄Xᐱ(ΨnxPn), ∈n⅄Xᐱ(ΨnxQn), ∈n⅄Xᐱ(ΨnxRn), ∈n⅄Xᐱ(ΨnxSn), ∈n⅄Xᐱ(ΨnxTn),∈n⅄Xᐱ(ΨnxUn),  ∈n⅄Xᐱ(ΨnxVn), ∈n⅄Xᐱ(ΨnxWn), ∈n⅄Xᐱ(ΨnxYn), ∈n⅄Xᐱ(ΨnxZn), ∈n⅄Xᐱ(Ψnn), ∈n⅄Xᐱ(Ψnn), n⅄Xᐱ(ΨncnxΨncn), ∈n⅄Xᐱ(Ψncnxᐱncn), ∈n⅄Xᐱ(Ψncnxᗑncn), ∈n⅄Xᐱ(Ψncnx∘⧊°ncn), ∈n⅄Xᐱ(Ψncnx∘∇°ncn)


if +⅄=(nncn+nncn) then

n+⅄ᐱ(Ψn+An), ∈n+⅄ᐱ(Ψn+Bn), ∈n+⅄ᐱ(Ψn+Dn), ∈n+⅄ᐱ(Ψn+En), ∈n+⅄ᐱ(Ψn+Fn), ∈n+⅄ᐱ(Ψn+Gn), ∈n+⅄ᐱ(Ψn+Hn), ∈n+⅄ᐱ(Ψn+In), ∈n+⅄ᐱ(Ψn+Jn), ∈n+⅄ᐱ(Ψn+Kn), ∈n+⅄ᐱ(Ψn+Ln), ∈n+⅄ᐱ(Ψn+Mn), ∈n+⅄ᐱ(Ψn+Nn), ∈n+⅄ᐱ(Ψn+On), ∈n+⅄ᐱ(Ψn+Pn), ∈n+⅄ᐱ(Ψn+Qn), ∈n+⅄ᐱ(Ψn+Rn), ∈n+⅄ᐱ(Ψn+Sn), ∈n+⅄ᐱ(Ψn+Tn),∈n+⅄ᐱ(Ψn+Un),  ∈n+⅄ᐱ(Ψn+Vn), ∈n+⅄ᐱ(Ψn+Wn), ∈n+⅄ᐱ(Ψn+Yn), ∈n+⅄ᐱ(Ψn+Zn), ∈n+⅄ᐱ(Ψnn), ∈n+⅄ᐱ(Ψnn),  ∈n+⅄ᐱ(Ψn+Ψn), ∈n+⅄ᐱ(Ψncn+ᐱncn), ∈n+⅄ᐱ(Ψncn+ᗑncn), ∈n+⅄ᐱ(Ψncn+∘⧊°ncn), ∈n+⅄ᐱ(Ψncn+∘∇°ncn)


if 1-⅄=(n2-n1) then

1-⅄ᐱ(Ψn2-An1), ∈1-⅄ᐱ(Ψn2-Bn1), ∈1-⅄ᐱ(Ψn2-Dn1), ∈1-⅄ᐱ(Ψn2-En1), ∈1-⅄ᐱ(Ψn2-Fn1), ∈1-⅄ᐱ(Ψn2-Gn1), ∈1-⅄ᐱ(Ψn2-Hn1), ∈1-⅄ᐱ(Ψn2-In1), ∈1-⅄ᐱ(Ψn2-Jn1), ∈1-⅄ᐱ(Ψn2-Kn1), ∈1-⅄ᐱ(Ψn2-Ln1), ∈1-⅄ᐱ(Ψn2-Mn1), ∈1-⅄ᐱ(Ψn2-Nn1), ∈1-⅄ᐱ(Ψn2-On1), ∈1-⅄ᐱ(Ψn2-Pn1), ∈1-⅄ᐱ(Ψn2-Qn1), ∈1-⅄ᐱ(Ψn2-Rn1), ∈1-⅄ᐱ(Ψn2-Sn1), ∈1-⅄ᐱ(Ψn2-Tn1),∈1-⅄ᐱ(Ψn2-Un1),  ∈1-⅄ᐱ(Ψn2-Vn1), ∈1-⅄ᐱ(Ψn2-Wn1), ∈1-⅄ᐱ(Ψn2-Yn1), ∈1-⅄ᐱ(Ψn2-Zn1), ∈1-⅄ᐱ(Ψn2n1), ∈1-⅄ᐱ(Ψn2n1),1-⅄ᐱ(Ψn2-Ψn1), ∈1-ᐱ(Ψn2cn-n1cn), ∈1-ᐱ(Ψn2cn-n1cn), ∈1-ᐱ(Ψn2cn-∘⧊°n1cn), ∈1-ᐱ(Ψn2cn-∘∇°n1cn)


if 2-⅄=(n1-n2) then

2-⅄ᐱ(Ψn1-An2), ∈2-⅄ᐱ(Ψn1-Bn2), ∈2-⅄ᐱ(Ψn1-Dn2), ∈2-⅄ᐱ(Ψn1-En2), ∈2-⅄ᐱ(Ψn1-Fn2), ∈2-⅄ᐱ(Ψn1-Gn2), ∈2-⅄ᐱ(Ψn1-Hn2), ∈2-⅄ᐱ(Ψn1-In2), ∈2-⅄ᐱ(Ψn1-Jn2), ∈2-⅄ᐱ(Ψn1-Kn2), ∈2-⅄ᐱ(Ψn1-Ln2), ∈2-⅄ᐱ(Ψn1-Mn2), ∈2-⅄ᐱ(Ψn1-Nn2), ∈2-⅄ᐱ(Ψn1-On2), ∈2-⅄ᐱ(Ψn1-Pn2), ∈2-⅄ᐱ(Ψn1-Qn2), ∈2-⅄ᐱ(Ψn1-Rn2), ∈2-⅄ᐱ(Ψn1-Sn2), ∈2-⅄ᐱ(Ψn1-Tn2),∈2-⅄ᐱ(Ψn1-Un2),  ∈2-⅄ᐱ(Ψn1-Vn2), ∈2-⅄ᐱ(Ψn1-Wn2), ∈2-⅄ᐱ(Ψn1-Yn2), ∈2-⅄ᐱ(Ψn1-Zn2), ∈2-⅄ᐱ(Ψn1-φn2), ∈2-⅄ᐱ(Ψn1-Θn2),2-⅄ᐱ(Ψn1-Ψn2), ∈2-ᐱ(Ψn1cn-n2cn), ∈2-ᐱ(Ψn1cn-n2cn), ∈2-ᐱ(Ψn1cn-∘⧊°n2cn), ∈2-ᐱ(Ψn1cn-∘∇°n2cn)


and if 3-⅄=(nncn-nncn) then the cn factor difference is critical to the precision value of that path function subtraction difference for any 3-⅄=(Ψncn-⅄Ψncn) variables just as the cn variable factor is crucial for path set division function 3=(Ψncn/⅄Ψncn) when pertaining to variables of path psi 1Ψ and 2Ψ rather than base Ψ variable whole numbers. The cn factor is important for accurate addition function equations where a cn factor is applicable as well with addition path psi 1Ψncn and 2Ψncn


ᐱ∀Ψ complex for all for any equations of psi specific numerals can then be factored to a library of psi Ψ and many paths the variables can be quantified with.

Similar term base numerals and path difference mid phase variables later related in equations

For simplicity a few base variables will be used here to explain paths of similar terms and variables expressed from the similar terms that become quadratic equations with decimal number variables in further terms from the same numeral sequences explained. a simple error can cause extreme inaccuracy with this simple logic factored incorrectly.

From Y and P limit to ten digits 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229 : 433494437 are common factors.

Phi Theta Θ   φ Q scale set paths and functions of cn stem cycle cell groups from y and p bases

123ncn|Θ/Y|ncn    123ncn|Y/Θ|ncn   123ncn|YxΘ|ncn    123ncn|Y+Θ|ncn    123ncn|Y-Θ|ncn    123ncn|Θ-Y|ncn 

123ncn|Θ/φ|ncn   123ncn|φ/Θ|ncn   123ncn|φxΘ|ncn   123ncn|φ+Θ|ncn   123ncn|φ-Θ|ncn   123ncn|φ-Θ|ncn 

123ncn|Θ/P|ncn    123ncn|P/Θ|ncn   123ncn|PxΘ|ncn    123ncn|P+Θ|ncn    123ncn|P-Θ|ncn    123ncn|Θ-P|ncn 

123ncn|Θ/Q|ncn   123ncn|Q/Θ|ncn   123ncn|QxΘ|ncn   123ncn|Q+Θ|ncn   123ncn|Q-Θ|ncn   123ncn|Θ-Q|ncn 

Phi Prime Theta Ratio sets of y p base variables

123ncn|A/Θn|ncn     123ncnn/A|ncn 

123ncn|Mn|ncn   123ncnn/M|ncn 

123ncn|V/Θn|ncn     123ncnn/V|ncn 

123ncn|W/Θn|ncn   123ncnn/W|ncn 

123ncn|n|ncn    123ncnn/|ncn 

123ncn|n|ncn    123ncnn/|ncn 

Using the ratios of common factors is one example of points given a value equal at Y and P base and those points with values being sent out to paths of division functions of φ, Θ, 1Q, and 2Q and even more paths when concerning A, M, V, W, E, F, I, H, or combination paths of these mentioned variables noted.

The variables created in differing paths of the points given the same value such as 2 : 3 : 5 : 13 : 89 are in ratios of φ, Θ, 1Q, and 2Q. As long as proper notation library and record of the newer variables rooted to the common factors are maintained, complete able cycles of systems that involve these valued points divided then have a system of decimal stem cycle variants that are able to work as though clockwork to simple ten base numbers.

2 and 3 for example produce quotient partial deriving to 1φn4 and 12φn3 and 12φn4 and 13φn2 and 13φn3 and 14φn1 and 14φn2 and 14φn3 and 15φn1 and 15φn2 and 16φn1 and 22φn3 and 22φn4 and 1Θn4 and 12Θn3 and 12Θn4 and 22Θn3 and 22Θn4 and 32Θn4 and 21Qn1 and 11Qn1 and many more. When these ratios derive from 2 and 3 and then belong to a system that is measured in cycles of decimals, these few numbers are a basic numeral representation of orbits and cycles of a field array stemmed to points that were plotted initially with values 2 and 3. Among the systems are particles mixed of the values 3 and 3 now divided between the system points until that system is made to stop.

An equation such as (12Θn4/15φn2)x(11Qn1/21Qn1 )+(21Qn1 /12φn3)-(/22φn4) should not then be limited to a calculator that can only factor to a ten digit decimal limit and actually depends on the stem cycle variable cn that must be defined in each variable of more extensive degrees in numeral digit precision lengths or that system will surely collapse when the factoring precision is lost in something such as chemistry of fuel types in nuclear energy. This is simply a random expression of terms based on Y P φ Θ Q of common factors 2 and 3 that if in practical application an extraction is made of an assumed value 2 and/or 3 at the wrong time in an extremely volatile state of that system will create a balance of a collapsing system being taken from that was started and is not complete enough to take 2 and/or 3 from. A similar disruption of a system by removing just one digit 1 anywhere in the wrong place at the wrong time of division remainders or adding 1 or 0.0000001 will corrupt that system balance and cause a catastrophric numerical chaotic failure to the simple systems of 2 and 3. 

Phi Prime Radical base array sets

AGAIN TO ADVANCE FURTHER IN THIS PHI PRIME RATIO SCALE WILL REQUIRE PHI RATIOS PAST φn21 that infact extends the decimal length and precision of what is called the GOLDEN RATIO if one chooses to factor variable past the noted numeral base y and or p of φ and Q.

AM and VW paths in wave functions of cycle variants 1⅄, 2⅄, 3

A=∈1/Q)cn and path ⅄ of Q is a variant in the definition of A

M=2/Q)cn and path ⅄ of Q is a variant in the definition of M

V= 1(Q/φ)cn and path ⅄ of Q is a variant in the definition of V

W=2(Q/φ)cn and path ⅄ of Q is a variant in the definition of W

that 3⅄A, 3⅄M, 3⅄V, 3⅄W vary from 

3⅄A of A=∈1/Q)cn and path ⅄ of Q is a variant in the definition of A

3⅄M of M=2/Q)cn and path ⅄ of Q is a variant in the definition of M

3⅄V of V= 1(Q/φ)cn and path ⅄ of Q is a variant in the definition of V

3⅄W of W=2(Q/φ)cn and path ⅄ of Q is a variant in the definition of W

Given A=∈1/Q)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so 

A=∈1n2/1Qn1)cn 

and 

A=∈1n2/2Qn1)cn

then

An1 of 1n2/1Qn1)=(1/1.5)=0.^6

An2 of 1n3/1Qn2)=(2/1.^6)=1.25 and An2 of 1n3/1Qn2c2)=(2/1.^66)=^1.2048192771084337349397590361445783132530

An3 of 1n4/1Qn3)=(1.5/1.4)=1.0^714285

An4 of 1n5/1Qn4)=(1.^6/1.^571428) and An4 of 1n5c2/1Qn4)=(1.^66/1.^571428) and An4 of 1n5/1Qn4)=(1.^6/1.^571428571428) and An4 of 1n5/1Qn4)=(1.^66/1.^571428571428) and so on for cn variant of An4 of 1n5/1Qn4)

An5 of 1n6/1Qn5)=(1.6/1.^18)=^0.988875154511742892459826946847960444993819530284301606922126081582200247218788627935723114956736711990111248454882571075401730531520395550061804697156983930778739184177997527812113720642768850432632880

An6 of 1n7/1Qn6)=(1.625/1.^307692)

An7 of 1n8/1Qn7)=(1.^615384/1.^1176470588235294)

An8 of 1n9/1Qn8)=(1.^619047/1.^210526315789473684)

An9 of 1n10/1Qn9)=(1.6^1762941/1.^268695652173913043478)

An10 of 1n11/1Qn10)=(1.6^18/1.^0689655172413793103448275862)

An11 of 1n12/1Qn11)=(1.^61797752808988764044943820224719101123595505/1.^193548387096774)

An12 of 1n13/1Qn12)=(1.6180^5/1.^108)

An13 of 1n14/1Qn13)=(1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/1.^04878)

An14 of 1n15/1Qn14)=(1.6183^0223896551724135014/1.^093023255813953488372)

An15 of 1n16/1Qn15)=(1.618^032786885245901639344262295081967213114754098360655737704918/1.^12765957446808510638297872340425531914893610702)

An16 of 1n17/1Qn16)=(1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843/1.^1132075471698)

An17 of 1n18/1Qn17)=(1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.^0338983050847457627118644067796610169491525423728813559322)

An18 of 1n19/1Qn18)=(1.6180340557314241486068^11145510835913312693/1.^098360655737704918032786885245901639344262295081967213114754)

An19 of 1n20/1Qn19)=(1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.^059701492537313432835820895522388)

An20 of 1n21/1Qn20)=(1.6^1803399852/1.^02816901408450704225352112676056338)

An21 of 1n22/1Qn21)=(1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/1.^08219178)

An22 of 1n23/1Qn22)=(1.6180339901755970865563773925808819377787815481903901530122522725989498052058043024109310597932923042177178024956241883575179831742984585850601321212805601038902377053814013889673084523742307040822087^96792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869/1.^0506329113924) and so on for variables of cn to set variables beyond An22 of 1n23/1Qn22) of ∈An of n2/1Qn1)cn 

so if A=∈1n2/1Qn1)cn 

and 

A=∈1n2/2Qn1)cn

then

An1 of 1n2/2Qn1)=(1/0.^6)

An2 of 1n3/2Qn2)=(2/0.6)

An3 of 1n4/2Qn3)=(1.5/0.^714285)

An4 of 1n5/2Qn4)=(1.^6/0.^63)

An5 of 1n6/2Qn5)=(1.6/0.^846153)

An6 of 1n7/2Qn6)=(1.625/0.^7647058823529411)

An7 of 1n8/2Qn7)=(1.^615384/0.^894736842105263157)

An8 of 1n9/2Qn8)=(1.^619047/0.^8260869565217391304347)


An ultimate and eventual equation of A variable set then includes a function such as An1 of 1(2φn2/2Qn1) or 

An1 of 1(3φn2/3Qn1) such that Q is a variable of further division tier paths of Q divided by Q ratios just as phi  ratios are potential to definitions and variables. Then on to further complex functions of A of (φ/J), A of (φ/K), A of (φ/L), and A of (φ/U) are definable to variable set ∈A


Functions then X, +⅄, and -⅄ of set A variables φn/1Qn and φn/2Qn replaced where functions of division paths 1⅄,  2⅄, and 3⅄ formulate  A of X(φnx1Qn),  A of X(φnx2Qn),   A of +⅄(φnx+1Qn),  A of +⅄(φn+2Qn),   A of -⅄(φn-1Qn), and A of -⅄(φn-2Qn) so then

if A of X(φnx1Qn) and  A of X(φnx2Qn) then

An1 of Xn2x1Qn1)=(1x1.5)

An2 of Xn3x1Qn2)=(2x1.^6)

An3 of Xn4x1Qn3)=(1.5x1.4)

An4 of Xn5x1Qn4)=(1.^6x1.^571428)

An5 of Xn6x1Qn5)=(1.6x1.^18)

An6 of Xn7x1Qn6)=(1.625x1.^307692)

An7 of Xn8x1Qn7)=(1.^615384x1.^1176470588235294)

An8 of Xn9x1Qn8)=(1.^619047x1.^210526315789473684)

so if A of Xn2x1Qn1)cn 

and 

A of Xn2x2Qn1)cn

then

An1 of Xn2x2Qn1)=(1x0.^6)

An2 of Xn3x2Qn2)=(2x0.6)

An3 of Xn4x2Qn3)=(1.5x0.^714285)

An4 of Xn5x2Qn4)=(1.^6x0.^63)

An5 of Xn6x2Qn5)=(1.6x0.^846153)

An6 of Xn7x2Qn6)=(1.625x0.^7647058823529411)

An7 of Xn8x2Qn7)=(1.^615384x0.^894736842105263157)

An8 of Xn9x2Qn8)=(1.^619047x0.^8260869565217391304347)

AND IF A of +⅄(φnx+1Qn) then A of +⅄(φn+2Qn)then 

An1 of +⅄n2+1Qn1)=(1+1.5)

An2 of +⅄n3+1Qn2)=(2+1.^6)

An3 of +⅄n4+1Qn3)=(1.5+1.4)

An4 of +⅄n5+1Qn4)=(1.^6+1.^571428)

An5 of +⅄n6+1Qn5)=(1.6+1.^18)

An6 of +⅄n7+1Qn6)=(1.625+1.^307692)

An7 of +⅄n8+1Qn7)=(1.^615384+1.^1176470588235294)

An8 of +⅄n9+1Qn8)=(1.^619047+1.^210526315789473684)

so if A of +⅄n2+1Qn1)cn 

and 

A of +⅄n2+2Qn1)cn

then

An1 of +⅄n2+2Qn1)=(1+0.^6)

An2 of +⅄n3+2Qn2)=(2+0.6)

An3 of +⅄n4+2Qn3)=(1.5+0.^714285)

An4 of +⅄n5+2Qn4)=(1.^6+0.^63)

An5 of +⅄n6+2Qn5)=(1.6+0.^846153)

An6 of +⅄n7+2Qn6)=(1.625+0.^7647058823529411)

An7 of +⅄n8+2Qn7)=(1.^615384+0.^894736842105263157)

An8 of +⅄n9+2Qn8)=(1.^619047+0.^8260869565217391304347)

AND IF A of -⅄(φnx-1Qn) then A of -⅄(φn-2Qn)then 

An1 of -⅄n2-1Qn1)=(1-1.5)

An2 of -⅄n3-1Qn2)=(2-1.^6)

An3 of -⅄n4-1Qn3)=(1.5-1.4)

An4 of -⅄n5-1Qn4)=(1.^6-1.^571428)

An5 of -⅄n6-1Qn5)=(1.6-1.^18)

An6 of -⅄n7-1Qn6)=(1.625-1.^307692)

An7 of -⅄n8-1Qn7)=(1.^615384-1.^1176470588235294)

An8 of -⅄n9-1Qn8)=(1.^619047-1.^210526315789473684)

so if A of -⅄n2-1Qn1)cn 

and 

A of -⅄n2-2Qn1)cn

then

An1 of -⅄n2-2Qn1)=(1-0.^6)

An2 of -⅄n3-2Qn2)=(2-0.6)

An3 of -⅄n4-2Qn3)=(1.5-0.^714285)

An4 of -⅄n5-2Qn4)=(1.^6-0.^63)

An5 of -⅄n6-2Qn5)=(1.6-0.^846153)

An6 of -⅄n7-2Qn6)=(1.625-0.^7647058823529411)

An7 of -⅄n8-2Qn7)=(1.^615384-0.^894736842105263157)

An8 of -⅄n9-2Qn8)=(1.^619047-0.^8260869565217391304347)

THEN IF M=2/Q)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so

M=2n1/1Qn2)cn

and

M=2n1/2Qn2)cn

then

Mn1 of 2n1/1Qn2)=(0/1.^6)

Mn2 of 2n2/1Qn3)=(1/1.4)

Mn3 of 2n3/1Qn4)=(2/1.^571428)

Mn4 of 2n4/1Qn5)=(1.5/1.^18)

Mn5 of 2n5/1Qn6)=(1.^6/1.^307692)

Mn6 of 2n6/1Qn7)=(1.6/1.^1176470588235294)

Mn7 of 2n7/1Qn8)=(1.625/1.^210526315789473684)

if M=2n1/1Qn2)cn

and

M=2n1/2Qn2)cn

then

Mn1 of 2n1/2Qn2)=(0/0.6)

Mn2 of 2n2/2Qn3)=(1/0.^714285)

Mn3 of 2n3/2Qn4)=(2/0.^63)

Mn4 of 2n4/2Qn5)=(1.5/0.^846153)

Mn5 of 2n5/2Qn6)=(1.^6/0.^7647058823529411)

Mn6 of 2n6/2Qn7)=(1.6/0.^894736842105263157)

Mn7 of 2n7/2Qn8)=(1.625/0.^8260869565217391304347)

V= 1⅄(Q/φ)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so

V= 1⅄(1Qn2n1)cn

and

V= 1⅄(2Qn2n1)cn

then

Vn1 of 1⅄(1Qn2n1)=(1.^6/0)

Vn2 of 1⅄(1Qn3n2)=(1.4/1)

Vn3 of 1⅄(1Qn4n3)=(1.^571428/2)

Vn4 of 1⅄(1Qn5n4)=(1.^18/1.5)

Vn5 of 1⅄(1Qn6n5)=(1.^307692/1.^6)

Vn6 of 1⅄(1Qn7n6)=(1.^1176470588235294/1.6)

Vn7 of 1⅄(1Qn8n7)=(1.^210526315789473684/1.625)

if V= 1⅄(1Qn2n1)cn

and

V= 1⅄(2Qn2n1)cn

then

Vn1 of 1⅄(2Qn2n1)=(0.6/0)

Vn2 of 1⅄(2Qn3n2)=(0.^714285/1)

Vn3 of 1⅄(2Qn4n3)=(0.^63/2)

Vn4 of 1⅄(2Qn5n4)=(0.^846153/1.5)

Vn5 of 1⅄(2Qn6n5)=(0.^7647058823529411/1.^6)

Vn6 of 1⅄(2Qn7n6)=(0.^894736842105263157/1.6)

Vn7 of 1⅄(2Qn8n7)=(0.^8260869565217391304347/1.625)

W=2(Q/φ)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so

W=2(1Qn1/φn2)cn

and

W=2(2Qn1/φn2)cn

then

Wn1 of2(1Qn1/φn2)=(1.5/1)

Wn2 of2(1Qn2/φn3)=(1.^6/2)

Wn3 of2(1Qn3/φn4)=(1.4/1.5)

Wn4 of2(1Qn4/φn5)=(1.^571428/1.^6)

Wn5 of2(1Qn5/φn6)=(1.^18/1.6)

Wn6 of2(1Qn6/φn7)=(1.^307692/1.625)

Wn7 of2(1Qn7/φn8)=(1.^1176470588235294/1.^615384)

Wn8 of2(1Qn8/φn9)=(1.^210526315789473684/1.^619047)

if W=2(1Qn1/φn2)cn

and

W=2(2Qn1/φn2)cn

then

Wn1 of2(2Qn1/φn2)=(0.^6/1)

Wn2 of2(2Qn2/φn3)=(0.6/2)

Wn3 of2(2Qn3/φn4)=(0.^714285/1.5)

Wn4 of2(2Qn4/φn5)=(0.^63/1.^6)

Wn5 of2(2Qn5/φn6)=(0.^846153/1.6)

Wn6 of2(2Qn6/φn7)=(0.^7647058823529411/1.625)

Wn7 of2(2Qn7/φn8)=(0.^894736842105263157/1.^615384)

Wn8 of2(2Qn8/φn9)=(0.^8260869565217391304347/1.^619047)

Then EF and IH paths in wave functions of cycle variants 1⅄, 2⅄, 3

E=∈1/Q)cn and path ⅄ of Q is a variant in the definition of E

F=2/Q)cn and path ⅄ of Q is a variant in the definition of F

I= 1(Q/Θ)cn and path ⅄ of Q is a variant in the definition of I

H=2(Q/Θ)cn and path ⅄ of Q is a variant in the definition of H

E=∈1⅄(Θ/Q)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so 

E=∈1⅄(Θn2/1⅄Qn1)cn

and

E=∈1⅄(Θn2/2⅄Qn1)cn

then

En1 of 1⅄(Θn2/1⅄Qn1)=(1/1.5)

En2 of 1⅄(Θn3/1⅄Qn2)=(0.5/1.^6)

En3 of 1⅄(Θn4/1⅄Qn3)=(0.^6/1.4)

En4 of 1⅄(Θn5/1⅄Qn4)=(0.6/1.^571428)

En5 of 1⅄(Θn6/1⅄Qn5)=(0.625/1.^18)

En6 of 1⅄(Θn7/1⅄Qn6)=(0.^615384/1.^307692)

En7 of 1⅄(Θn8/1⅄Qn7)=(0.^619047/1.^1176470588235294)

En8 of 1⅄(Θn9/1⅄Qn8)=(0.6^1764705882352941/1.^210526315789473684)

if E=∈1⅄(Θn2/1⅄Qn1)cn

and

E=∈1⅄(Θn2/2⅄Qn1)cn

then

En1 of 1⅄(Θn2/2⅄Qn1)=(1/0.^6)

En2 of 1⅄(Θn3/2⅄Qn2)=(0.5/0.6)

En3 of 1⅄(Θn4/2⅄Qn3)=(0.^6/0.^714285)

En4 of 1⅄(Θn5/2⅄Qn4)=(0.6/0.^63)

En5 of 1⅄(Θn6/2⅄Qn5)=(0.625/0.^846153)

En6 of 1⅄(Θn7/2⅄Qn6)=(0.^615384/0.^7647058823529411)

En7 of 1⅄(Θn8/2⅄Qn7)=(0.^619047/0.^894736842105263157)

En8 of 1⅄(Θn9/2⅄Qn8)=(0.6^1764705882352941/0.^8260869565217391304347)

F=2⅄(Θ/Q)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so

F=2⅄(Θn1/1Qn2)cn

and

F=2⅄(Θn1/2Qn2)cn

then

Fn1 of 2⅄(Θn1/1Qn2)=(0/1.^6)

Fn2 of 2⅄(Θn2/1Qn3)=(1/1.4)

Fn3 of 2⅄(Θn3/1Qn4)=(0.5/1.^571428)

Fn4 of 2⅄(Θn4/1Qn5)=(0.^6/1.^18)

Fn5 of 2⅄(Θn5/1Qn6)=(0.6/1.^307692)

Fn6 of 2⅄(Θn6/1Qn7)=(0.625/1.^1176470588235294)

Fn7 of 2⅄(Θn7/1Qn8)=(0.^615384/1.^210526315789473684)

if F=2⅄(Θn1/1Qn2)cn

and

F=2⅄(Θn1/2Qn2)cn

then

Fn1 of 2⅄(Θn1/2Qn2)=(0/0.6)

Fn2 of 2⅄(Θn2/2Qn3)=(1/0.^714285)

Fn3 of 2⅄(Θn3/2Qn4)=(0.5/0.^63)

Fn4 of 2⅄(Θn4/2Qn5)=(0.^6/0.^846153)

Fn5 of 2⅄(Θn5/2Qn6)=(0.6/0.^7647058823529411)

Fn6 of 2⅄(Θn6/2Qn7)=(0.625/0.^894736842105263157)

Fn7 of 2⅄(Θn7/2Qn8)=(0.^615384/0.^8260869565217391304347)

I= 1⅄(Q/Θ)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so

I= 1⅄(1Qn2n1)cn

and

I= 1⅄(2Qn2n1)cn

then

In1 of 1⅄(1⅄Qn2n1)=(1.^6/0)

In2 of 1⅄(1⅄Qn3n2)=(1.4/1)

In3 of 1⅄(1⅄Qn4n3)=(1.^571428/0.5)

In4 of 1⅄(1⅄Qn5n4)=(1.^18/0.^6)

In5 of 1⅄(1⅄Qn6n5)=(1.^307692/0.6)

In6 of 1⅄(1⅄Qn7n6)=(1.^1176470588235294/0.625)

In7 of 1⅄(1⅄Qn8n7)=(1.^210526315789473684/0.^615384)

if I= 1⅄(1Qn2n1)cn

and

I= 1⅄(2Qn2n1)cn

then

In1 of 1⅄(2⅄Qn2n1)=(0.6/0)

In2 of 1⅄(2⅄Qn3n2)=(0.^714285/1)

In3 of 1⅄(2⅄Qn4n3)=(0.^63/0.5)

In4 of 1⅄(2⅄Qn5n4)=(0.^846153/0.^6)

In5 of 1⅄(2⅄Qn6n5)=(0.^7647058823529411/0.6)

In6 of 1⅄(2⅄Qn7n6)=(0.^894736842105263157/0.625)

In7 of 1⅄(2⅄Qn8n7)=(0.^8260869565217391304347/0.^615384)

H=2⅄(Q/Θ)cn

The definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

so

H=2⅄(1Qn1n2)cn

and

H=2⅄(2Qn1n2)cn

then

Hn1 of 2⅄(1⅄Qn1n2)=(1.5/1)

Hn2 of 2⅄(1⅄Qn2n3)=(1.^6/0.5)

Hn3 of 2⅄(1⅄Qn3n4)=(1.4/0.^6)

Hn4 of 2⅄(1⅄Qn4n5)=(1.^571428/0.6)

Hn5 of 2⅄(1⅄Qn5n6)=(1.^18/0.625)

Hn6 of 2⅄(1⅄Qn6n7)=(1.^307692/0.^615384)

Hn7 of 2⅄(1⅄Qn7n8)=(1.^1176470588235294/0.^619047)

Hn8 of 2⅄(1⅄Qn8n9)=(1.^210526315789473684/0.6^1764705882352941)

then

if H=2⅄(1Qn1n2)cn

and

H=2⅄(2Qn1n2)cn

then

Hn1 of 2⅄(2⅄Qn1n2)=(0.^6/1)

Hn2 of 2⅄(2⅄Qn2n3)=(0.6/0.5)

Hn3 of 2⅄(2⅄Qn3n4)=(0.^714285/0.^6)

Hn4 of 2⅄(2⅄Qn4n5)=(0.^63/0.6)

Hn5 of 2⅄(2⅄Qn5n6)=(0.^846153/0.625)

Hn6 of 2⅄(2⅄Qn6n7)=(0.^7647058823529411/0.^615384)

Hn7 of 2⅄(2⅄Qn7n8)=(0.^894736842105263157/0.^619047)

Hn8 of 2⅄(2⅄Qn8n9)=(0.^8260869565217391304347/0.6^1764705882352941)

Then DB and OG paths in wave functions of cycle variants 1⅄, 2⅄, 3

Variables of set 3φ/Θ=(φn1cn/Θn1cn) differ from D and B sets

D=1/Θ)cn

B=2/Θ)cn

O=1/φ)cn

G=2/φ)cn

Variables of set 3Θ/φ=(Θn1cnn1cn) differ from O and G sets

IF D=1n2/Θn1)cn

then

Dn1=n2/Θn1)=(1/0)=0

Dn2=n3/Θn2)=(2/1)=2

Dn3=n4/Θn3)=(1.5/0.5)=3

Dn4=n5/Θn4)=(1.^6/0.^6) ↓ and Dn4=n5c2/Θn4)=(1.^66/0.^6) and Dn4=n5/Θn4c2)=(1.^6/0.^66) and Dn4=n5c2/Θn4c2)=(1.^66/0.^66) and so on for cn 

Dn5=n6/Θn5)=(1.6/0.6)=2.^6 or 2.6 or 2.66 or 2.666 and so on

Dn6=n7/Θn6)=(1.625/0.625)=2.6

Dn7=n8/Θn7)=(1.^615384/0.^615384)=2.^625001 or 2.625001

Dn8=n9/Θn8)=(1.^619047/0.^619047)=2.^615386230770846155461540076924692309307693923078538463153847769232384617000001 or 2.615386230770846155461540076924692309307693923078538463153847769232384617000001

Dn9=n10/Θn9)=(1.6^1762941/0.6^1764705882352941) with a quotient potential of 61,764,705,882,352,941 digits long to divisor of cn of variable Θn9 of Dn9 and Dn8=n9c1/Θn8c2), Dn8=n9c2/Θn8c2) each have quotients based on cn of Dn variables φncn/Θncn

Dn10=n11/Θn10)=(1.6^18/0.6^18)=2.^6181229773462783171521035598705501 or 2.6181229773462783171521035598705501

Dn11=n12/Θn11)=(1.^61797752808988764044943820224719101123595505/0.^6179775280878651685393258764044943820224719101123595505)

Dn12=n13/Θn12)=(1.6180^5/0.6180^5)

Dn13=n14/Θn13)=(1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

Dn14=n15/Θn14)=(1.6183^0223896551724135014/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

Dn15=n16/Θn15)=(1.618^032786885245901639344262295081967213114754098360655737704918/0.6^18032786885245901639344262295081967213114754098360655737749)

Dn16=n17/Θn16)=(1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843/0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

Dn17=n18/Θn17)=(1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

Dn18=n19/Θn18)=(1.6180340557314241486068^11145510835913312693/0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

Dn19=n20/Θn19)=(1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

Dn20=n21/Θn20)=(1.6^1803399852/0.6^1803399852)

Dn21=n22/Θn21)=(1.6^180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981)

Dn22=n23/Θn22)=(1.6180339901755970865563773925808819377787815481903901530122522725989498052058043024109310597932923042177178024956241883575179831742984585850601321212805601038902377053814013889673084523742307040822087^96792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869/0.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114)

and so on for Dn=1/Θ)ncn equations beyond Dn22 that differs from equations such as Dn1of 1(2φn2/2Θn1)ncn or Dn1of 1(1φn2/2Θn1)ncn and Dn1of 1(2φn2/1Θn1)ncn of 1ᐱD(nφncn/nΘncn) sets


IF B=2n1/Θn2)cn

then

Bn1=(φn1/Θn2)=(0/1)=0

Bn2=(φn2/Θn3)=(1/0.5)

Bn3=(φn3/Θn4)=(2/0.^6) and Bn3=(φn3/Θn4c2)=(2/0.^66) and Bn3=(φn3/Θn4c3)=(2/0.^666) and so on for variants of ncn 

Bn4=(φn4/Θn5)=(1.5/0.6)

Bn5=(φn5/Θn6)=(1.^6/0.625)

Bn6=(φn6/Θn7)=(1.6/0.^615384)

Bn7=(φn7/Θn8)=(1.625/0.^619047)

Bn8=(φn8/Θn9)=(1.^615384/0.6^1764705882352941)

Bn9=(φn9/Θn10)=(1.^619047/0.6^18)

Bn10=(φn10/Θn11)=(1.6^1762941/0.^6179775280878651685393258764044943820224719101123595505)

Bn11=(φn11/Θn12)=(1.6^18/0.6180^5)

Bn12=(φn12/Θn13)=(1.^61797752808988764044943820224719101123595505/0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566)

Bn13=(φn13/Θn14)=(1.6180^5/0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

Bn14=(φn14/Θn15)=(1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/0.6^18032786885245901639344262295081967213114754098360655737749)

Bn15=(φn15/Θn16)=(1.6183^0223896551724135014/0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

Bn16=(φn16/Θn17)=(1.618^032786885245901639344262295081967213114754098360655737704918/0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

Bn17=(φn17/Θn18)=(1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843/0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

Bn18=(φn18/Θn19)=(1.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

Bn19=(φn19/Θn20)=(1.6180340557314241486068^11145510835913312693/0.6^1803399852)

Bn20=(φn20/Θn21)=(1.6180339631667062903611576177947859363788567328390337239894762018655823965558478832791126524754843338914135374312365462807940684046878737144223872279359005022721836881128916527146615642190863429801482898828031571394403252^5711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981)

Bn21=(φn21/Θn22)=(1.6^1803399852/0.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114)

and so on for Bn1=2n1/Θn2)ncn equations beyond Bn21 that differs from equations such as Bn1of 2(2φn1/2Θn2)ncn or Bn1of 2(1φn1/2Θn2)ncn and Bn1of 2(2φn1/1Θn2)ncn of 2ᐱB(nφncn/nΘncn) sets


IF O=1n2/φn1)cn

On1=n2/φn1)=(1/0)=0

On2=n3/φn2)=(0.5/1)

On3=n4/φn3)=(0.^6/2) and On3=n4c2/φn3)=(0.^66/2) and On3=n4c3/φn3)=(0.^666/2) and so on for variants of ncn

On4=n5/φn4)=(0.6/1.5)

On5=n6/φn5)=(0.625/1.^6)

On6=n7/φn6)=(0.^615384/1.6)

On7=n8/φn7)=(0.^619047/1.625)

On8=n9/φn8)=(0.6^1764705882352941/1.^615384)

On9=n10/φn9)=(0.6^18/1.^619047)

On10=n11/φn10)=(0.^6179775280878651685393258764044943820224719101123595505/1.6^1762941)

On11=n12/φn11)=(0.6180^5/1.6^18)

On12=n13/φn12)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/1.^61797752808988764044943820224719101123595505)

On13=n14/φn13)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/1.6180^5)

On14=n15/φn14)=(0.6^18032786885245901639344262295081967213114754098360655737749/1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

On15=n16/φn15)=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/1.6183^0223896551724135014)

and so on for On=1/φ)cn

IF G=2n1/φn2)cn

Gn1=n1/φn2)=(0/1)=0

Gn2=n2/φn3)=(1/2)=0.5

Gn3=n3/φn4)=(0.5/1.5)

Gn4=n4/φn5)=(0.^6/1.^6) and Gn4=n4c2/φn5)=(0.^66/1.^6) and Gn4=n4/φn5c2)=(0.^6/1.^66) and Gn4=n4c2/φn5c2)=(0.^66/1.^66) and so on for variants of ncn

Gn5=n5/φn6)=(0.6/1.6)

Gn6=n6/φn7)=(0.625/1.625)

Gn7=n7/φn8)=(0.^615384/1.^615384)

Gn8=n8/φn9)=(0.^619047/1.^619047)

Gn9=n9/φn10)=(0.6^1764705882352941/1.6^1762941)

Gn10=n10/φn11)=(0.6^18/1.6^18)

Gn11=n11/φn12)=(0.^6179775280878651685393258764044943820224719101123595505/1.^61797752808988764044943820224719101123595505)

Gn12=n12/φn13)=(0.6180^5/1.6180^5)

Gn13=n13/φn14)=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/1.^61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

Gn14=n14/φn15)=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/1.6183^0223896551724135014)

Gn15=n15/φn16)=(0.6^18032786885245901639344262295081967213114754098360655737749/1.618^032786885245901639344262295081967213114754098360655737704918)

Gn16=n16/φn17)=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/1.618034447821681864235057244174265450860192502532928064842958459979736575481256332320141843^9716312056737588652482269503546099290780141843)

and so on for Gn=2/φ)ncn

Then LK and UJ paths in wave functions of cycle variants 1⅄, 2⅄, 3

L=1(1Qn2/2Qn1)cn

K=2(1Qn1/2Qn2)cn

U=1(2Qn2/1Qn1)cn

J=2(2Qn1/1Qn2)cn

Variables of set 3(1Qn1cn/2Qn1cn) differ from 3(2Qn1cn/1Qn1cn) sets

L=1(1Qn2/2Qn1)cn

12Qn1 of ∈11Qn and ∈21Qn variables is (11Qn2/21Qn1)=(1.^6/0.^6)=2.^6 depending of cn variable factor c1

then

Ln1=∈12Qn1 of ∈11Qn and ∈21Qn variables is (11Qn2/21Qn1)=(1.^6/0.^6)=2.^6

Ln2=∈12Qn2 of ∈11Qn and ∈21Qn variables is (11Qn3/21Qn2)=(1.4/0.6)

Ln3=∈12Qn3 of ∈11Qn and ∈21Qn variables is (11Qn4/21Qn3)=(1.^571428/0.^714285)

Ln4=∈12Qn4 of ∈11Qn and ∈21Qn variables is (11Qn5/21Qn4)=(1.^18/0.^63)

Ln5=∈12Qn5 of ∈11Qn and ∈21Qn variables is (11Qn6/21Qn5)=(1.^307692/0.^846153)

Ln6=∈12Qn6 of ∈11Qn and ∈21Qn variables is (11Qn7/21Qn6)=(1.^1176470588235294/0.^7647058823529411)

Ln7=∈12Qn7 of ∈11Qn and ∈21Qn variables is (11Qn8/21Qn7)=(1.^210526315789473684/0.^894736842105263157)

Variable Factor 12Qnc1 will differ variants of ∈12Qn given a factor 11Qnc2 factor 21Qnc2 and so on . . .

K=2(1Qn1/2Qn2)cn

22Qn1 of ∈11Qn and ∈21Qn variables is (11Qn1/21Qn2)=(1.5/0.6) depending of cn variable factor

then

Kn1=22Qn1 of ∈11Qn and ∈21Qn variables is (11Qn1/21Qn2)=(1.5/0.6)

Kn2=22Qn2 of ∈11Qn and ∈21Qn variables is (11Qn2/21Qn3)=(1.^6/0.^714285)

Kn3=22Qn3 of ∈11Qn and ∈21Qn variables is (11Qn3/21Qn4)=(1.4/0.^63)

Kn4=22Qn4 of ∈11Qn and ∈21Qn variables is (11Qn4/21Qn5)=(1.^571428/0.^846153)

Kn5=22Qn5 of ∈11Qn and ∈21Qn variables is (11Qn5/21Qn6)=(1.^18/0.^7647058823529411)

Kn6=22Qn6 of ∈11Qn and ∈21Qn variables is (11Qn6/21Qn7)=(1.^307692/0.^894736842105263157)

Kn7=22Qn7 of ∈11Qn and ∈21Qn variables is (11Qn7/21Qn8)=(1.^1176470588235294/0.^8260869565217391304347)

Variable Factor 22Qnc1 will differ variants of ∈11Qn and ∈21Qn given a factor 11Qnc2 factor 21Qnc2 and so on . . .

U=1(2Qn2/1Qn1)cn

12Qn1 of ∈21Qn and ∈11Qn variables is (21Qn2/11Qn1)=(0.6/1.5)=0.4

then

Un1=12Qn1 of ∈21Qn and ∈11Qn variables is (21Qn2/11Qn1)=(0.6/1.5)=0.4

Un2=12Qn2 of ∈21Qn and ∈11Qn variables is (21Qn3/11Qn2)=(0.^714285/1.^6)

Un3=12Qn3 of ∈21Qn and ∈11Qn variables is (21Qn4/11Qn3)=(0.^63/1.4)

Un4=12Qn4 of ∈21Qn and ∈11Qn variables is (21Qn5/11Qn4)=(0.^846153/1.^571428)

Un5=12Qn5 of ∈21Qn and ∈11Qn variables is (21Qn6/11Qn5)=(0.^7647058823529411/1.^18)

Un6=12Qn6 of ∈21Qn and ∈11Qn variables is (21Qn7/11Qn6)=(0.^894736842105263157/1.^307692)

Un7=12Qn7 of ∈21Qn and ∈11Qn variables is (21Qn8/11Qn7)=(0.^8260869565217391304347/1.^1176470588235294)

Variable Factor 12Qnc1 will differ variants of ∈21Qn and ∈11Qn given a factor 11Qnc2 factor 21Qnc2 and so on . . .

J=2(2Qn1/1Qn2)cn

22Qn1 of ∈21Qn and ∈11Qn variables is (21Qn1/11Qn2)=(0.^6/1.^6

depending of cn variable factor and are crossed variants of two different path sets variables 

then

Jn1=22Qn1 of ∈21Qn and ∈11Qn variables is (21Qn1/11Qn2)=(0.^6/1.^6)

Jn2=22Qn2 of ∈21Qn and ∈11Qn variables is (21Qn2/11Qn3)=(0.6/1.4)

Jn3=22Qn3 of ∈21Qn and ∈11Qn variables is (21Qn3/11Qn4)=(0.^714285/1.^571428)

Jn4=22Qn4 of ∈21Qn and ∈11Qn variables is (21Qn4/11Qn5)=(0.^63/1.^18)

Jn5=22Qn5 of ∈21Qn and ∈11Qn variables is (21Qn5/11Qn6)=(0.^846153/1.^307692)

Jn6=22Qn6 of ∈21Qn and ∈11Qn variables is (21Qn6/11Qn7)=(0.^7647058823529411/1.^1176470588235294)

Jn7=22Qn7 of ∈21Qn and ∈11Qn variables is (21Qn7/11Qn8)=(0.^894736842105263157/1.^210526315789473684)

Variable Factor 22Qnc1 will differ variants of ∈21Qn and ∈11Qn given a factor 11Qnc2 factor 21Qnc2 and so on . . .

Then RZ and TS paths in wave functions of cycle variants

R=/P)cn  that paths  1⅄, 2⅄, 3⅄ are then applicable to the variables φ and P of R

Z=(P/φ)cn  that paths  1⅄, 2⅄, 3⅄ are then applicable to the variables P and φ of Z

T=/P)cn  that paths  1⅄, 2⅄, 3⅄ are then applicable to the variables Θ and P of T

S=(P/Θ)cn  that paths  1⅄, 2⅄, 3⅄ are then applicable to the variables Θ and P of S

Phi Prime 

R=/P)cn

R represents /P)cn

3φncn/pn that path 3⅄ of φncn/pn  differ from paths 2φncn/pn and 1φncn/pn

Path 3⅄R=φn1cn/pn1

3⅄Rn1=1φn1/pn1=(φn1/pn1)=(0/2)=0 

3⅄Rn2=1φn2/pn2=(φn2/pn2)=(1/3)=0.^3

3⅄Rn3=1φn3/pn3=(φn3/pn3)=(2/5)=0.4

3⅄Rn4=1φn4/pn4=(φn4/pn4)=(1.5/7)=0.2^142857

3⅄Rn5=1φn5/pn5=(φn5/pn5)=(1.^6/11)=1.^45. . .(φn5c2/pn5)=(1.^66/11)=0.150^9. . . and so on

3⅄Rn6=1φn6/pn6=(φn6/pn6)=(1.6/13)=0.1^230769

3⅄Rn7=1φn7/pn7=(φn7/pn7)=(1.625/17)=0.095^5882352941176470 

3⅄Rn8=1φn8/pn8=(φn8/pn8)=(1.^615384/19)=0.079757^052631578421. . .(φn8c2/pn8)=0.079757079757^052631578421. . . and so on

3⅄Rn9=1φn9/pn9=(φn9/pn9)=(1.^619047/23)=0.070393^3478260865217391304

Path 1⅄R=φn2/pn1

1⅄Rn1=(φn2/pn1)=(1/2)

1⅄Rn2=(φn3/pn2)=(2/3)

1⅄Rn3=(φn4/pn3)=(1.5/5)

1⅄Rn4=(φn5/pn4)=(1.^6/7)

1⅄Rn5=(φn6/pn5)=(1.6/11)

1⅄Rn6=(φn7/pn6)=(1.625/13)

1⅄Rn7=(φn8/pn7)=(1.^615384/17)

1⅄Rn8=(φn9/pn8)=(1.^619047/19)

1⅄Rn9=(φn10/pn9)=(1.6^1762941/23)

Path 2⅄R=φn1/pn2

2⅄Rn1=(φn1/pn2)=(0/3)

2⅄Rn2=(φn2/pn3)=(1/5)

2⅄Rn3=(φn3/pn4)=(2/7)

2⅄Rn4=(φn4/pn5)=(1.5/11)

2⅄Rn5=(φn5/pn6)=(1.^6/13)

2⅄Rn6=(φn6/pn7)=(1.6/17)

2⅄Rn7=(φn7/pn8)=(1.625/19)

2⅄Rn8=(φn8/pn9)=(1.^615384/23)


Variable Differential ratio scale of divisor and dividend to applicable cycle shell phi prime to prime phi and comparable quotient sets.

Z=(P/φ)cn

Z represents (P/φ)cn

3p/φncn that path 3⅄ of p/φncn  differ from paths 2p/φncn and 1p/φncn

3Zn1=pn1/φn1=(pn1/φn1)=(2/0)=0

3Zn2=pn2/φn2=(pn2/φn2)=(3//1)=3

3Zn3=pn3/φn3=(pn3/φn3)=(5/2)=2.5

3Zn4=pn4/φn4=(pn4/φn4)=(7/.1.5)=4

3Zn5=pn5/φn5=(pn5/φn5)=(11/1.^6)=6.875 . . .(pn5/φn5c2)=(11/1.^66)=6.6265060^24096084337349397590361445784337951712047. . . and so on

3Zn6=pn6/φn6=(pn6/φn6)=(13/1.6)=8.125

3Zn7=pn7/φn7=(pn7/φn7)=(17/1.625)=10.46150^76923

3Zn8=pn8/φn8=(pn8/φn8)=(19/1.^615384)= 11.7619924287971155465202081053173734542375063761929052163510348003942096739846377084334127365385567765992482282850393466816496882475006561907261678956830078792410968537573691456644 extended shell 588704/1615384 →. . . then (pn8/φn8c2)=(19/1.^615384615384). . . and so on

3Zn9=pn9/φn9=(pn9/φn9)=(23/1.^619047)=^14.20588778460415293688200527841378292291699993885291779670386344559484684508849959266160895885048426636163125591783314505384957941307448146965467957384807235367472346386485383067940584800811835604525378200879900336432481577125308900853403267477719917951733334486274950634539948500568544335031657512104342863425212486110656454074526557907213317463915500908867994567174393331385685529820937872711539566176892949988480877948570980335963069632938389064678171788712742743107519423463308971265194895515695344236455149232851177266626601945465449736789605243084357649901454374085495973866107654688220910202112724337218128936343416837188790689831734347427838722408923274000075352969987900289491287158433325283330255390980002433530342232189677013700034650013248534477380829586787783183564158421589984725582395075621646561217802818571665924460500529014908152758999584323370476582829281670019462066264907689523528347231426882604396289916228497381484292920464940177771244441946404273625163444915434820607431408723773923795912039613426911016171859124534371145494849748030786011771122147781997681352054634609124997606616731941691624764444762875938746682461966823693197294457789057389933707915829497228925411059715993420821013843328822449255642362451491525570289188639983891758546848856148092056623433414842188027895422430602694053971255930186090953505364575580573016101447332906333170068565026216039435544490061128552784446652876661394017591830255699803649924924971294841965674869228626469768944323419888366427904810669486432450694760559761390497002248853801032335688834233966030634070536556381624498856426033339365688580998575087690474705181504922340117365338992629614828970375782790740478812536016557888683898614431823165108857247504241692798294305230175529184761158879266630307829235346472338357070548291680229171852330414126334813010369680435466048854665738548664739195341457042321810299515702756003994942703948680921554470006120884693279441548021768361264373424613368234523148494145012467210649227601175259272893251400360829549728945484596802934071710086242091798446864112036278131518109109865247889653604867554802300365585433900312961884367779317092091829329228861175741037783337975982167287299256908539406206243549446063023494685453850320589828460816764429939340859159740266959513837461173146919144410261098041008074503087310003971472106739334929745708432182635834537230852470620062295906171964124574518219668731049808930809297074142998937029005334619686766350822428255634333036656749309933559680478701359503460986617436059607905144199025723156894148224233144559731743426843074969411017715977361991344290808111191336631981653404749831227876645952835217260524246671035491866511596019139654376926673530786938242064621965884869308920618116706926976177961479808801103365127757254730715044096928625296239083856120297928349207898226549321915917203144812967134369786670800785894418136101052038637544184943364831286553138976200196782428181516657638722038334897010401798094805153896088254386685500791515008520444434287577815838576644161658061810435398107652217631730270955691835999819646989865025536627411063421877190717749392080649913189672690168969770488441657345339573218072112792278420577043161810620692296147054409167862328888537516205520902110933160062678847494853453914555908506670899609461615382382352087369915759085437297373084289708699006267267102190362602197465546089767622558208625197415516658874016628300475526652407249449830671994080468324884947750127080930942708889859281416784071123321311858148651645072687821910049553842476469182179393186238571208865462213264963895427371781053916285320932622709532212468198884899573638072273380575116102250274389810796104127922166558475448828848081618384148205703725710248065683083937649740866077389970766753528464584412929334355333724098188625778003973942695919266086778209650491925188089042504633898830608376409085097591360843755616730088749739816076988500025014715446802964954074835381554704712092978153197529163761150849851795531568879717512833166671504903810698515855314885855691650705631152153087587945254214361905491316805503484457214645405599713905772963972015636358919784292858700210679492318629415946541391324649624130738638223596967845899470490974011254769009176385861559300007967650105277981429816429047458165204592578226574027807716514715137979317462680206318902416050923784176741008753915111791072155409941774389501972456636527537495823160167678887641927627795857686651468425561456832321730005367354993400438653108896776931120591310814324723124158841590145313879090600828759140407906626552533681851113648955218718171862830418141042230398499858249945801449865260242599504523339964806457131880668072020145184173158654443014934093945388861472211739375076819882313484413979334756804465837001643559451949202215871435480254742450342701601621200619870825244727299454555673800698806149543527766642969598782493652129925814383399617182206569667217813936222975614667146784497299954849982736758105231040235397737063840642056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Path 1Zn=(pn2/φn1)

1Zn1=(pn2/φn1)=(3/0)

1Zn2=(pn3/φn2)=(5/1)

1Zn3=(pn4/φn3)=(7/2)

1Zn4=(pn5/φn4)=(11/1.5)

1Zn5=(pn6/φn5)=(13/1.^6)

1Zn6=(pn7/φn6)=(17/1.6)

1Zn7=(pn8/φn7)=(19/1.625)

1Zn8=(pn9/φn8)=(23/1.^615384)

Path 2Zn=(pn1/φn2)

2Zn1=(pn1/φn2)=(2/1)

2Zn2=(pn2/φn3)=(3/2)

2Zn3=(pn3/φn4)=(5/1.5)

2Zn4=(pn4/φn5)=(7/1.^6)

2Zn5=(pn5/φn6)=(11/1.6)

2Zn6=(pn6/φn7)=(13/1.625)

2Zn7=(pn7/φn8)=(17/1.^615384)

2Zn8=(pn8/φn9)=(19/1.^619047)

2Zn9=(pn9/φn10)=(23/1.6^1762941)


T=/P)cn

T represents /P)cn

3Θncn/pn that path 3⅄ of Θncn/pn  differ from paths 2Θncn/pn and 1Θncn/pn


Path 1⅄T=Θn2cn/pn1

1⅄Tn1=1Θn2/pn1=(Θn2/pn1)=(1/2)=0.5

1⅄Tn2=1Θn3/pn2=(0.5/3)=0.1^6

1⅄Tn3=1Θn4/pn3=(0.^6/5)=0.12

1⅄Tn4=1Θn5/pn4=(0.6/7)=0.0^857142 or 0.0857142

1⅄Tn5=1Θn6/pn5=(0.625/11)=0.056^81 or 0.05681

1⅄Tn6=1Θn7/pn6=(0.^615384/13)=0.047337^230769 or 0.047337230769

1⅄Tn7=1Θn8/pn7=(0.^619047/17)=0.036414^5294117647058823 or 0.0364145294117647058823

1⅄Tn8=1Θn9/pn8=(0.6^1764705882352941/19)=0.03250773993808049^526315789473684210526315789473684210526315789473684210526315789473684210

or

0.03250773993808049526315789473684210526315789473684210526315789473684210526315789473684210

1⅄Tn9=1Θn10/pn9=(0.6^18/23)

1⅄Tn10=1Θn11/pn10=(0.^6179775280878651685393258764044943820224719101123595505/29)

1⅄Tn11=1Θn12/pn11=(0.6180^5/31)=0.01993^709677419354838 or 0.01993709677419354838

1⅄Tn12=1Θn13/pn12=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/37)=0.016703398793643417236979468739125391485906507365735297529288945597958473494954181649460619417700962765340447^729

or

0.016703398793643417236979468739125391485906507365735297529288945597958473494954181649460619417700962765340447729

1⅄Tn13=1Θn14/pn13=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/41)=0.014879989648702788380668952578119945654331364430355178883353820275473895321860639192534062237174095878889816911431066830562204826227599146011515817428989454616^02439

or

0.01487998964870278838066895257811994565433136443035517888335382027547389532186063919253406223717409587888981691143106683056220482622759914601151581742898945461602439

1⅄Tn14=1Θn15/pn14=(0.6^18032786885245901639344262295081967213114754098360655737749/47)=0.0131496337635158702476456226020230205790024415765608650156967872340425531914893617021276595744^6808510638297872340425531914893617021276595744

or

0.01314963376351587024764562260202302057900244157656086501569678723404255319148936170212765957446808510638297872340425531914893617021276595744

1⅄Tn15=1Θn16/pn15=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/53)=0.01166102731739022385349161744183823669973810479631435071017568006728986255280916059719753015618130030012808013610904016363671101928848616^7358490566037

or

0.011661027317390223853491617441838236699738104796314350710175680067289862552809160597197530156181300300128080136109040163636711019288486167358490566037

1⅄Tn16=1Θn17/pn16=(0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/59)=0.0104751493796631395731403160587117795018201500695159355995882109463719049488978274943485136325525614764972458953758636426350254184222^5254237288135593220338983050847457627118644067796610169491525423728813559322033898305084745762711864406779661016949152542372881355932203389830508474576271186440677966101694915254237288135593220338983050847457627118644067796610169491525423728813559322033898305084745762711864406779661016949152542372881355932203389830508474576271186440677966101694915254237288135593220338983050847457627118644067796610169491

or

0.0104751493796631395731403160587117795018201500695159355995882109463719049488978274943485136325525614764972458953758636426350254184222^5254237288135593220338983050847457627118644067796610169491525423728813559322033898305084745762711864406779661016949152542372881355932203389830508474576271186440677966101694915254237288135593220338983050847457627118644067796610169491525423728813559322033898305084745762711864406779661016949152542372881355932203389830508474576271186440677966101694915254237288135593220338983050847457627118644067796610169491

1⅄Tn17=1Θn18/pn17=(0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/61)=0.010131705831599248845353499467086230523270567933817185200223316246256915190580114703344668324620616149824899761457646043749682789422930518195198700^704918032786885245901639344262295081967213114754098360655737

or

0.010131705831599248845353499467086230523270567933817185200223316246256915190580114703344668324620616149824899761457646043749682789422930518195198700704918032786885245901639344262295081967213114754098360655737

1⅄Tn18=1Θn19/pn18=(0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/67)=0.009224387509950843724453551424889425153591049773852574011073548783230463325563048188857196914256747832233237067472967618258861159402699489874235614560538612843460287655242086624995091512064170893915973826157421455268503214613371792080020847686941994166931427531084115419077775437569388170365584181460551821138269427795250011601880575596^059701492537313432835820895522388


or

0.009224387509950843724453551424889425153591049773852574011073548783230463325563048188857196914256747832233237067472967618258861159402699489874235614560538612843460287655242086624995091512064170893915973826157421455268503214613371792080020847686941994166931427531084115419077775437569388170365584181460551821138269427795250011601880575596059701492537313432835820895522388

1⅄Tn19=1Θn20/pn19=(0.6^1803399852/71)=0.00870470420^4507042253521126760563380281690140845070422535211267605633802816901408450704225352112676056338028169014084507042253521126760563380281690140845070422535211267605633802816901408

or

0.008704704204507042253521126760563380281690140845070422535211267605633802816901408450704225352112676056338028169014084507042253521126760563380281690140845070422535211267605633802816901408

1⅄Tn20=1Θn21/pn20=(0.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981/73)=0.0084662189728405197119608338818959324604722060225916016108968310185243123778248888065697358639798362571928445744864578040642856964075198546288254419579054336481206620795987275016331730612796567958771453386362441775190286562427258096408521033516966227733155790943836367322522269972893081603588225135096576218497280547845087590637976216995512215633908927762440273421954351248595220872577459959101842419448901081022904470013^43835616

or

0.0084662189728405197119608338818959324604722060225916016108968310185243123778248888065697358639798362571928445744864578040642856964075198546288254419579054336481206620795987275016331730612796567958771453386362441775190286562427258096408521033516966227733155790943836367322522269972893081603588225135096576218497280547845087590637976216995512215633908927762440273421954351248595220872577459959101842419448901081022904470013^43835616

1⅄Tn21=1Θn22/pn21=(0.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114/79)=0.007823215065513887171599713830137746047832677825194812063446231298720883610200054460897861516371503370929458843070422515078593079177711913285671709421806801036901189205878632245282735680964915603476063291853950452018305151128991565707930921854329248289520422479343095794718150559367738993645513872877400800046313204480659591514677640799646075634894712504350796794382951594839508308145763664003419^1645569620253

or

0.0078232150655138871715997138301377460478326778251948120634462312987208836102000544608978615163715033709294588430704225150785930791777119132856717094218068010369011892058786322452827356809649156034760632918539504520183051511289915657079309218543292482895204224793430957947181505593677389936455138728774008000463132044806595915146776407996460756348947125043507967943829515948395083081457636640034191645569620253


and so on for cn of variable Θncn and beyond variable 1⅄Tn21


Path 2⅄T=Θn1cn/pn1

2⅄Tn1=1Θn1/pn2=(Θn1/pn2)=(0/3)=0

2⅄Tn2=1Θn2/pn3=(1/5)=0.2

2⅄Tn3=1Θn3/pn4=(0.5/7)=0.0^714285 or 0.0714285

2⅄Tn4=1Θn4/pn5=(0.^6/11)=0.0^54 or 0.054 and 2⅄Tn4=1Θn4c2/pn5=(0.^66/11)=0.06 and so on for cn of 2⅄Tn4=1Θn4cn/pn5

2⅄Tn5=1Θn5/pn6=(0.6/13)=0.0^461538 or 0.0461538

2⅄Tn6=1Θn6/pn7=(0.625/17)=0.036^7647058823529411 or 0.0367647058823529411

2⅄Tn7=1Θn7/pn8=(0.^615384/19)=0.032388^631578947368421052631578947368421052631578947368421052631578947368421052631578947368421052

or

0.032388631578947368421052631578947368421052631578947368421052631578947368421052631578947368421052

2⅄Tn8=1Θn8/pn9=(0.^619047/23)=0.026915^0869565217391304347826 or 0.0269150869565217391304347826

2⅄Tn9=1Θn9/pn10=(0.6^1764705882352941/29)=0.02129817444219066^931034482758620689655172413793103448275862068965517241379310344827586206896551724137

or

0.02129817444219066931034482758620689655172413793103448275862068965517241379310344827586206896551724137

2⅄Tn10=1Θn10/pn11=(0.6^18/31)=0.019^935483870967741 or 0.019935483870967741

2⅄Tn11=1Θn11/pn12=(0.^6179775280878651685393258764044943820224719101123595505/37)=0.0167020953537260856361979966595809292438505921651989067^702 or 0.0167020953537260856361979966595809292438505921651989067702

2⅄Tn12=1Θn12/pn13=(0.6180^5/41)=0.01507^43902 or 0.0150743902

2⅄Tn13=1Θn13/pn14=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/43)=0.014372691985228056692284659147619522906477692384469907176364906677313105100309412116977742289649665635292943^395348837209302325581395348837209302325581

or

0.014372691985228056692284659147619522906477692384469907176364906677313105100309412116977742289649665635292943395348837209302325581395348837209302325581

2⅄Tn14=1Θn14/pn15=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/47)=0.012980416502059879225689937355381229187820977481799198600372481516902759748857153338168011738811445341159201986567526384107455273943224786946215925842309949771^4255319148936170212765957446808510638297872340

or

0.0129804165020598792256899373553812291878209774817991986003724815169027597488571533381680117388114453411592019865675263841074552739432247869462159258423099497714255319148936170212765957446808510638297872340

2⅄Tn15=1Θn15/pn16=(0.6^18032786885245901639344262295081967213114754098360655737749/53)=0.011660995978966903804515929477265697494587070832044540674297^1509433962264 or 0.0116609959789669038045159294772656974945870708320445406742971509433962264

2⅄Tn16=1Θn16/pn17=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/59)=0.01047516013257087905483145295622756856078168735940102690914086514519258839489636460426218810640015111706420757989456150292789294953033503^1694915254237288135593220338983050847457627118644067796610

or

0.010475160132570879054831452956227568560781687359401026909140865145192588394896364604262188106400151117064207579894561502927892949530335031694915254237288135593220338983050847457627118644067796610

2⅄Tn17=1Θn17/pn18=(0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/61)=0.0101317018590184464723816171715409014853670303951055770553394171448515146227044561010911853167311660182514345545438681133683032735559^491803278688524590163934426229508196721311475409836065573770

or

0.0101317018590184464723816171715409014853670303951055770553394171448515146227044561010911853167311660182514345545438681133683032735559491803278688524590163934426229508196721311475409836065573770

2⅄Tn18=1Θn18/pn19=(0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/67)=0.009224388891456032530844230858093433759992606626311168615128690910771221292916223834388429370176978882676401275356961323413890300817891964326971951^388059701492537313432835820895522

or

0.009224388891456032530844230858093433759992606626311168615128690910771221292916223834388429370176978882676401275356961323413890300817891964326971951388059701492537313432835820895522

2⅄Tn19=1Θn19/pn20=(0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/71)=0.008704703706573331401949125992501288525219723026029893785097574203893535814263721530330030890918339503656716669305476484835826727887054448191180086979663198035378017928186194420770015933919710561864369666937285035253376272945012817878329532324297374777245149923699094832087478229819000104429494931800802422764282417778616208131352092463^88732394366197183098591549295774647

or

0.00870470370657333140194912599250128852521972302602989378509757420389353581426372153033003089091833950365671666930547648483582672788705444819118008697966319803537801792818619442077001593391971056186436966693728503525337627294501281787832953232429737477724514992369909483208747822981900010442949493180080242276428241777861620813135209246388732394366197183098591549295774647

2⅄Tn20=1Θn20/pn21=(0.6^1803399852/73)=0.00846621915^78082191 or 0.0084662191578082191


and so on for cn of variable Θncn and beyond variable 2⅄Tn17=(1Θn17/pn18)


Path 3⅄T=Θn1cn/pn1

3⅄Tn1=1Θn1c1/pn1=(Θn1c1/pn1)=(0/2)

3⅄Tn2=1Θn2c1/pn2=(1/3)=0.^3 or 0.3 or 0.33 and so on for cn of 3⅄Tn2=1Θn2c1/pn2

3⅄Tn3=1Θn3c1/pn3=(0.5/5)=0.1

3⅄Tn4=1Θn4c1/pn4=(0.^6/7)=0.0^857142 or 0.0857142 and 3⅄Tn4=1Θn4c2/pn4=(0.^66/7)=0.09^428571 or 0.09428571

3⅄Tn5=1Θn5c1/pn5=(0.6/11)=0.0^54 or 0.054

3⅄Tn6=1Θn6c1/pn6=(0.625/13)=0.048^076923 or 0.048076923

3⅄Tn7=1Θn7c1/pn7=(0.^615384/17)=0.036199^0588235294117647 or 0.0361990588235294117647

3⅄Tn8=1Θn8c1/pn8=(0.^619047/19)=0.032581^421052631578947368 or 0.032581421052631578947368

3⅄Tn9=1Θn9c1/pn9=(0.6^1764705882352941/23)=0.02685421994884910^4782608695652173913043

or

0.026854219948849104782608695652173913043

3⅄Tn10=1Θn10c1/pn10=(0.6^18/29)=0.021^3103448275862068965517241379 or 0.0213103448275862068965517241379

3⅄Tn11=1Θn11c1/pn11=(0.^6179775280878651685393258764044943820224719101123595505/31)

3⅄Tn12=1Θn12c1/pn12=(0.6180^5/37)

3⅄Tn13=1Θn13c1/pn13=(0.6180257553648064377682403433476394849785407725322060085836909871244635193133047210300429184^54935622317596566/41)

3⅄Tn14=1Θn14c1/pn14=(0.610079575596814323607427055702917771827585941644562334217506631^294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/43)

3⅄Tn15=1Θn15c1/pn15=(0.6^18032786885245901639344262295081967213114754098360655737749/47)

3⅄Tn16=1Θn16c1/pn16=(0.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/53)

3⅄Tn17=1Θn17c1/pn17=(0.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/59)

3⅄Tn18=1Θn18c1/pn18=(0.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/61)

3⅄Tn19=1Θn19c1/pn19=(0.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/67)

3⅄Tn20=1Θn20c1/pn20=(0.6^1803399852/71)


and so on for cn of variable Θncn and beyond variable where c1, c2, c3, . . . of theta quotient ratio decimal stem count variable changes the quotient of 3⅄Tn=Θncn/Pn variables and the cn of 3⅄Tncn is then dependent of definition to variable Θncn

S=(P/Θ)cn

S represents (P/Θ)cn

3⅄Pn1/Θn1cn that path 3⅄ of Pn1/Θn1cn  differ from paths 2⅄Pn1/Θn2cn and 1⅄Pn2/Θn1cn based on cn of theta Θn variable and variable of the sequential set with no steps

Path 1⅄S=Pn2/Θn1cn

1⅄Sn1=Pn2/Θn1cn=(Pn2/Θn1cn)=(3/0)=0

1⅄Sn2=Pn3/Θn2cn=(Pn3/Θn2cn)=(5/1)=5

1⅄Sn3=Pn4/Θn3cn=(Pn4/Θn3cn)=(7/0.5)=14

1⅄Sn4=Pn5/Θn4cn=(Pn5/Θn4c1)=(11/0.^6)=18.^3 or 18.3 and 1⅄Sn4=Pn5/Θn4cn=(Pn5/Θn4c2)=(11/0.^66)=18.^6 or 18.6 and so on for cn variants of 1⅄Sn4 

1⅄Sn5=Pn6/Θn5cn=(Pn6/Θn5cn)=(13/0.6)=21.^6 or 21.6

1⅄Sn6=Pn7/Θn6cn=(Pn7/Θn6cn)=(17/0.625)=27.2

1⅄Sn7=Pn8/Θn7cn=(Pn8/Θn7cn)=(19/0.^615384)=^30.8750 or 30.8750308750

1⅄Sn8=Pn9/Θn8cn=(Pn9/Θn8cn)=(23/0.^619047)=^37.1538833077294615756154217692679231140769602308063846525384986923448461910000371538833077294615756154217692679231140769602308063846525384986923448461910000 

or

37.1538833077294615756154217692679231140769602308063846525384986923448461910000371538833077294615756154217692679231140769602308063846525384986923448461910000371538833077294615756154217692679231140769602308063846525384986923448461910000371538833077294615756154217692679231140769602308063846525384986923448461910000

1⅄Sn9=Pn10/Θn9cn=(Pn10/Θn9cn)=(29/0.6^1764705882352941)=46.9523809523809525151020408163265309955296404275996123681799 extended shell continues with a quotient decimal stem cycle potential having the probability based on divisor or 61,764,705,882,352,941 or less digits determined by this cn variable

1⅄Sn10=Pn11/Θn10cn=(Pn11/Θn10cn)=(31/0.6^18)=^50.16181229773462783171521035598705 or 50.1618122977346278317152103559870550.16181229773462783171521035598705 and so on . . . for 1⅄Sn10c1, 1⅄Sn10c2, 1⅄Sn10c3 infinitely

and so on for cn variables of 1⅄Sn


Path 2⅄S=Pn1/Θn2cn

2⅄Sn1=Pn1/Θn2cn=(Pn1/Θn2cn)=(2/1)=2

2⅄Sn2=Pn2/Θn3cn=(Pn2/Θn3cn)=(3/0.5)=6

2⅄Sn3=Pn3/Θn4cn=(Pn3/Θn4cn)=(5/0.^6)=8.^3 or 8.3

2⅄Sn4=Pn4/Θn5cn=(Pn4/Θn5cn)=(7/0.6)=11.^6 or 11.6 or 11.66 or 11.666 and so on

2⅄Sn5=Pn5/Θn6cn=(Pn5/Θn6cn)=(11/0.625)=17.6

2⅄Sn6=Pn6/Θn7cn=(Pn6/Θn7cn)=(13/0.^615384)=^21.1250 or 21.1250211250 and so on . . . 2⅄Sn6c1, 2⅄Sn6c2, 2⅄Sn6c3  infinitely

while 2⅄Sn6=Pn6/Θn7c2=(13/0.^615384615384)=^21.1250000000 or 21.1250000000211250000000 and so on . . .

2⅄Sn7=Pn7/Θn8cn=(Pn7/Θn8cn)=(17/0.^619047)=^27.4615659231043846428461813077197692582307966923351538736154120769505384890000 or 27.4615659231043846428461813077197692582307966923351538736154120769505384890000274615659231043846428461813077197692582307966923351538736154120769505384890000 and so on . . .

2⅄Sn8=Pn8/Θn9cn=(Pn8/Θn9cn)=(19/0.6^1764705882352941)=30.76190476190476199265306122448979616948493683187560810329029571012078505701989250510700492481874049078191883281544902128167285566318767985239863522815527576875800541377697838692763451555327158169800337777  extended shell continues with a quotient decimal stem cycle potential having the probability based on divisor or 61,764,705,882,352,941 or less digits determined by this cn variable

2⅄Sn9=Pn9/Θn10cn=(Pn9/Θn10cn)=(23/0.6^18)=^37.21682847896440129449838187702265 or 37.216828478964401294498381877022653721682847896440129449838187702265 and so on for 2⅄Sn9c1, 2⅄Sn9c2, 2⅄Sn9c3 infintely

2⅄Sn10=Pn10/Θn11cn=(Pn10/Θn11cn)=(29/0.^6179775280878651685393258764044943820224719101123595505)

and so on for cn variables of 2⅄Sn


Path 3⅄S=Pn1/Θn1cn

3⅄Sn1=Pn1/Θn1cn=(Pn1/Θn1cn)=(2/0)=0

and so on for cn variables of 2⅄Sn and the variants of Θncn variables



such that AMVWEFIHDBOGLKUJRZTS are factors defined within sets ⑆⨊=1∘⧊°n∘⧊° and ⑆⨊=1∘∇°n∘∇° of sets ∈0 base to nΘn1 and nφn1 factorable variables to degrees in stem cell cycles of cn precision, and the definition of Q variable should be accurate to its defining base path where 1⅄Q and 2⅄Q, differ from prime base just as φ and Θ differ in paths 1⅄ and 2⅄ of Y base.

IF WAVE MAV MAP DBOGL JUNK. . . Nn is a number applicable to a short phrase of letters pertaining to precise numeral keys if (In2Fn3 Wn5An8Vn13En21 Mn34An55Vn89 Mn2An3Pn5 Dn8Bn13On21Gn34Ln55 Jn89Un1Nn0Kn1) cipher numeral example that a shift in Ncn can alter the number of each letter in the example very much. 

DNA of these number ratios from these definitions is then (1/Θ)cn)x(a number)x(1/Q)cn)

RNA of these number ratios from these definitions is then /P)cnx(a number)x(1/Q)cn)

The DNA and RNA examples here are only examples of letters that represent ratio sets of a defined path as explained.

RNA of these number ratios from these definitions is then /P)cnx(a number)x(1/Q)cn)

The DNA and RNA examples here are only examples of letters that represent ratio sets of a defined path as explained.

The acronym of their letter structure forms multiplication equations of variables from letters defined in a list of

A  B  C  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇°  2  3ncn  1  1-⅄  2-⅄  ncn +⅄

As proven prime numbers divided by later with previous and previous to later return to either the remainder or the dividend and as RNA represents a phi ratio divided by a prime multiplied with a number and multiplied again by quotient divided with a quotient from prime base while yet DNA of the acronym examples here represents phi divided by a theta quotient multiplied by a number multiplied again by a quotient of phi divided by a prime base quotient as well the RNA factors common to DNA of this example have base path variable in both acronym structures as well as in some case with certain variables the common factors of the Y base and prime base of the 10 digits mentioned on this page and more.  | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229 : 433494437 | for | Y,φ,Θ,P,Q | of this DNA RNA acronym example.

A predictable unit measure common factor along with identified and definable quotient variables that are represented here in no way are exact to a scale measure of dna rna structure sequencing and are mere formulas structured from letters affixed to definitions of sets in consecutive sequence numerals explained here. If the acronyms here DNA and RNA multiplication equations represented by letters defined from a library of variables, then D+N+A and R+N+A would be addition of the variables while D-N-A and R-N-A are differences from subtraction using the variables just as D/N/A and R/N/A equal ᐱ complex equations with quotients dependent of cn in the variables used. A multitude of combinations using the letters that represent numbers from the definitions yet the values as applied require solving the base equations and structuring the sequences of the consecutive values. As (N) represents a number, that number could be any whole number, fractional number, or a number from the for all for any equations described here on this page using the variables on similar paths with 2nd or third or forth and so on of consecutive variables such as ⅄∀Y or ⅄∀P and so on.

AMVWEFIHDBOGLKUJRZTS variables are all ratio sets that are then also applicable to division with Y in paths  1⅄, 2⅄, 3⅄ and more such as every other or every third of the consecutive numbers in Y Θ φ P Q scale to degrees in stem cycle variants of Ncn applicable in functions with AMVWEFIHDBOGLKUJRZTS that have such potential.

N a number or whole number of a consecutive or sequential numbers set as well as Y can be applied to equations or functions of these ratios φΘQAMVWEFIHDBOGLKUJRZTSᐱᗑ from libraries of properly ordered and calculated groups. The Libraries of ordinal sequential numbers are then also applicable to the cn stem cycle variants to alternate set paths 1⅄, 2⅄, 3⅄ using the variant defined ⅄Nncn. Such numbers should not be overly seen and labeled as maleware or malicious number equations if they are defined to the cycle stem decimal that is labelled in this explanation. The control and limit of numbers to 10 or 11 digits rounded is simply a mask of the limit in the potential of progress in that limited system of round whole numbers that within a ten digit limit of prime and fibonacci numbers exist infinite potential in numerals that is not including the numbers not mentioned in prime and fibonacci sequences.

Continuing on 3⅄ and 2⅄ and 1⅄ to ⅄ᐱ and ⅄ᗑ from A M V W E F I H from Y φ Q P

A1A=(1An2cn/1An1cn) and A2A=(1An1/1An2) for a set 1⅄A, 2⅄A, 3⅄A and so on can be stemmed of each 1A, 2A, 3A tier of A and so on where 3⅄A A=(1An1cn/1An1cn) two ratios of same tier numeral number same and cycle number differential of pair sets differ to the equaling a different quotient.

(1⅄A) of 1⅄A, 2⅄A, 3⅄A . . . →and so on

(2⅄A) of 1⅄A, 2⅄A, 3⅄A . . . →and so on

(3⅄A) of 1⅄A, 2⅄A, 3⅄A . . . →and so on

of all variable sets mentioned previously and below

| 2A/1A | : | 2M/1M | : | 2V/1V | : | 2W/1W | Later variable divided by the previous variable

Numeral Array logic symbols to use of next tier alt paths and stem cell cycle notations 

ᐱ for (⅄ᐱ)

1ᐱ is a ratio of divided variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  Y  Z  φ  Θ using the later divided by previous path 1⅄ for ᐱ

(ᐱ)=1(⅄ᐱ) and 2(⅄ᐱ) and and 3(⅄ᐱ)of variables ⅄A , ⅄M, ⅄V, ⅄W, A, M, V, W, φ, Θ, Q, Y, P and whole numbers or a variable factors noted that (ᐱ) is applicable with in quanta such that 1⅄, 2⅄, and 3⅄ paths differ variables of ᐱ

(ᐱ)=sets like

∈(A/A) then

Example

if ∈(ᐱ) of A/A=∈(A/A)

then ᐱ of A/A needs a definition of the path of variables of A.

as (ᐱ) of 1⅄(A/A) and (ᐱ) of 2⅄(A/A) and (ᐱ) of 3⅄(A/A) differ in path of Nn/Nn

(ᐱ) of 1⅄(A/A)=(An2/An1)=(1n2/1Qn1)n2 /1n2/1Qn1)n1) of set ∈A=1n2/1Qn1)cn 

and

(ᐱ) of 1⅄(A/A)=(An2/An1)=(1n2/2Qn1)n2 /1n2/2Qn1)n1) of set A=∈1n2/2Qn1)cn

and the defined path of Q in the base of A is essential to the definition of an ∈(ᐱ) of 1⅄(A/A)ncn

then as 2⅄(A/A) would differ in path of its set (ᐱ)

(ᐱ) of 2⅄(A/A)=(An1/An2) dependent again on the path of Q to the A

and so on for 

(ᐱ) of 3⅄(A/A)=(Ancn/Ancn) that is division path of like terms with a difference in variant stem decimal cycle of Nncn

(ᐱ)=sets like ∈(A/A) that ∈1ᐱ(An2/An1) and ∈2ᐱ(An1/An2) ∈3ᐱ(An1cn/An1cn) for all variables A,B,D,E,F,G,H,I,J,K,L,M,N,O,P,Q,R,S,T,U,V,W,X,Y,Z,φ that provide variables for factoring complex ᗑ variables.

nᐱ(An/An), ∈nᐱ(An/Bn), ∈nᐱ(An/Dn), ∈nᐱ(An/En), ∈nᐱ(An/Fn), ∈nᐱ(An/Gn), ∈nᐱ(An/Hn), ∈nᐱ(An/In), ∈nᐱ(An/Jn), ∈nᐱ(An/Kn), ∈nᐱ(An/Ln), ∈nᐱ(An/Mn), ∈nᐱ(An/Nn), ∈nᐱ(An/On), ∈nᐱ(An/Pn), ∈nᐱ(An/Qn), ∈nᐱ(An/Rn), ∈nᐱ(An/Sn), ∈nᐱ(An/Tn),∈nᐱ(An/Un),  ∈nᐱ(An/Vn), ∈nᐱ(An/Wn), ∈nᐱ(An/Yn), ∈nᐱ(An/Zn), ∈nᐱ(Ann), ∈nᐱ(Ann)

nᐱ(Bn/An), ∈nᐱ(Bn/Bn), ∈nᐱ(Bn/Dn), ∈nᐱ(Bn/En), ∈nᐱ(Bn/Fn), ∈nᐱ(Bn/Gn), ∈nᐱ(Bn/Hn), ∈nᐱ(Bn/In), ∈nᐱ(Bn/Jn), ∈nᐱ(Bn/Kn), ∈nᐱ(Bn/Ln), ∈nᐱ(Bn/Mn), ∈nᐱ(Bn/Nn), ∈nᐱ(Bn/On), ∈nᐱ(Bn/Pn), ∈nᐱ(Bn/Qn), ∈nᐱ(Bn/Rn), ∈nᐱ(Bn/Sn), ∈nᐱ(Bn/Tn),∈nᐱ(Bn/Un),  ∈nᐱ(Bn/Vn), ∈nᐱ(Bn/Wn), ∈nᐱ(Bn/Yn), ∈nᐱ(Bn/Zn), ∈nᐱ(Bnn), ∈nᐱ(Bnn)

nᐱ(Dn/An), ∈nᐱ(Dn/Bn), ∈nᐱ(Dn/Dn), ∈nᐱ(Dn/En), ∈nᐱ(Dn/Fn), ∈nᐱ(Dn/Gn), ∈nᐱ(Dn/Hn), ∈nᐱ(Dn/In), ∈nᐱ(Dn/Jn), ∈nᐱ(Dn/Kn), ∈nᐱ(Dn/Ln), ∈nᐱ(Dn/Mn), ∈nᐱ(Dn/Nn), ∈nᐱ(Dn/On), ∈nᐱ(Dn/Pn), ∈nᐱ(Dn/Qn), ∈nᐱ(Dn/Rn), ∈nᐱ(Dn/Sn), ∈nᐱ(Dn/Tn),∈nᐱ(Dn/Un),  ∈nᐱ(Dn/Vn), ∈nᐱ(Dn/Wn), ∈nᐱ(Dn/Yn), ∈nᐱ(Dn/Zn), ∈nᐱ(Dnn), ∈nᐱ(Dnn)

nᐱ(En/An), ∈nᐱ(En/Bn), ∈nᐱ(En/Dn), ∈nᐱ(En/En), ∈nᐱ(En/Fn), ∈nᐱ(En/Gn), ∈nᐱ(En/Hn), ∈nᐱ(En/In), ∈nᐱ(En/Jn), ∈nᐱ(En/Kn), ∈nᐱ(En/Ln), ∈nᐱ(En/Mn), ∈nᐱ(En/Nn), ∈nᐱ(En/On), ∈nᐱ(En/Pn), ∈nᐱ(En/Qn), ∈nᐱ(En/Rn), ∈nᐱ(En/Sn), ∈nᐱ(En/Tn),∈nᐱ(En/Un),  ∈nᐱ(En/Vn), ∈nᐱ(En/Wn), ∈nᐱ(En/Yn), ∈nᐱ(En/Zn), ∈nᐱ(Enn), ∈nᐱ(Enn)

nᐱ(Fn/An), ∈nᐱ(Fn/Bn), ∈nᐱ(Fn/Dn), ∈nᐱ(Fn/En), ∈nᐱ(Fn/Fn), ∈nᐱ(Fn/Gn), ∈nᐱ(Fn/Hn), ∈nᐱ(Fn/In), ∈nᐱ(Fn/Jn), ∈nᐱ(Fn/Kn), ∈nᐱ(Fn/Ln), ∈nᐱ(Fn/Mn), ∈nᐱ(Fn/Nn), ∈nᐱ(Fn/On), ∈nᐱ(Fn/Pn), ∈nᐱ(Fn/Qn), ∈nᐱ(Fn/Rn), ∈nᐱ(Fn/Sn), ∈nᐱ(Fn/Tn),∈nᐱ(Fn/Un),  ∈nᐱ(Fn/Vn), ∈nᐱ(Fn/Wn), ∈nᐱ(Fn/Yn), ∈nᐱ(Fn/Zn), ∈nᐱ(Fnn), ∈nᐱ(Fnn)

nᐱ(Gn/An), ∈nᐱ(Gn/Bn), ∈nᐱ(Gn/Dn), ∈nᐱ(Gn/En), ∈nᐱ(Gn/Fn), ∈nᐱ(Gn/Gn), ∈nᐱ(Gn/Hn), ∈nᐱ(Gn/In), ∈nᐱ(Gn/Jn), ∈nᐱ(Gn/Kn), ∈nᐱ(Gn/Ln), ∈nᐱ(Gn/Mn), ∈nᐱ(Gn/Nn), ∈nᐱ(Gn/On), ∈nᐱ(Gn/Pn), ∈nᐱ(Gn/Qn), ∈nᐱ(Gn/Rn), ∈nᐱ(Gn/Sn), ∈nᐱ(Gn/Tn),∈nᐱ(Gn/Un),  ∈nᐱ(Gn/Vn), ∈nᐱ(Gn/Wn), ∈nᐱ(Gn/Yn), ∈nᐱ(Gn/Zn), ∈nᐱ(Gnn), ∈nᐱ(Gnn)

nᐱ(Hn/An), ∈nᐱ(Hn/Bn), ∈nᐱ(Hn/Dn), ∈nᐱ(Hn/En), ∈nᐱ(Hn/Fn), ∈nᐱ(Hn/Gn), ∈nᐱ(Hn/Hn), ∈nᐱ(Hn/In), ∈nᐱ(Hn/Jn), ∈nᐱ(Hn/Kn), ∈nᐱ(Hn/Ln), ∈nᐱ(Hn/Mn), ∈nᐱ(Hn/Nn), ∈nᐱ(Hn/On), ∈nᐱ(Hn/Pn), ∈nᐱ(Hn/Qn), ∈nᐱ(Hn/Rn), ∈nᐱ(Hn/Sn), ∈nᐱ(Hn/Tn),∈nᐱ(Hn/Un),  ∈nᐱ(Hn/Vn), ∈nᐱ(Hn/Wn), ∈nᐱ(Hn/Yn), ∈nᐱ(Hn/Zn), ∈nᐱ(Hnn), ∈nᐱ(Hnn)

nᐱ(In/An), ∈nᐱ(In/Bn), ∈nᐱ(In/Dn), ∈nᐱ(In/En), ∈nᐱ(In/Fn), ∈nᐱ(In/Gn), ∈nᐱ(In/Hn), ∈nᐱ(In/In), ∈nᐱ(In/Jn), ∈nᐱ(In/Kn), ∈nᐱ(In/Ln), ∈nᐱ(In/Mn), ∈nᐱ(In/Nn), ∈nᐱ(In/On), ∈nᐱ(In/Pn), ∈nᐱ(In/Qn), ∈nᐱ(In/Rn), ∈nᐱ(In/Sn), ∈nᐱ(In/Tn),∈nᐱ(In/Un),  ∈nᐱ(In/Vn), ∈nᐱ(In/Wn), ∈nᐱ(In/Yn), ∈nᐱ(In/Zn), ∈nᐱ(Inn), ∈nᐱ(Inn)

nᐱ(Jn/An), ∈nᐱ(Jn/Bn), ∈nᐱ(Jn/Dn), ∈nᐱ(Jn/En), ∈nᐱ(Jn/Fn), ∈nᐱ(Jn/Gn), ∈nᐱ(Jn/Hn), ∈nᐱ(Jn/In), ∈nᐱ(Jn/Jn), ∈nᐱ(Jn/Kn), ∈nᐱ(Jn/Ln), ∈nᐱ(Jn/Mn), ∈nᐱ(Jn/Nn), ∈nᐱ(Jn/On), ∈nᐱ(Jn/Pn), ∈nᐱ(Jn/Qn), ∈nᐱ(Jn/Rn), ∈nᐱ(Jn/Sn), ∈nᐱ(Jn/Tn),∈nᐱ(Jn/Un),  ∈nᐱ(Jn/Vn), ∈nᐱ(Jn/Wn), ∈nᐱ(Jn/Yn), ∈nᐱ(Jn/Zn), ∈nᐱ(Jnn), ∈nᐱ(Jnn)

nᐱ(Kn/An), ∈nᐱ(Kn/Bn), ∈nᐱ(Kn/Dn), ∈nᐱ(Kn/En), ∈nᐱ(Kn/Fn), ∈nᐱ(Kn/Gn), ∈nᐱ(Kn/Hn), ∈nᐱ(Kn/In), ∈nᐱ(Kn/Jn), ∈nᐱ(Kn/Kn), ∈nᐱ(Kn/Ln), ∈nᐱ(Kn/Mn), ∈nᐱ(Kn/Nn), ∈nᐱ(Kn/On), ∈nᐱ(Kn/Pn), ∈nᐱ(Kn/Qn), ∈nᐱ(Kn/Rn), ∈nᐱ(Kn/Sn), ∈nᐱ(Kn/Tn),∈nᐱ(Kn/Un),  ∈nᐱ(Kn/Vn), ∈nᐱ(Kn/Wn), ∈nᐱ(Kn/Yn), ∈nᐱ(Kn/Zn), ∈nᐱ(Knn), ∈nᐱ(Knn)

nᐱ(Ln/An), ∈nᐱ(Ln/Bn), ∈nᐱ(Ln/Dn), ∈nᐱ(Ln/En), ∈nᐱ(Ln/Fn), ∈nᐱ(Ln/Gn), ∈nᐱ(Ln/Hn), ∈nᐱ(Ln/In), ∈nᐱ(Ln/Jn), ∈nᐱ(Ln/Kn), ∈nᐱ(Ln/Ln), ∈nᐱ(Ln/Mn), ∈nᐱ(Ln/Nn), ∈nᐱ(Ln/On), ∈nᐱ(Ln/Pn), ∈nᐱ(Ln/Qn), ∈nᐱ(Ln/Rn), ∈nᐱ(Ln/Sn), ∈nᐱ(Ln/Tn),∈nᐱ(Ln/Un),  ∈nᐱ(Ln/Vn), ∈nᐱ(Ln/Wn), ∈nᐱ(Ln/Yn), ∈nᐱ(Ln/Zn), ∈nᐱ(Lnn), ∈nᐱ(Lnn)

nᐱ(Mn/An), ∈nᐱ(Mn/Bn), ∈nᐱ(Mn/Dn), ∈nᐱ(Mn/En), ∈nᐱ(Mn/Fn), ∈nᐱ(Mn/Gn), ∈nᐱ(Mn/Hn), ∈nᐱ(Mn/In), ∈nᐱ(Mn/Jn), ∈nᐱ(Mn/Kn), ∈nᐱ(Mn/Ln), ∈nᐱ(Mn/Mn), ∈nᐱ(Mn/Nn), ∈nᐱ(Mn/On), ∈nᐱ(Mn/Pn), ∈nᐱ(Mn/Qn), ∈nᐱ(Mn/Rn), ∈nᐱ(Mn/Sn), ∈nᐱ(Mn/Tn),∈nᐱ(Mn/Un),  ∈nᐱ(Mn/Vn), ∈nᐱ(Mn/Wn), ∈nᐱ(Mn/Yn), ∈nᐱ(Mn/Zn), ∈nᐱ(Mnn), ∈nᐱ(Mnn)

nᐱ(Nn/An), ∈nᐱ(Nn/Bn), ∈nᐱ(Nn/Dn), ∈nᐱ(Nn/En), ∈nᐱ(Nn/Fn), ∈nᐱ(Nn/Gn), ∈nᐱ(Nn/Hn), ∈nᐱ(Nn/In), ∈nᐱ(Nn/Jn), ∈nᐱ(Nn/Kn), ∈nᐱ(Nn/Ln), ∈nᐱ(Nn/Mn), ∈nᐱ(Nn/Nn), ∈nᐱ(Nn/On), ∈nᐱ(Nn/Pn), ∈nᐱ(Nn/Qn), ∈nᐱ(Nn/Rn), ∈nᐱ(Nn/Sn), ∈nᐱ(Nn/Tn),∈nᐱ(Nn/Un),  ∈nᐱ(Nn/Vn), ∈nᐱ(Nn/Wn), ∈nᐱ(Nn/Yn), ∈nᐱ(Nn/Zn), ∈nᐱ(Nnn), ∈nᐱ(Nnn)

nᐱ(On/An), ∈nᐱ(On/Bn), ∈nᐱ(On/Dn), ∈nᐱ(On/En), ∈nᐱ(On/Fn), ∈nᐱ(On/Gn), ∈nᐱ(On/Hn), ∈nᐱ(On/In), ∈nᐱ(On/Jn), ∈nᐱ(On/Kn), ∈nᐱ(On/Ln), ∈nᐱ(On/Mn), ∈nᐱ(On/Nn), ∈nᐱ(On/On), ∈nᐱ(On/Pn), ∈nᐱ(On/Qn), ∈nᐱ(On/Rn), ∈nᐱ(On/Sn), ∈nᐱ(On/Tn),∈nᐱ(On/Un),  ∈nᐱ(On/Vn), ∈nᐱ(On/Wn), ∈nᐱ(On/Yn), ∈nᐱ(On/Zn), ∈nᐱ(Onn), ∈nᐱ(Onn)

nᐱ(Pn/An), ∈nᐱ(Pn/Bn), ∈nᐱ(Pn/Dn), ∈nᐱ(Pn/En), ∈nᐱ(Pn/Fn), ∈nᐱ(Pn/Gn), ∈nᐱ(Pn/Hn), ∈nᐱ(Pn/In), ∈nᐱ(Pn/Jn), ∈nᐱ(Pn/Kn), ∈nᐱ(Pn/Ln), ∈nᐱ(Pn/Mn), ∈nᐱ(Pn/Nn), ∈nᐱ(Pn/On), ∈nᐱ(Pn/Pn), ∈nᐱ(Pn/Qn), ∈nᐱ(Pn/Rn), ∈nᐱ(Pn/Sn), ∈nᐱ(Pn/Tn),∈nᐱ(Pn/Un),  ∈nᐱ(Pn/Vn), ∈nᐱ(Pn/Wn), ∈nᐱ(Pn/Yn), ∈nᐱ(Pn/Zn), ∈nᐱ(Pnn), ∈nᐱ(Pnn)

nᐱ(Qn/An), ∈nᐱ(Qn/Bn), ∈nᐱ(Qn/Dn), ∈nᐱ(Qn/En), ∈nᐱ(Qn/Fn), ∈nᐱ(Qn/Gn), ∈nᐱ(Qn/Hn), ∈nᐱ(Qn/In), ∈nᐱ(Qn/Jn), ∈nᐱ(Qn/Kn), ∈nᐱ(Qn/Ln), ∈nᐱ(Qn/Mn), ∈nᐱ(Qn/Nn), ∈nᐱ(Qn/On), ∈nᐱ(Qn/Pn), ∈nᐱ(Qn/Qn), ∈nᐱ(Qn/Rn), ∈nᐱ(Qn/Sn), ∈nᐱ(Qn/Tn),∈nᐱ(Qn/Un),  ∈nᐱ(Qn/Vn), ∈nᐱ(Qn/Wn), ∈nᐱ(Qn/Yn), ∈nᐱ(Qn/Zn), ∈nᐱ(Qnn), ∈nᐱ(Qnn)

nᐱ(Rn/An), ∈nᐱ(Rn/Bn), ∈nᐱ(Rn/Dn), ∈nᐱ(Rn/En), ∈nᐱ(Rn/Fn), ∈nᐱ(Rn/Gn), ∈nᐱ(Rn/Hn), ∈nᐱ(Rn/In), ∈nᐱ(Rn/Jn), ∈nᐱ(Rn/Kn), ∈nᐱ(Rn/Ln), ∈nᐱ(Rn/Mn), ∈nᐱ(Rn/Nn), ∈nᐱ(Rn/On), ∈nᐱ(Rn/Pn), ∈nᐱ(Rn/Qn), ∈nᐱ(Rn/Rn), ∈nᐱ(Rn/Sn), ∈nᐱ(Rn/Tn),∈nᐱ(Rn/Un),  ∈nᐱ(Rn/Vn), ∈nᐱ(Rn/Wn), ∈nᐱ(Rn/Yn), ∈nᐱ(Rn/Zn), ∈nᐱ(Rnn), ∈nᐱ(Rnn)

nᐱ(Sn/An), ∈nᐱ(Sn/Bn), ∈nᐱ(Sn/Dn), ∈nᐱ(Sn/En), ∈nᐱ(Sn/Fn), ∈nᐱ(Sn/Gn), ∈nᐱ(Sn/Hn), ∈nᐱ(Sn/In), ∈nᐱ(Sn/Jn), ∈nᐱ(Sn/Kn), ∈nᐱ(Sn/Ln), ∈nᐱ(Sn/Mn), ∈nᐱ(Sn/Nn), ∈nᐱ(Sn/On), ∈nᐱ(Sn/Pn), ∈nᐱ(Sn/Qn), ∈nᐱ(Sn/Rn), ∈nᐱ(Sn/Sn), ∈nᐱ(Sn/Tn),∈nᐱ(Sn/Un),  ∈nᐱ(Sn/Vn), ∈nᐱ(Sn/Wn), ∈nᐱ(Sn/Yn), ∈nᐱ(Sn/Zn), ∈nᐱ(Snn), ∈nᐱ(Snn)

nᐱ(Tn/An), ∈nᐱ(Tn/Bn), ∈nᐱ(Tn/Dn), ∈nᐱ(Tn/En), ∈nᐱ(Tn/Fn), ∈nᐱ(Tn/Gn), ∈nᐱ(Tn/Hn), ∈nᐱ(Tn/In), ∈nᐱ(Tn/Jn), ∈nᐱ(Tn/Kn), ∈nᐱ(Tn/Ln), ∈nᐱ(Tn/Mn), ∈nᐱ(Tn/Nn), ∈nᐱ(Tn/On), ∈nᐱ(Tn/Pn), ∈nᐱ(Tn/Qn), ∈nᐱ(Tn/Rn), ∈nᐱ(Tn/Sn), ∈nᐱ(Tn/Tn),∈nᐱ(Tn/Un),  ∈nᐱ(Tn/Vn), ∈nᐱ(Tn/Wn), ∈nᐱ(Tn/Yn), ∈nᐱ(Tn/Zn), ∈nᐱ(Tnn), ∈nᐱ(Tnn)

nᐱ(Un/An), ∈nᐱ(Un/Bn), ∈nᐱ(Un/Dn), ∈nᐱ(Un/En), ∈nᐱ(Un/Fn), ∈nᐱ(Un/Gn), ∈nᐱ(Un/Hn), ∈nᐱ(Un/In), ∈nᐱ(Un/Jn), ∈nᐱ(Un/Kn), ∈nᐱ(Un/Ln), ∈nᐱ(Un/Mn), ∈nᐱ(Un/Nn), ∈nᐱ(Un/On), ∈nᐱ(Un/Pn), ∈nᐱ(Un/Qn), ∈nᐱ(Un/Rn), ∈nᐱ(Un/Sn), ∈nᐱ(Un/Tn),∈nᐱ(Un/Un),  ∈nᐱ(Un/Vn), ∈nᐱ(Un/Wn), ∈nᐱ(Un/Yn), ∈nᐱ(Un/Zn), ∈nᐱ(Unn), ∈nᐱ(Unn)

nᐱ(Vn/An), ∈nᐱ(Vn/Bn), ∈nᐱ(Vn/Dn), ∈nᐱ(Vn/En), ∈nᐱ(Vn/Fn), ∈nᐱ(Vn/Gn), ∈nᐱ(Vn/Hn), ∈nᐱ(Vn/In), ∈nᐱ(Vn/Jn), ∈nᐱ(Vn/Kn), ∈nᐱ(Vn/Ln), ∈nᐱ(Vn/Mn), ∈nᐱ(Vn/Nn), ∈nᐱ(Vn/On), ∈nᐱ(Vn/Pn), ∈nᐱ(Vn/Qn), ∈nᐱ(Vn/Rn), ∈nᐱ(Vn/Sn), ∈nᐱ(Vn/Tn),∈nᐱ(Vn/Un),  ∈nᐱ(Vn/Vn), ∈nᐱ(Vn/Wn), ∈nᐱ(Vn/Yn), ∈nᐱ(Vn/Zn), ∈nᐱ(Vnn), ∈nᐱ(Vnn)

nᐱ(Wn/An), ∈nᐱ(Wn/Bn), ∈nᐱ(Wn/Dn), ∈nᐱ(Wn/En), ∈nᐱ(Wn/Fn), ∈nᐱ(Wn/Gn), ∈nᐱ(Wn/Hn), ∈nᐱ(Wn/In), ∈nᐱ(Wn/Jn), ∈nᐱ(Wn/Kn), ∈nᐱ(Wn/Ln), ∈nᐱ(Wn/Mn), ∈nᐱ(Wn/Nn), ∈nᐱ(Wn/On), ∈nᐱ(Wn/Pn), ∈nᐱ(Wn/Qn), ∈nᐱ(Wn/Rn), ∈nᐱ(Wn/Sn), ∈nᐱ(Wn/Tn),∈nᐱ(Wn/Un),  ∈nᐱ(Wn/Vn), ∈nᐱ(Wn/Wn), ∈nᐱ(Wn/Yn), ∈nᐱ(Wn/Zn), ∈nᐱ(Wnn), ∈nᐱ(Wnn)

nᐱ(Yn/An), ∈nᐱ(Yn/Bn), ∈nᐱ(Yn/Dn), ∈nᐱ(Yn/En), ∈nᐱ(Yn/Fn), ∈nᐱ(Yn/Gn), ∈nᐱ(Yn/Hn), ∈nᐱ(Yn/In), ∈nᐱ(Yn/Jn), ∈nᐱ(Yn/Kn), ∈nᐱ(Yn/Ln), ∈nᐱ(Yn/Mn), ∈nᐱ(Yn/Nn), ∈nᐱ(Yn/On), ∈nᐱ(Yn/Pn), ∈nᐱ(Yn/Qn), ∈nᐱ(Yn/Rn), ∈nᐱ(Yn/Sn), ∈nᐱ(Yn/Tn),∈nᐱ(Yn/Un),  ∈nᐱ(Yn/Vn), ∈nᐱ(Yn/Wn), ∈nᐱ(Yn/Yn), ∈nᐱ(Yn/Zn), ∈nᐱ(Ynn), ∈nᐱ(Ynn)

nᐱ(Zn/An), ∈nᐱ(Zn/Bn), ∈nᐱ(Zn/Dn), ∈nᐱ(Zn/En), ∈nᐱ(Zn/Fn), ∈nᐱ(Zn/Gn), ∈nᐱ(Zn/Hn), ∈nᐱ(Zn/In), ∈nᐱ(Zn/Jn), ∈nᐱ(Zn/Kn), ∈nᐱ(Zn/Ln), ∈nᐱ(Zn/Mn), ∈nᐱ(Zn/Nn), ∈nᐱ(Zn/On), ∈nᐱ(Zn/Pn), ∈nᐱ(Zn/Qn), ∈nᐱ(Zn/Rn), ∈nᐱ(Zn/Sn), ∈nᐱ(Zn/Tn),∈nᐱ(Zn/Un),  ∈nᐱ(Zn/Vn), ∈nᐱ(Zn/Wn), ∈nᐱ(Zn/Yn), ∈nᐱ(Zn/Zn), ∈nᐱ(Znn), ∈nᐱ(Znn)

nᐱ(φn/An), ∈nᐱ(φn/Bn), ∈nᐱ(φn/Dn), ∈nᐱ(φn/En), ∈nᐱ(φn/Fn), ∈nᐱ(φn/Gn), ∈nᐱ(φn/Hn), ∈nᐱ(φn/In), ∈nᐱ(φn/Jn), ∈nᐱ(φn/Kn), ∈nᐱ(φn/Ln), ∈nᐱ(φn/Mn), ∈nᐱ(φn/Nn), ∈nᐱ(φn/On), ∈nᐱ(φn/Pn), ∈nᐱ(φn/Qn), ∈nᐱ(φn/Rn), ∈nᐱ(φn/Sn), ∈nᐱ(φn/Tn),∈nᐱ(φn/Un),  ∈nᐱ(φn/Vn), ∈nᐱ(φn/Wn), ∈nᐱ(φn/Yn), ∈nᐱ(φn/Zn), ∈nᐱ(φnn), ∈nᐱ(φnn)

nᐱ(Θn/An), ∈nᐱ(Θn/Bn), ∈nᐱ(Θn/Dn), ∈nᐱ(Θn/En), ∈nᐱ(Θn/Fn), ∈nᐱ(Θn/Gn), ∈nᐱ(Θn/Hn), ∈nᐱ(Θn/In), ∈nᐱ(Θn/Jn), ∈nᐱ(Θn/Kn), ∈nᐱ(Θn/Ln), ∈nᐱ(Θn/Mn), ∈nᐱ(Θn/Nn), ∈nᐱ(Θn/On), ∈nᐱ(Θn/Pn), ∈nᐱ(Θn/Qn), ∈nᐱ(Θn/Rn), ∈nᐱ(Θn/Sn), ∈nᐱ(Θn/Tn),∈nᐱ(Θn/Un),  ∈nᐱ(Θn/Vn), ∈nᐱ(Θn/Wn), ∈nᐱ(Θn/Yn), ∈nᐱ(Θn/Zn), ∈nᐱ(Θnn), ∈nᐱ(Θnn)

With 27 base sets to each set of ᐱ have 1⅄, 2⅄, 3⅄ paths occur with infinite library potential each that then 81 basic sets have other potential functions of X, 1+⅄, 1-⅄, 2-⅄, n from Y, P, N, whole number fractals in quantum field fractal polarization.

27 libraries multiplied by 8 basic function potentials multiplied by 27 library variables equals 5832 base libraries each with infinite numeral library stacking to infinite variables more give infinite cycles of a cn in those ratios. 

5,832 library base paths of 27 sets ᐱ with 8 functions applicable to  1⅄, 2⅄, 3⅄, X, 1+⅄, 1-⅄, 2-⅄, n , 3 libraries that all 5,832 libraries align to are ᐱ of (N) and ᐱ of (Y) and ᐱ of (P).

ᐱ of (P) is a function of a complex ratio with a prime number.

ᐱ of (Y) is a function of a complex ratio with a fibonacci number.

ᐱ of (N) is a function of a complex ratio with a number.

This library is a base logic of sets ᐱ prior to factoring variable sets for a library of (ᗑ) variables.

Another array of libraries are factorable of variables such as 2φ from 11φ for example to all sets and paths of the 5,832 library bases and more just as are array sets of variant paths for 3φ from 12φ and so on for all sets ᐱ of A,B,D,E,F,G,H,I,J,K,L,M,N,O,P,Q,R,S,T,U,V,W,X,Y,Z,φ variables and paths 1⅄, 2⅄, 3⅄, X, 1+⅄, 1-⅄, 2-⅄, n and so on.

Then a set of ᐱ of (Ψ) included to such a library creates even more base libraries with their relations to A through Z Phi and Theta sets accountable for path variations and cn variants.


Numeral Array logic symbols to use of next tier alt paths and stem cell cycle notations 

ᗑ for (⅄ᗑ )

ᗑ=(ᐱ/ᐱ) for paths 1⅄, 2⅄, and 3⅄ of ᗑ variables

(ᗑ)=1(⅄ᗑ) and 2(⅄ᗑ) and 3(⅄ᗑ) of variables ⅄ᐱ, ⅄A , ⅄M, ⅄V, ⅄W, A, M, V, W, φ, Θ, Q, Y, P  and whole numbers or a variable factors noted that (ᐱ) is applicable with in quanta such that (ᗑ)=(ᐱ/ᐱ) variables defined before a variable 

nncn=(⅄)(ncn)ncn 

or 

nncn=(⅄)(ncn)ncn 

⅄ represents alternate path factoring of the variables 1⅄, 2⅄, 3ncn.

1ᗑ=(ᐱn2/ᐱn1) and 2ᗑ=(ᐱn1/ᐱn2) and 3ᗑ=(ᐱncn/ᐱncn) are depending an accuracy of decimal stem variant notation to variable factoring precision noted with Nncn that ᐱ or N is a number and n1 is a numerated variable in a set of ᐱ and the numerated ordinal ratio of that set to a number of cycles in that complex ratio defined with a whole number of cycles or a percent of whole and partial cycles using the decimal variant stem.

n10c10.33 variant for example is a notation of a ratio of a set label of the 10th number of a undefined set in ᗑ with 10 whole cycles of the variant decimal stem and one third of that decimal stem totaling 10 and 33% of that decimal stem cycle and no more.

As the numbers of a stem variant in decimal ratios can be counted, then the variables can be noted to a definition of that number variation potential to a notation. If a specific number of decimal stem variant is to be noted differently, it should be noted as different notation so not to be confused as that many cycles of a stem decimal repeatable cycle and only digits of that decimal stem.

See Page  


refers to all or for any and when applied with notation for path of consecutive variables of sets ∈ and variables of not same sets ∉.

Given ∀ represents for any and ⅄ represents a function of sequential variables of sets ∈ variable number N or n.

Then

12nd=(n3/n1)

22nd=(n1/n3)

and

13rd=(n4/n1)

23rd=(n1/n4)

and so on for functions of 1∀ and 2∀ variables.

Path functions +⅄, 1-⅄, 2-⅄, and X of function to set ∈ consecutive variables Nncn

+⅄then are

+⅄2nd=(n3+n1)

+⅄2nd=(n1+n3)

and

+⅄3rd=(n4+n1)

+⅄3rd=(n1+n4)

and so on for functions of +⅄∀ variables.

1-⅄then are

1-⅄2nd=(n3-n1)

and

1-⅄3rd=(n4-n1)

and so on for functions of 1-⅄∀ variables.

2-⅄then are

2-⅄2nd=(n1-n3)

and

2-⅄3rd=(n1-n4)

and so on for functions of 2-⅄∀ variables.

Xthen are

X2nd=(n3xn1)

X2nd=(n1xn3)

and

X3rd=(n4xn1)

X3rd=(n1xn4)

and so on for functions of X∀ variables.


Practical application of (for all, for any 12nd) added in combination notation for variables of sets.

if 12nd=(n3/n1) then 1∀Y2nd=(Y3/Y1) is not φ=(Yn2/Yn1) and 1∀P2nd=(P3/P1) is not 1Q=(Pn2/Pn1).

If plotted points on a graph are visual lines connecting the numbers, a web of lines then forms an arc of the crossing lines and so instead, precise equations can be formulated for exact numbers and quotients, products, sums, and differences from this for all for any formula combination, rather than trying to guess or estimate what the crossing in the web numeral representation line graph factors are from a visual representation. ≠


Since 1∀Y2nd=(Y3/Y1) and is not φ=(Yn2/Yn1) it is 1∀Y2nd a variable from path division of factors from ordinal consecutive Y base of which the second ordinal from the divisor is the denominator.

So values for an ordinal consecutive set 1∀Y2ndφ and 1∀P2nd1Q

1∀Y2nd=(Y3/Y1)≠φ 1Q

Although the (for all for any ∀) set is a quotient producing factor path the variables of sets φ and 1Q are applicable to a function for entirely different library sets for 1φ2nd=(φn3/φn1) and 1(1Q)2nd=(1Qn3/1Qn1) after the variables are factored complete notable quotients for sets φ and 1Q. 

(Functions for all for any ∀) are then applicable in combination with variables from all sets A  B  C  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ following the factored definitions of each set base.

A computer can print out such combinatorial sequence equation answers, yet if the reader can not comprehend what the computer is printing out from such an equation then the reader is dependent of a computer the reader has no idea of what they are reading. If the computer is limited and the reader can not comprehend the computer print out, it is highly probable the reader has no idea nor comprehends the computers limits and will have no idea.


When a reader is relying on something such as DNA and RNA sequencing and a computer default is to print out basic complex quotients rooted to computer shell structures of basic prime and consecutive Y numeral algorithms, the DNA RNA sequence reader will certainly not be aware of what they have been reading.


To Begin  1∀Y2nd=(Y3/Y1)

1st tier fibonacci 01 to 10 digit value for basic numerical display of decimal precision laws not applicable to standard definition floating point. 9 bold numbers are also prime numbers in the ten digit base logic that prime fibonacci scale bases share in common of the ten digit example shown below. 2 - 3- 5 - 13- 89 - 1597 - 28657 - 514229 - 434894437

0  1  1  2  3  5  8  13  21  34  55  89  144  233  377  610  987  1597  2584  4181  6765  10946  17711  28657  46368  75025  121393  196418  317811  514229  832040  1346296  2178309  3524578  5702887  9227465  14930352  24157817  39088169  63245986  102334155  165780141  269114296  434894437  704008733  1138903170


After factoring quotients for sets φ and 1Q from Y base and P base then

if 12nd=(n3/n1) of (Nn) then

(Nn1)1∀Y2nd=(Yn3/Yn1)=(1/0)=0

(Nn2)1∀Y2nd=(Yn4/Yn2)=(2/1)=2

(Nn3)1∀Y2nd=(Yn5/Yn3)=(3/1)=3

(Nn4)1∀Y2nd=(Yn6/Yn4)=(5/2)=2.5

(Nn5)1∀Y2nd=(Yn7/Yn5)=(8/3)=2.^6 or 2.6

(Nn6)1∀Y2nd=(Yn8/Yn6)=(13/5)=2.6

(Nn7)1∀Y2nd=(Yn9/Yn7)=(21/8)=2.625

(Nn8)1∀Y2nd=(Yn10/Yn8)=(34/13)=2.^615384 (a path  number bridge example) or 2.615384

(Nn9)1∀Y2nd=(Yn11/Yn9)=(55/21)=2.^619047 (a path  number bridge example) or 2.619047

(Nn10)1∀Y2nd=(Yn12/Yn10)=(89/34)=2.6^1764705882352941 or 2.61764705882352941

(Nn11)1∀Y2nd=(Yn13/Yn11)=(144/55)=2.6^18 or 2.618

(Nn12)1∀Y2nd=(Yn14/Yn12)=(233/89)=2.^61797752808988764044943820224719101123595505 or 2.61797752808988764044943820224719101123595505

(Nn13)1∀Y2nd=(Yn15/Yn13)=(377/144)=2.6180^5 or 2.61805

(Nn14)1∀Y2nd=(Yn16/Yn14)=(610/233)=^2.618025751072961373390557939914163090128755364806866952789699570815450643776824034334763948497854077253218884120171673819742489270386266094420600858369098712446351931330472103004291845493562231759656652360515021459227467811158798283 

or 

2.6180257510729613733905579399141630901287553648068669527896995708154506437768240343347639484978540772532188841201716738197424892703862660944206008583690987124463519313304721030042918454935622317596566523605150214592274678111587982832618025751072961373390557939914163090128755364806866952789699570815450643776824034334763948497854077253218884120171673819742489270386266094420600858369098712446351931330472103004291845493562231759656652360515021459227467811158798283

(Nn15)1∀Y2nd=(Yn17/Yn15)=(987/377)=2.^618037135278514588859416445623342175066312997347480106100795755968169761273209549071 or 2.618037135278514588859416445623342175066312997347480106100795755968169761273209549071

(Nn16)1∀Y2nd=(Yn18/Yn16)=(1597/610)=2.6^180327868852459016393442622950819672131147540983606557377049 or 2.6180327868852459016393442622950819672131147540983606557377049

(Nn17)1∀Y2nd=(Yn19/Yn17)=(2584/987)=2.^618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745694022289766970 

or 

2.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745694022289766970

(Nn18)1∀Y2nd=(Yn20/Yn18)=(4181/1597)=2.^6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129 

or 

2.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129

(Nn19)1∀Y2nd=(Yn21/Yn19)=(6765/2584)=2.618^034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743

or

2.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743

(Nn20)1∀Y2nd=(Yn22/Yn20)=(10946/4181)=2.^618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936

or

2.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936

(Nn21)1∀Y2nd=(Yn23/Yn21)=(17711/6765)=2.61^803399852

or

2.61803399852

(Nn22)1∀Y2nd=(Yn24/Yn22)=(28657/10946)=2.6^180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981

or

2.6180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981

(Nn23)1∀Y2nd=(Yn25/Yn23)=(46368/17711)=2.^618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114

or

2.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114

(Nn24)1∀Y2nd=(Yn26/Yn24)=(75025/28657)=2.^61803398820532505147084481976480441078968489374323899919740377569180304986565237114841051052098963604006002023938304777192309034441846669225669120982656942457340265903618662106989566249083993439648253480824929336636772865268520780263111979621035000174477440066999336985727745402519454234567470426073908643612380919147154272952507240813762780472484907701434204557350734550022682067208709913808144606902327529050493771155389608123669609519489130055483825941305789161461423038001186446592455595491502948668737132288795058798897302578776564190250200649056077049237533586907212897372369752590989984994940154238057019227413895383326935827197543357643856649335240953344732526084377290016400879366297937676658408067836828698049342220050947412499563806399832501657535680636493701364413581323934815228390969047702132114317618731897965593048818787730746414488606623163624943294831978225215479638482744181177373765572111525979690825976201277174861290435146735527096346442404997033883518861011271242628328157169278012353002756743553058589524374498377359807376906166032731967756569075618522525037512649614404857451931465261541682660432006141605890358376661897616638168684789056774958997801584255155808353979830407928254876644449872631468751090484000418745856160798408765746588966046690162961929022577380744669714205953170255086017377953030673133963778483442090937641762920054436961300903793139547056565586069721185050772935059496807062846773912133161182259133893987507415291202847471821893429179607076804969117493108141117353526189063754056600481557734584918170080608577310953693687406218375963987856370171336846145793348919984645985274104058345255958404578288027358062602505496039362110479115050423980179362808388875318421328122273789998953135359598003978085633527584883274592595177443556548138325714485117074362284956555117423317165090553791394772655895592699863907596747740517151132358586034825697037373067662351257982342883065219667097044352165265031231461771992881320445266427050982307987577206267229647206616184527340614858498796105663537704574798478556722615765781484454060090030359074571657884635516627700038385036814739854136860103988554279931604843493736259901594723802212373940049551592979027811703946679694315525002617161601004990054785916181037791813518512056391108629654185713787207314094287608612206441707087273615521513068360261018250340231008130648707122169103534912935757406567330844121855044142792336950832257389119586837421921345570017796698886833932372544230031056984331925881983459538681648462853753009735841155738563003803608193460585546288864849774924102313570855288411208430749904037407963150364657849740028614300170987891265659350246013190494469065149876121017552430470740133300764211187493457095997487524863035209547405520466203719859022228425864535715531981714764280978469483895732281815961196217329099347454374149422479673378232194577241162717660606483581672889695362389643019157622919356527201032906445196636074955508252782915169068639424922357539170185295041351153295878842865617475660397110653592490490979516348536134277837875562689744216072861778971978923125239906480092124088355375649928464249572530271835851624384967023763827337125309697456118923823149666748089472031266357260006281187842411976131486198834490700352444428935338660711170045713089297553826290260669295460097009456677251631364064626443800816554419513556897093205848483791045817775761594025892452105942701608681997417733887008409812611229368042712077328401437694106152074536762396622116760302892835956310849007223366018773772551209128659664305405311093275639459817845552570052692186900233799769689779111560875178839376068674320410370939037582440590431657186725756359702690442125833129776319921834106849984297030393970059671284502913773249118888927661653348222074885717276756115434274348326761349757476358306870921589838433890497958613951216107757266985378790522385455560596014935268869735143245978295006455665282478975468471926579893219806678996405764734619813658094008444708099242767910109222877481941584953065568621977178350839236486722266810901350455386118574868269532749415500575775552221097812052901559828314198974072652406043898523920857033185609100743273894685417175559200195414732875039257424015074850821788742715566877202777680845866629444812785706808109711414314129183096625606309104232822696025403915273755103465121959730606832536553023694036361098509962661827825662141885054262483860836793802561328820183550266950483302508985588163450465854764978888229751893080224726942806295146037617336078445057054122901908783194332972746623861534703562829326168126461248560561119447255469867746100429214502564818368984890253690197857417035977248141815263286457061101999511463167812401856439962312872945528143211082806993055797885333426387968035732979725721464214677042258435984227239417943259936490211815612241337195100673482918658617440764909097253725093345430435844645287364343790347908015493596677949541124332623791743727536029591373835363087552779425620267299438182642984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or

2.618033988205325051470844819764804410789684893743238999197403775691803049865652371148410510520989636040060020239383047771923090344418466692256691209826569424573402659036186621069895662490839934396482534808249293366367728652685207802631119796210350001744774400669993369857277454025194542345674704260739086436123809191471542729525072408137627804724849077014342045573507345500226820672087099138081446069023275290504937711553896081236696095194891300554838259413057891614614230380011864465924555954915029486687371322887950587988973025787765641902502006490560770492375335869072128973723697525909899849949401542380570192274138953833269358271975433576438566493352409533447325260843772900164008793662979376766584080678368286980493422200509474124995638063998325016575356806364937013644135813239348152283909690477021321143176187318979655930488187877307464144886066231636249432948319782252154796384827441811773737655721115259796908259762012771748612904351467355270963464424049970338835188610112712426283281571692780123530027567435530585895243744983773598073769061660327319677565690756185225250375126496144048574519314652615416826604320061416058903583766618976166381686847890567749589978015842551558083539798304079282548766444498726314687510904840004187458561607984087657465889660466901629619290225773807446697142059531702550860173779530306731339637784834420909376417629200544369613009037931395470565655860697211850507729350594968070628467739121331611822591338939875074152912028474718218934291796070768049691174931081411173535261890637540566004815577345849181700806085773109536936874062183759639878563701713368461457933489199846459852741040583452559584045782880273580626025054960393621104791150504239801793628083888753184213281222737899989531353595980039780856335275848832745925951774435565481383257144851170743622849565551174233171650905537913947726558955926998639075967477405171511323585860348256970373730676623512579823428830652196670970443521652650312314617719928813204452664270509823079875772062672296472066161845273406148584987961056635377045747984785567226157657814844540600900303590745716578846355166277000383850368147398541368601039885542799316048434937362599015947238022123739400495515929790278117039466796943155250026171616010049900547859161810377918135185120563911086296541857137872073140942876086122064417070872736155215130683602610182503402310081306487071221691035349129357574065673308441218550441427923369508322573891195868374219213455700177966988868339323725442300310569843319258819834595386816484628537530097358411557385630038036081934605855462888648497749241023135708552884112084307499040374079631503646578497400286143001709878912656593502460131904944690651498761210175524304707401333007642111874934570959974875248630352095474055204662037198590222284258645357155319817147642809784694838957322818159611962173290993474543741494224796733782321945772411627176606064835816728896953623896430191576229193565272010329064451966360749555082527829151690686394249223575391701852950413511532958788428656174756603971106535924904909795163485361342778378755626897442160728617789719789231252399064800921240883553756499284642495725302718358516243849670237638273371253096974561189238231496667480894720312663572600062811878424119761314861988344907003524444289353386607111700457130892975538262902606692954600970094566772516313640646264438008165544195135568970932058484837910458177757615940258924521059427016086819974177338870084098126112293680427120773284014376941061520745367623966221167603028928359563108490072233660187737725512091286596643054053110932756394598178455525700526921869002337997696897791115608751788393760686743204103709390375824405904316571867257563597026904421258331297763199218341068499842970303939700596712845029137732491188889276616533482220748857172767561154342743483267613497574763583068709215898384338904979586139512161077572669853787905223854555605960149352688697351432459782950064556652824789754684719265798932198066789964057647346198136580940084447080992427679101092228774819415849530655686219771783508392364867222668109013504553861185748682695327494155005757755522210978120529015598283141989740726524060438985239208570331856091007432738946854171755592001954147328750392574240150748508217887427155668772027776808458666294448127857068081097114143141291830966256063091042328226960254039152737551034651219597306068325365530236940363610985099626618278256621418850542624838608367938025613288201835502669504833025089855881634504658547649788882297518930802247269428062951460376173360784450570541229019087831943329727466238615347035628293261681264612485605611194472554698677461004292145025648183689848902536901978574170359772481418152632864570611019995114631678124018564399623128729455281432110828069930557978853334263879680357329797257214642146770422584359842272394179432599364902118156122413371951006734829186586174407649090972537250933454304358446452873643437903479080154935966779495411243326237917437275360295913738353630875527794256202672994381826429842621349059566598038873573646927452280420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(Nn25)1∀Y2nd=(Yn27/Yn25)=(121393/46368)=2.61803^398895790200138026224982746721877156659765355417529330572808833678398895790200138026224982746721877156659765355417529330572808833678

or

2.61803398895790200138026224982746721877156659765355417529330572808833678398895790200138026224982746721877156659765355417529330572808833678

(Nn26)1∀Y2nd=(Yn28/Yn26)=(196418/75025)=2.61^803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589

or

2.61803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589

(Nn27)1∀Y2nd=(Yn29/Yn27)=(317811/121393)=2.^6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575

or

2.6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575

(Nn28)1∀Y2nd=(Yn30/Yn28)=(514229/196418)=2.6^180339887383030068527324379639340589966296367949984217332423708621409443126393711370648311254569336822490810414524127116659369304238919040006516714354081601482552515553564337280697288435886731358633119164231384089034609862639880255373743750572758097526703255302467187324990581311285116435357248317363989043773992200307507458583225569957946827683817165432903298068405135985500310562168436701320652893319349550448533230152022727041309859585170401897993055626266431793420154975613233003085256952010508201895956582390615931330122493865124377602867354315795904652323106843568308403506806911790161797798572432261808999175228339561547312364447250252013562911749432333085562422995855776965451231557189259640155179260556568135303281776619250781496604180879552790477451150098259833620136647354112148581087273060513802197354621266889999898176338217474976835116944475557229989104868189269822521357513058884623608834220896251871009785253897300654726145261635898950198047022167011170055697542995041187671191031371870195195959637100469407080817440356790110885967681169750226557647466118176541864798541885163274241668278874644889979533443981712470343858505839587003227810078506043234326792860124835809345375678400146626072966836033357431599955197588815688989807451455569245181195206142003278721909397305745909234387887057194350823244305511714812288079503915119795538087140689753484914824506918917818122575324053803622885886222240324206539115559673756987648789825779714690099685364885091997678420511358429471840666334042704843751590994715351953486951297742569418281420236434542659023103788858454927756111965298496064515472105407854677269903980286939078903155515278640450467879725890702481442637640134814528200063130670305165514362227494425154517406754981722652710036758341903491533362522783044323839973933142583673594069789937785742650877210846256453074565467523343074463643861560549440478978505024997708967609893186978790131250700037674754859534258571006730544043824904031198769970165667097720168212689264731338268386807726379456057998757751326253194717388426722601798205867079391909091834760561659318392408027777494934272826319380097547067987658972191957967192416173670437536274679510024539502489588530582736816381390707572625726766385972772352839352808805710270952764003299086641753810750542210998991945748353002270667657750308016576892138195073771242961439379282957773727458786872893522996874013583276481788838090195399606960665519453410583551405675650907757944791210581514932440000407294647130100092659532222097771080043580527242920709914569947764461505564663116414992515960858984410797381095418953456404199207811911331955319777209828019835249315235874512519219216161451598122371676730238572839556456129275320999093769410135527293832540805832459346903033326884501420440081866224073150118624565976641651987088759685975827062692828559500656762618497286399413495708132655866570273600179209644737244040770194177723019275219175431986885112362410777016363062448451771222596707022777953140750847681984339520817847651437240986060340701972324328727509698703784785508456455111038703173843537761304972049404840696881141239601258540459632009286317954566282112637334663829180624993636021138592186052194809029722326874319054261829363907584844566180288975552138806015741938111578368581290920384078852243684387377938885438198128481096437190074229449439460741887199747477318779337942551090022299381930372980073109389159852966632386033866549908867822704640104267429665305623720840248857029396491156614974187701738129906627702145424553757802238084085979900009164129560427252084839474997199849300980561862965715973077823824700383875204920119337331609119327149242941074646926452769094482175768004968994694987221130446293109592807176531682432363632660957753362726430367888890020262908694722479609811728049364111232168131230335305318249854901281959901841990041645877669052734474437169709497092934456108910588642588764777158916188943986803653432984756997831156004032217006587990917329368998767933692431447219704915028154242482868168905090164852508425908012503945666894072844647639218401572157337922186357665794377297396368968220835157673940270239998370821411479599629361871111608915679825677891028317160341720208942153977741347534340029936156564062356810475618324186174383203168752354672178720891160687920659002739056501949923123135354193607510513293079045708641774175482898716003624922359457890824669836776670162612387866692461994318239672535103707399525501736093433392051644961256096691749228685761997372949526010854402346017167469376533718905599283161421051023836919223289107922899123298272052459550550356891934547750206192915109613171908888187436996609272062641916728609394251036055758637192110702685089961205184860857966174179555845187304625848954780111802380637212475435041594965838161471962854728181734871549450661344683277500025455915445631255791220763881110692502723782952682544369660621735278844097791444775937032247553686525674836318463684591025262450488244458247207486075614251239703082202242157032451201010090724882648229795639910802472278508079707562443360588133470455864533800364528709181439582930281338777505116639004571882414035373540103249193047480373489191418301784968791047663656080399963343481758290991660642100011200602796077752548137136107688704701198464499180319522650673563522691403028235701412294188923622071296927980124021220051115478214827561628771293873270270545469356168986549094278528444439918948365221110081560753087802543555071327475078658778727000580394872160392632039833416489323789062102251321162011628262175564357645429644940891364335244224052785386268060972008675375983871131973648036330682524004928265230274211121

or

2.6180339887383030068527324379639340589966296367949984217332423708621409443126393711370648311254569336822490810414524127116659369304238919040006516714354081601482552515553564337280697288435886731358633119164231384089034609862639880255373743750572758097526703255302467187324990581311285116435357248317363989043773992200307507458583225569957946827683817165432903298068405135985500310562168436701320652893319349550448533230152022727041309859585170401897993055626266431793420154975613233003085256952010508201895956582390615931330122493865124377602867354315795904652323106843568308403506806911790161797798572432261808999175228339561547312364447250252013562911749432333085562422995855776965451231557189259640155179260556568135303281776619250781496604180879552790477451150098259833620136647354112148581087273060513802197354621266889999898176338217474976835116944475557229989104868189269822521357513058884623608834220896251871009785253897300654726145261635898950198047022167011170055697542995041187671191031371870195195959637100469407080817440356790110885967681169750226557647466118176541864798541885163274241668278874644889979533443981712470343858505839587003227810078506043234326792860124835809345375678400146626072966836033357431599955197588815688989807451455569245181195206142003278721909397305745909234387887057194350823244305511714812288079503915119795538087140689753484914824506918917818122575324053803622885886222240324206539115559673756987648789825779714690099685364885091997678420511358429471840666334042704843751590994715351953486951297742569418281420236434542659023103788858454927756111965298496064515472105407854677269903980286939078903155515278640450467879725890702481442637640134814528200063130670305165514362227494425154517406754981722652710036758341903491533362522783044323839973933142583673594069789937785742650877210846256453074565467523343074463643861560549440478978505024997708967609893186978790131250700037674754859534258571006730544043824904031198769970165667097720168212689264731338268386807726379456057998757751326253194717388426722601798205867079391909091834760561659318392408027777494934272826319380097547067987658972191957967192416173670437536274679510024539502489588530582736816381390707572625726766385972772352839352808805710270952764003299086641753810750542210998991945748353002270667657750308016576892138195073771242961439379282957773727458786872893522996874013583276481788838090195399606960665519453410583551405675650907757944791210581514932440000407294647130100092659532222097771080043580527242920709914569947764461505564663116414992515960858984410797381095418953456404199207811911331955319777209828019835249315235874512519219216161451598122371676730238572839556456129275320999093769410135527293832540805832459346903033326884501420440081866224073150118624565976641651987088759685975827062692828559500656762618497286399413495708132655866570273600179209644737244040770194177723019275219175431986885112362410777016363062448451771222596707022777953140750847681984339520817847651437240986060340701972324328727509698703784785508456455111038703173843537761304972049404840696881141239601258540459632009286317954566282112637334663829180624993636021138592186052194809029722326874319054261829363907584844566180288975552138806015741938111578368581290920384078852243684387377938885438198128481096437190074229449439460741887199747477318779337942551090022299381930372980073109389159852966632386033866549908867822704640104267429665305623720840248857029396491156614974187701738129906627702145424553757802238084085979900009164129560427252084839474997199849300980561862965715973077823824700383875204920119337331609119327149242941074646926452769094482175768004968994694987221130446293109592807176531682432363632660957753362726430367888890020262908694722479609811728049364111232168131230335305318249854901281959901841990041645877669052734474437169709497092934456108910588642588764777158916188943986803653432984756997831156004032217006587990917329368998767933692431447219704915028154242482868168905090164852508425908012503945666894072844647639218401572157337922186357665794377297396368968220835157673940270239998370821411479599629361871111608915679825677891028317160341720208942153977741347534340029936156564062356810475618324186174383203168752354672178720891160687920659002739056501949923123135354193607510513293079045708641774175482898716003624922359457890824669836776670162612387866692461994318239672535103707399525501736093433392051644961256096691749228685761997372949526010854402346017167469376533718905599283161421051023836919223289107922899123298272052459550550356891934547750206192915109613171908888187436996609272062641916728609394251036055758637192110702685089961205184860857966174179555845187304625848954780111802380637212475435041594965838161471962854728181734871549450661344683277500025455915445631255791220763881110692502723782952682544369660621735278844097791444775937032247553686525674836318463684591025262450488244458247207486075614251239703082202242157032451201010090724882648229795639910802472278508079707562443360588133470455864533800364528709181439582930281338777505116639004571882414035373540103249193047480373489191418301784968791047663656080399963343481758290991660642100011200602796077752548137136107688704701198464499180319522650673563522691403028235701412294188923622071296927980124021220051115478214827561628771293873270270545469356168986549094278528444439918948365221110081560753087802543555071327475078658778727000580394872160392632039833416489323789062102251321162011628262175564357645429644940891364335244224052785386268060972008675375983871131973648036330682524004928265230274211121

(Nn29)1∀Y2nd=(Yn31/Yn29)=(832040/317811)=^2.61803398875432253760883040549257262964466302299165227131848803219523553306839599636

or

2.61803398875432253760883040549257262964466302299165227131848803219523553306839599636261803398875432253760883040549257262964466302299165227131848803219523553306839599636

(Nn30)1∀Y2nd=(Yn32/Yn30)=(1346296/514229)

(Nn31)1∀Y2nd=(Yn33/Yn31)=(2178309/832040)

(Nn32)1∀Y2nd=(Yn34/Yn32)=(3524578/1346269)

(Nn33)1∀Y2nd=(Yn35/Yn33)=(5702887/2178309)

(Nn34)1∀Y2nd=(Yn36/Yn34)=(9227465/3524578)

(Nn35)1∀Y2nd=(Yn37/Yn35)=(14930352/5702887)

(Nn36)1∀Y2nd=(Yn38/Yn36)=(24157817/9227465)

(Nn37)1∀Y2nd=(Yn39/Yn37)=(39088169/14930352)

(Nn38)1∀Y2nd=(Yn40/Yn38)=(63245986/24157817)

(Nn39)1∀Y2nd=(Yn41/Yn39)=(102334155/39088169)

(Nn40)1∀Y2nd=(Yn42/Yn40)=(165780141/63245986)

(Nn41)1∀Y2nd=(Yn43/Yn41)=(269114296/102334155)

(Nn42)1∀Y2nd=(Yn44/Yn42)=(434894437/165780141)

(Nn43)1∀Y2nd=(Yn45/Yn43)=(704008733/269114296)

(Nn44)1∀Y2nd=(Yn46/Yn44)=(1138903170/434894437)


Then if 22nd=(n1/n3) then 2∀Y2nd=(Yn1/Yn3) and where 0.333 is commonly occurring in estimations of rounded variables these quotients may be more suitable to precision of factoring more complex equations for correct answers.

(Nn1)2∀Y2nd=(Yn1/Yn3)=(0/1)=0

(Nn2)2∀Y2nd=(Yn2/Yn4)=(1/2)=0.5

(Nn3)2∀Y2nd=(Yn3/Yn5)=(1/3)=0.^3 or 0.33  or 0.333 and so on. . .

(Nn4)2∀Y2nd=(Yn4/Yn6)=(2/5)=0.4

(Nn5)2∀Y2nd=(Yn5/Yn7)=(3/8)=0.375

(Nn6)2∀Y2nd=(Yn6/Yn8)=(5/13)=0.^384615 or 0.384615

(Nn7)2∀Y2nd=(Yn7/Yn9)=(8/21)=0.^380952380952 or 0.380952380952

(Nn8)2∀Y2nd=(Yn8/Yn10)=(13/34)=0.3^8235294117647058 or 0.38235294117647058

(Nn9)2∀Y2nd=(Yn9/Yn11)=(21/55)=0.3^81 or 0.381

(Nn10)2∀Y2nd=(Yn10/Yn12)=(34/89)=0.^38202247191011235955056179775280898876404494 or 0.38202247191011235955056179775280898876404494

(Nn11)2∀Y2nd=(Yn11/Yn13)=(55/144)=0.3819^4 or 0.38194

(Nn12)2∀Y2nd=(Yn12/Yn14)=(89/233)=0.^3819742489270386266094420600858369098712446351931330472103004291845493562231759656652360515021459227467811158798283261802575107296137339055793991416309012875536480686695278969957081545064377682403433476394849785407725321888412017167

or

0.3819742489270386266094420600858369098712446351931330472103004291845493562231759656652360515021459227467811158798283261802575107296137339055793991416309012875536480686695278969957081545064377682403433476394849785407725321888412017167

(Nn13)2∀Y2nd=(Yn13/Yn15)=(144/377)=0.^381962864721485411140583554376657824933687002652519893899204244031830238726790450928

or

0.381962864721485411140583554376657824933687002652519893899204244031830238726790450928

(Nn14)2∀Y2nd=(Yn14/Yn16)=(233/610)=0.3^819672131147540983606557377049180327868852459016393442622950819672131147540983606557377049180327868852459016393442622950

or

0.3819672131147540983606557377049180327868852459016393442622950819672131147540983606557377049180327868852459016393442622950

(Nn15)2∀Y2nd=(Yn15/Yn17)=(377/987)=0.^381965552178318135764944275582573454913880445795339412360688956433637284701114488348530901722391084093211752786220871327254305977710233029

or

0.381965552178318135764944275582573454913880445795339412360688956433637284701114488348530901722391084093211752786220871327254305977710233029

(Nn16)2∀Y2nd=(Yn16/Yn18)=(610/1597)=0.^3819661865998747651847213525360050093926111458985597996242955541640576080150281778334376956793988728866624921728240450845335003130870

or

0.3819661865998747651847213525360050093926111458985597996242955541640576080150281778334376956793988728866624921728240450845335003130870

(Nn17)2∀Y2nd=(Yn17/Yn19)=(987/2584)=0.381^965944272445820433436532507739938080495356037151702786377708978328173374613003095975232198142414860681114551083591331269349845201238390092879256

or

0.381965944272445820433436532507739938080495356037151702786377708978328173374613003095975232198142414860681114551083591331269349845201238390092879256

(Nn18)2∀Y2nd=(Yn18/Yn20)=(1597/4181)=0.^381966036833293470461612054532408514709399665151877541258072231523558957187275771346567806744797895240373116479311169576656302320019134178426213824443912939488160727098780196125328868691700550107629753647452762497010284620904089930638603204974886390815594355417364266921789045682850992585505859842143027983735948337718249222674001435063

or

0.381966036833293470461612054532408514709399665151877541258072231523558957187275771346567806744797895240373116479311169576656302320019134178426213824443912939488160727098780196125328868691700550107629753647452762497010284620904089930638603204974886390815594355417364266921789045682850992585505859842143027983735948337718249222674001435063

(Nn19)2∀Y2nd=(Yn19/Yn21)=(2584/6765)=0.3^8196600147 or 0.38196600147

(Nn20)2∀Y2nd=(Yn20/Yn22)=(4181/10946)=0.3^819660149826420610268591266215969303855289603508130824045313356477251964187831171204092819294719532249223460624885803033071441622510506120957427370729033436871916681892928923807783665265850539009683902795541750411109080942810158962177964553261465375479627261099945185455874291978805042938059565137949936049698520007308605883427736159327608258724648273341860040197332358852548876301845422985565503380230221085327973689018

or

0.3819660149826420610268591266215969303855289603508130824045313356477251964187831171204092819294719532249223460624885803033071441622510506120957427370729033436871916681892928923807783665265850539009683902795541750411109080942810158962177964553261465375479627261099945185455874291978805042938059565137949936049698520007308605883427736159327608258724648273341860040197332358852548876301845422985565503380230221085327973689018

(Nn21)2∀Y2nd=(Yn21/Yn23)=(6765/17711)=0.^381966009824402913443622607419118062221218451809609846987747727401050194794195697589068940206651233696572751397436621308791146744960758850431934955677262718084806052735588052622663881203771667325390999943537914290553893060809666309073457173507989385127886624131895432217266105809948619502004404042685336796341256846027892270340466376827960024843317712156287053243746824007678843656484670543729885

or

0.381966009824402913443622607419118062221218451809609846987747727401050194794195697589068940206651233696572751397436621308791146744960758850431934955677262718084806052735588052622663881203771667325390999943537914290553893060809666309073457173507989385127886624131895432217266105809948619502004404042685336796341256846027892270340466376827960024843317712156287053243746824007678843656484670543729885

(Nn22)2∀Y2nd=(Yn22/Yn24)=(10946/28657)=0.^38196601179467494852915518023519558921031510625676100080259622430819695013434762885158948947901036395993997976061695222807690965558153330774330879017343057542659734096381337893010433750916006560351746519175070663363227134731479219736888020378964999825522559933000663014272254597480545765432529573926091356387619080852845727047492759186237219527515092298565795442649265449977317932791290086191855393097672470949506228844610391876330390480510869944516174058694210838538576961998813553407544404508497051331262867711204941201102697421223435809749799350943922950762466413092787102627630247409010015005059845761942980772586104616673064172802456642356143350664759046655267473915622709983599120633702062323341591932163171301950657779949052587500436193600167498342464319363506298635586418676065184771609030952297867885682381268102034406951181212269253585511393376836375056705168021774784520361517255818822626234427888474020309174023798722825138709564853264472903653557595002966116481138988728757371671842830721987646997243256446941410475625501622640192623093833967268032243430924381477474962487350385595142548068534738458317339567993858394109641623338102383361831315210943225041002198415744844191646020169592071745123355550127368531248909515999581254143839201591234253411033953309837038070977422619255330285794046829744913982622046969326866036221516557909062358237079945563038699096206860452943434413930278814949227064940503192937153226087866838817740866106012492584708797152528178106570820392923195030882506891858882646473810936245943399518442265415081829919391422689046306312593781624036012143629828663153854206651080015354014725895941654744041595421711972641937397494503960637889520884949576019820637191611124681578671877726210001046864640401996021914366472415116725407404822556443451861674285514882925637715043444882576682834909446208605227344104407300136092403252259482848867641413965174302962626932337648742017657116934780332902955647834734968768538228007118679554733572949017692012422793732770352793383815472659385141501203894336462295425201521443277384234218515545939909969640925428342115364483372299961614963185260145863139896011445720068395156506263740098405276197787626059950448407020972188296053320305684474997382838398995009945214083818962208186481487943608891370345814286212792685905712391387793558292912726384478486931639738981749659768991869351292877830896465087064242593432669155878144955857207663049167742610880413162578078654429982203301113166067627455769968943015668074118016540461318351537146246990264158844261436996196391806539414453711135150225075897686429144711588791569250095962592036849635342150259971385699829012108734340649753986809505530934850123878982447569529259866699235788812506542904002512475136964790452594479533796280140977771574135464284468018285235719021530516104267718184038803782670900652545625850577520326621767805422758837282339393516418327110304637610356980842377080643472798967093554803363925044491747217084830931360575077642460829814704958648846704121157134382524339602889346407509509020483651463865722162124437310255783927138221028021076874760093519907875911644624350071535750427469728164148375615032976236172662874690302543881076176850333251910527968733642739993718812157588023868513801165509299647555571064661339288829954286910702446173709739330704539902990543322748368635935373556199183445580486443102906794151516208954182224238405974107547894057298391318002582266112991590187388770631957287922671598562305893847925463237603377883239697107164043689150992776633981226227448790871340335694594688906724360540182154447429947307813099766200230310220888439124821160623931325679589629060962417559409568342813274243640297309557874166870223680078165893150015702969606029940328715497086226750881111072338346651777925114282723243884565725651673238650242523641693129078410161566109502041386048783892242733014621209477614544439403985064731130264856754021704993544334717521024531528073420106780193321003594235265380186341905991555291900757232089890777122518058415046934431378022821649160763513277733189098649544613881425131730467250584499424224447778902187947098440171685801025927347593956101476079142966814390899256726105314582824440799804585267124960742575984925149178211257284433122797222319154133370555187214293191890288585685870816903374393690895767177303974596084726244896534878040269393167463446976305963638901490037338172174337858114945737516139163206197438671179816449733049516697491014411836549534145235021111770248106919775273057193704853962382663921554942945877098091216805667027253376138465296437170673831873538751439438880552744530132253899570785497435181631015109746309802142582964022751858184736713542938898000488536832187598143560037687127054471856788917193006944202114666573612031964267020274278535785322957741564015772760582056740063509788184387758662804899326517081341382559235090902746274906654569564155354712635656209652091984506403322050458875667376208256272463970408626164636912447220574379732700561817357015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(Nn23)2∀Y2nd=(Yn23/Yn25)=(17711/46368)

(Nn24)2∀Y2nd=(Yn24/Yn26)=(28657/75025)

(Nn25)2∀Y2nd=(Yn25/Yn27)=(46368/121393)

(Nn26)2∀Y2nd=(Yn26/Yn28)=(75025/196418)

(Nn27)2∀Y2nd=(Yn27/Yn29)=(121393/317811)

(Nn28)2∀Y2nd=(Yn28/Yn30)=(196418/514229)

(Nn29)2∀Y2nd=(Yn29/Yn31)=(317811/832040)

(Nn30)2∀Y2nd=(Yn30/Yn32)=(514229/1346296)

(Nn31)2∀Y2nd=(Yn31/Yn33)=(832040/2178309)

(Nn32)2∀Y2nd=(Yn32/Yn34)=(1346269/3524578)

(Nn33)2∀Y2nd=(Yn33/Yn35)=(2178309/5702887)

(Nn34)2∀Y2nd=(Yn34/Yn36)=(3524578/9227465)

(Nn35)2∀Y2nd=(Yn35/Yn37)=(5702887/14930352)

(Nn36)2∀Y2nd=(Yn36/Yn38)=(9227465/24157817)

(Nn37)2∀Y2nd=(Yn37/Yn39)=(14930352/39088169)

(Nn38)2∀Y2nd=(Yn38/Yn40)=(24157817/63245986)

(Nn39)2∀Y2nd=(Yn39/Yn41)=(39088169/102334155)

(Nn40)2∀Y2nd=(Yn40/Yn42)=(63245986/165780141)

(Nn41)2∀Y2nd=(Yn41/Yn43)=(102334155/269114296)

(Nn42)2∀Y2nd=(Yn42/Yn44)=(165780141/434894437)

(Nn43)2∀Y2nd=(Yn43/Yn45)=(269114296/704008733)

(Nn44)2∀Y2nd=(Yn44/Yn46)=(434894437/1138903170)


if 12nd=(n3/n1) of (Nn) then

(Nn1)1∀Y2nd=(Yn3/Yn1)=0 and so on for (Nn) of 1∀Y2nd and vary in quotient to the cn defined as (Nncn) of 1∀Y2nd

(Nn1)1∀Y3rd=(Yn4/Yn1)=0 and so on for (Nn) of 1∀Y3rd and vary in quotient to the cn defined as (Nncn) of 1∀Y3rd

(Nn1)1∀Y4th=(Yn5/Yn1)=0 and so on for (Nn) of 1∀Y4th and vary in quotient to the cn defined as (Nncn) of 1∀Y4th 

(Nn1)1∀Y5th=(Yn6/Yn1)=0 and so on for (Nn) of 1∀Y5th and vary in quotient to the cn defined as (Nncn) of 1∀Y5th

(Nn1)1∀Y6th=(Yn7/Yn1)=0 and so on for (Nn) of 1∀Y6th and vary in quotient to the cn defined as (Nncn) of 1∀Y6th

(Nn1)1∀Y7th=(Yn8/Yn1)=0 and so on for (Nn) of 1∀Y7th and vary in quotient to the cn defined as (Nncn) of 1∀Y7th

(Nn1)1∀Y8th=(Yn9/Yn1)=0 and so on for (Nn) of 1∀Y8th and vary in quotient to the cn defined as (Nncn) of 1∀Y8th

(Nn1)1∀Y9th=(Yn10/Yn1)=0 and so on for (Nn) of 1∀Y9th and vary in quotient to the cn defined as (Nncn) of 1∀Y9th

(Nn1)1∀Y10th=(Yn11/Yn1)=0 and so on for (Nn) of 1∀Y10th and vary in quotient to the cn defined as (Nncn) of 1∀Y10th

and so on to the Nth number or quotient of path function (Nncn)1∀Ynth scale division

if 22nd=(n1/n3) of (Nn) then

(Nn1)2∀Y2nd=(Yn1/Yn3)=0 and so on for (Nn) of 2∀Y2nd and vary in quotient to the cn defined as (Nncn) of 2∀Y2nd

(Nn1)2∀Y3rd=(Yn1/Yn4)=0 and so on for (Nn) of 2∀Y3rd and vary in quotient to the cn defined as (Nncn) of 2∀Y3rd

(Nn1)2∀Y4th=(Yn1/Yn5)=0 and so on for (Nn) of 2∀Y4th and vary in quotient to the cn defined as (Nncn) of 2∀Y4th

(Nn1)2∀Y5th=(Yn1/Yn6)=0 and so on for (Nn) of 2∀Y5th and vary in quotient to the cn defined as (Nncn) of 2∀Y5th

(Nn1)2∀Y6th=(Yn1/Yn7)=0 and so on for (Nn) of 2∀Y6th and vary in quotient to the cn defined as (Nncn) of 2∀Y6th

(Nn1)2∀Y7th=(Yn1/Yn8)=0 and so on for (Nn) of 2∀Y7th and vary in quotient to the cn defined as (Nncn) of 2∀Y7th

(Nn1)2∀Y8th=(Yn1/Yn9)=0 and so on for (Nn) of 2∀Y8th and vary in quotient to the cn defined as (Nncn) of 2∀Y8th

(Nn1)2∀Y9th=(Yn1/Yn10)=0 and so on for (Nn) of 2∀Y9th and vary in quotient to the cn defined as (Nncn) of 2∀Y9th

(Nn1)2∀Y10th=(Yn1/Yn11)=0 and so on for (Nn) of 2∀Y10th and vary in quotient to the cn defined as (Nncn) of 2∀Y10th

and so on to the Nth number or quotient of path function (Nncn)2∀Ynth scale division


These are 10 base example sets of path 1∀Y and path 2∀Y variables that continue to Ynnn and these sets rooted from Y base factors and paths differ from variables factored in sets 1φ and 2Θ from Y base variables.


Path 1Nncn and path 2Nncn have quantum field fractal polarization math notation practical application with variables from sets φ  Θ just as Path 1Nncn and path 2Nncn were applied with Y base factors. 

N set is numbers that are not same numeral values within sets φ  Θ and are numbers definable as real numbers.


Now complex equation variable sets ᐱ and ᗑ can be formulated and answered with a combination of path 1∀Y and path 2∀Y variables with sets A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  Y  Z  φ  Θ with path functions of ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄ to specific notated cycles in decimal stem cn of any known Nncn


This is non-theoretical math. These are numeral values of number structure constants applicable as scale unit measures in real math and a standard unit measure base is itself within the logic of numbers and the relation among their values with one another. 


if 12nd=(n3/n1) of (Nn) then

(Nn1)1∀Y2nd=(Yn3/Yn1)=0 and so on for (Nn) of 1∀Y2nd and vary in quotient to the cn defined as (Nncn) of 1∀Y2nd

(Nn1)1∀Y3rd=(Yn4/Yn1)=0 and so on for (Nn) of 1∀Y3rd and vary in quotient to the cn defined as (Nncn) of 1∀Y3rd

so

(Nn1)1∀Y3rd=(Yn4/Yn1)=(2/0)=0

(Nn2)1∀Y3rd=(Yn5/Yn2)=(3/1)=3

(Nn3)1∀Y3rd=(Yn6/Yn3)=(5/1)=5

(Nn4)1∀Y3rd=(Yn7/Yn4)=(8/2)=4

(Nn5)1∀Y3rd=(Yn8/Yn5)=(13/3)=4.^3 or 4.3

(Nn6)1∀Y3rd=(Yn9/Yn6)=(21/5)=4.2

(Nn7)1∀Y3rd=(Yn10/Yn7)=(34/8)=4.25

(Nn8)1∀Y3rd=(Yn11/Yn8)=(55/13)=4.^230769 or 4.230769

(Nn8)1∀Y3rd=(Yn12/Yn9)=(89/21)=4.^238095 or 4.238095

(Nn9)1∀Y3rd=(Yn13/Yn10)=(144/34)=4.^2352941176470588 or 4.2352941176470588

(Nn10)1∀Y3rd=(Yn14/Yn11)=(233/55)=4.2^36 or 4.236

(Nn11)1∀Y3rd=(Yn15/Yn12)=(377/89)=4.^23595505617977528089887640449438202247191011 or 4.23595505617977528089887640449438202247191011

(Nn12)1∀Y3rd=(Yn16/Yn13)=(610/144)=4.236^1 or 4.2361

(Nn13)1∀Y3rd=(Yn17/Yn14)=(987/233)=4.^2360515021459227467811158798283261802575107296137339055793991416309012875536480686695278969957081545064377682403433476394849785407725321888412017167381974248927038626609442060085836909871244635193133047210300429184549356223175965665

or

4.2360515021459227467811158798283261802575107296137339055793991416309012875536480686695278969957081545064377682403433476394849785407725321888412017167381974248927038626609442060085836909871244635193133047210300429184549356223175965665

(Nn14)1∀Y3rd=(Yn18/Yn15)=(1597/377)=4.^236074270557029177718832891246684350132625994694960212201591511936339522546419098143 

or

4.236074270557029177718832891246684350132625994694960212201591511936339522546419098143

(Nn15)1∀Y3rd=(Yn19/Yn16)=(2584/610)=4.2^360655737704918032786885245901639344262295081967213114754098 

or

4.2360655737704918032786885245901639344262295081967213114754098

(Nn16)1∀Y3rd=(Yn20/Yn17)=(4181/987)=4.^236068895643363728470111448834853090172239108409321175278622087132725430597771023302938196555217831813576494427558257345491388044579533941

or

4.236068895643363728470111448834853090172239108409321175278622087132725430597771023302938196555217831813576494427558257345491388044579533941

(Nn17)1∀Y3rd=(Yn21/Yn18)=(6765/1597)=4.^2360676268002504696305572949279899812147777082028804007514088916718847839699436443331246086412022542266750156543519098309329993738259

or

4.2360676268002504696305572949279899812147777082028804007514088916718847839699436443331246086412022542266750156543519098309329993738259

(Nn18)1∀Y3rd=(Yn22/Yn19)=(10946/2584)=4.23^606811145510835913312693498452012383900928792569659442724458204334365325077399380804953560371517027863777089783281733746130030959752321981424148

or

4.23606811145510835913312693498452012383900928792569659442724458204334365325077399380804953560371517027863777089783281733746130030959752321981424148

(Nn19)1∀Y3rd=(Yn23/Yn20)=(17711/4181)=4.^236067926333413059076775890935182970581200669696244917483855536952882085625448457306864386510404209519253767041377660846687395359961731643147572351112174121023678545802439607749342262616598899784740492705094475005979430758191820138722793590050227218368811289165271466156421908634298014828988280315713944032528103324563501554651997129873

or

4.236067926333413059076775890935182970581200669696244917483855536952882085625448457306864386510404209519253767041377660846687395359961731643147572351112174121023678545802439607749342262616598899784740492705094475005979430758191820138722793590050227218368811289165271466156421908634298014828988280315713944032528103324563501554651997129873

(Nn20)1∀Y3rd=(Yn24/Yn21)=(28657/6765)=4.2^3606799704 or 4.23606799704

(Nn21)1∀Y3rd=(Yn25/Yn22)=(46368/10946)=4.^236067970034715877946281746756806139228942079298373835190937328704549607162433765759181436141056093550155307875022839393385711675497898775808514525854193312625616663621414215238443266946829892198063219440891649917778183811437968207564407089347706924904074547780010962908825141604238991412388086972410012790060295998538278823314452768134478348255070345331627991960533528229490224739630915402886899323953955782934405262196

or

4.236067970034715877946281746756806139228942079298373835190937328704549607162433765759181436141056093550155307875022839393385711675497898775808514525854193312625616663621414215238443266946829892198063219440891649917778183811437968207564407089347706924904074547780010962908825141604238991412388086972410012790060295998538278823314452768134478348255070345331627991960533528229490224739630915402886899323953955782934405262196

(Nn22)1∀Y3rd=(Yn26/Yn23)=(75025/17711)=4.^236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130088645474563830387894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407317486307944215459319067246344079950313364575687425893512506351984642312687030658912540229

or

4.236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130088645474563830387894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407317486307944215459319067246344079950313364575687425893512506351984642312687030658912540229

(Nn23)1∀Y3rd=(Yn27/Yn24)=(121393/28657)

(Nn24)1∀Y3rd=(Yn28/Yn25)=(196418/46368)

(Nn25)1∀Y3rd=(Yn29/Yn26)=(317811/75025)

(Nn26)1∀Y3rd=(Yn30/Yn27)=(514229/121393)

(Nn27)1∀Y3rd=(Yn31/Yn28)=(832040/196418)

(Nn28)1∀Y3rd=(Yn32/Yn29)=(1346296/317811)

(Nn29)1∀Y3rd=(Yn33/Yn30)=(2178309/514229)

(Nn30)1∀Y3rd=(Yn34/Yn31)=(3524578/832040)

(Nn31)1∀Y3rd=(Yn35/Yn32)=(5702887/1346296)

(Nn32)1∀Y3rd=(Yn36/Yn33)=(9227465/2178309)

(Nn33)1∀Y3rd=(Yn37/Yn34)=(14930352/3524578)

(Nn34)1∀Y3rd=(Yn38/Yn35)=(24157817/5702887)

(Nn35)1∀Y3rd=(Yn39/Yn36)=(39088169/9227465)

(Nn36)1∀Y3rd=(Yn40/Yn37)=(63245986/14930352)

(Nn37)1∀Y3rd=(Yn41/Yn38)=(102334155/24157817)

(Nn38)1∀Y3rd=(Yn42/Yn39)=(165780141/39088169)

(Nn39)1∀Y3rd=(Yn43/Yn40)=(269114296/63245986)

(Nn40)1∀Y3rd=(Yn44/Yn41)=(434894437/102334155)

(Nn41)1∀Y3rd=(Yn45/Yn42)=( 704008733/165780141)

(Nn42)1∀Y3rd=(Yn46/Yn43)=(1138903170/269114296)


Examples of 10 digit Y base for (Nncn) of 1∀Y3rd


if 22nd=(n1/n3) of (Nn) then

(Nn1)2∀Y2nd=(Yn1/Yn3)=0 and so on for (Nn) of 2∀Y2nd and vary in quotient to the cn defined as (Nncn) of 2∀Y2nd

(Nn1)2∀Y3rd=(Yn1/Yn4)=0 and so on for (Nn) of 2∀Y3rd and vary in quotient to the cn defined as (Nncn) of 2∀Y3rd

so

(Nn1)2∀Y3rd=(Yn1/Yn4)=(0/2)=0

(Nn2)2∀Y3rd=(Yn2/Yn5)=(1/3)=0.^3 or 0.3

(Nn3)2∀Y3rd=(Yn3/Yn6)=(1/5)=0.2

(Nn4)2∀Y3rd=(Yn4/Yn7)=(2/8)=0.25

(Nn5)2∀Y3rd=(Yn5/Yn8)=(3/13)=0.^230769 or 0.230769

(Nn6)2∀Y3rd=(Yn6/Yn9)=(5/21)=0.^238095 or 0.238095

(Nn7)2∀Y3rd=(Yn7/Yn10)=(8/34)=0.^2352941176470588 or 0.2352941176470588

(Nn8)2∀Y3rd=(Yn8/Yn11)=(13/55)=0.2^36 or 0.236

(Nn9)2∀Y3rd=(Yn9/Yn12)=(21/89)=0.^23595505617977528089887640449438202247191011 or 0.23595505617977528089887640449438202247191011

(Nn10)2∀Y3rd=(Yn10/Yn13)=(34/144)=0.236^1 or 0.2361

(Nn11)2∀Y3rd=(Yn11/Yn14)=(55/233)=0.^2360515021459227467811158798283261802575107296137339055793991416309012875536480686695278969957081545064377682403433476394849785407725321888412017167381974248927038626609442060085836909871244635193133047210300429184549356223175965665

or

0.2360515021459227467811158798283261802575107296137339055793991416309012875536480686695278969957081545064377682403433476394849785407725321888412017167381974248927038626609442060085836909871244635193133047210300429184549356223175965665

(Nn12)2∀Y3rd=(Yn12/Yn15)=(89/377)=0.^236074270557029177718832891246684350132625994694960212201591511936339522546419098143 

or

0.236074270557029177718832891246684350132625994694960212201591511936339522546419098143

(Nn13)2∀Y3rd=(Yn13/Yn16)=(144/610)=0.2^360655737704918032786885245901639344262295081967213114754098 

or

0.2360655737704918032786885245901639344262295081967213114754098

(Nn14)2∀Y3rd=(Yn14/Yn17)=(233/987)=0.^236068895643363728470111448834853090172239108409321175278622087132725430597771023302938196555217831813576494427558257345491388044579533941

or

0.236068895643363728470111448834853090172239108409321175278622087132725430597771023302938196555217831813576494427558257345491388044579533941

(Nn15)2∀Y3rd=(Yn15/Yn18)=(377/1597)=0.^2360676268002504696305572949279899812147777082028804007514088916718847839699436443331246086412022542266750156543519098309329993738259

or

0.2360676268002504696305572949279899812147777082028804007514088916718847839699436443331246086412022542266750156543519098309329993738259

(Nn16)2∀Y3rd=(Yn16/Yn19)=(610/2584)=0.23^606811145510835913312693498452012383900928792569659442724458204334365325077399380804953560371517027863777089783281733746130030959752321981424148

or

0.23^606811145510835913312693498452012383900928792569659442724458204334365325077399380804953560371517027863777089783281733746130030959752321981424148

(Nn17)2∀Y3rd=(Yn17/Yn20)=(987/4181)=0.^2360679263334130590767758909351829705812006696962449174838555369528820856254484573068643865104042095192537670413776608466873953599617316431475723511121741210236785458024396077493422626165988997847404927050944750059794307581918201387227935900502272183688112891652714661564219086342980148289882803157139440325281033245635015546519971298732

or

0.2360679263334130590767758909351829705812006696962449174838555369528820856254484573068643865104042095192537670413776608466873953599617316431475723511121741210236785458024396077493422626165988997847404927050944750059794307581918201387227935900502272183688112891652714661564219086342980148289882803157139440325281033245635015546519971298732

(Nn18)2∀Y3rd=(Yn18/Yn21)=(1597/6765)=0.2^3606799704 or 0.23606799704

(Nn19)2∀Y3rd=(Yn19/Yn22)=(2584/10946)=0.^236067970034715877946281746756806139228942079298373835190937328704549607162433765759181436141056093550155307875022839393385711675497898775808514525854193312625616663621414215238443266946829892198063219440891649917778183811437968207564407089347706924904074547780010962908825141604238991412388086972410012790060295998538278823314452768134478348255070345331627991960533528229490224739630915402886899323953955782934405262196

or

0.236067970034715877946281746756806139228942079298373835190937328704549607162433765759181436141056093550155307875022839393385711675497898775808514525854193312625616663621414215238443266946829892198063219440891649917778183811437968207564407089347706924904074547780010962908825141604238991412388086972410012790060295998538278823314452768134478348255070345331627991960533528229490224739630915402886899323953955782934405262196

(Nn20)2∀Y3rd=(Yn20/Yn23)=(4181/17711)=0.^236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130088645474563830387894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407317486307944215459319067246344079950313364575687425893512506351984642312687030658912540229

or

0.236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130088645474563830387894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407317486307944215459319067246344079950313364575687425893512506351984642312687030658912540229

(Nn21)2∀Y3rd=(Yn21/Yn24)=(6765/28657)

(Nn22)2∀Y3rd=(Yn22/Yn25)=(10946/46368)

(Nn23)2∀Y3rd=(Yn23/Yn26)=(17711/75025)

(Nn24)2∀Y3rd=(Yn24/Yn27)=(28657/121393)

(Nn25)2∀Y3rd=(Yn25/Yn28)=(46368/196418)

(Nn26)2∀Y3rd=(Yn26/Yn29)=(75025/317811)

(Nn27)2∀Y3rd=(Yn27/Yn30)=(121393/514229)

(Nn28)2∀Y3rd=(Yn28/Yn31)=(196418/832040)

(Nn29)2∀Y3rd=(Yn29/Yn32)=(317811/1346296)

(Nn30)2∀Y3rd=(Yn30/Yn33)=(514229/2178309)

(Nn31)2∀Y3rd=(Yn31/Yn34)=(832040/3524578)

(Nn32)2∀Y3rd=(Yn32/Yn35)=(1346296/5702887)

(Nn33)2∀Y3rd=(Yn33/Yn36)=(2178309/9227465)

(Nn34)2∀Y3rd=(Yn34/Yn37)=(3524578/14930352)

(Nn35)2∀Y3rd=(Yn35/Yn38)=(5702887/24157817)

(Nn36)2∀Y3rd=(Yn36/Yn39)=(9227465/39088169)

(Nn37)2∀Y3rd=(Yn37/Yn40)=(14930352/63245986)

(Nn38)2∀Y3rd=(Yn38/Yn41)=(24157817/102334155)

(Nn39)2∀Y3rd=(Yn39/Yn42)=(39088169/165780141)

(Nn40)2∀Y3rd=(Yn40/Yn43)=(63245986/269114296)

(Nn41)2∀Y3rd=(Yn41/Yn44)=(102334155/434894437)

(Nn42)2∀Y3rd=(Yn42/Yn45)=(165780141/704008733)

(Nn43)2∀Y3rd=(Yn43/Yn46)=(269114296/1138903170)


Examples of 10 digit Y base for (Nncn) of 2∀Y3rd


Crossed Paths of for all for any (Nncn) of functions examples

if

A=∈1/Q)cn and path ⅄ of Q is a variant in the definition of A

M=2/Q)cn and path ⅄ of Q is a variant in the definition of M

V= 1(Q/φ)cn and path ⅄ of Q is a variant in the definition of V

W=2(Q/φ)cn and path ⅄ of Q is a variant in the definition of W

E=∈1/Q)cn and path ⅄ of Q is a variant in the definition of E

F=2/Q)cn and path ⅄ of Q is a variant in the definition of F

I= 1(Q/Θ)cn and path ⅄ of Q is a variant in the definition of I

H=2(Q/Θ)cn and path ⅄ of Q is a variant in the definition of H

D=1/Θ)cn

B=2/Θ)cn

O=1/φ)cn

G=2/φ)cn

L=1(1Qn2/2Qn1)cn

K=2(1Qn1/2Qn2)cn

U=1(2Qn2/1Qn1)cn

J=2(2Qn1/1Qn2)cn


then function paths for all for any (Nncn) of ⅄∀ is applicable to both the variable factors of A M V W E F I H D B O G L K U J sets variables.

(Nncn) of 1⅄∀/Q)cn

(Nncn) of 2⅄∀/Q)cn 

(Nncn) of 1⅄∀(Ancn/Ancn)

(Nncn) of 2⅄∀(Ancn/Ancn)

and given that Set A has decimal stem looping variables of cn more complexly that Y base variables do not have

(Nncn) of 3⅄∀/Q)cn

(Nncn) of 3⅄∀(Ancn/Ancn)

With these equations the definition of cn is critical to an effective use of this math and the quotient correct answer.

As (Nncn) of ⅄∀ is applicable to both the variable factors of A it then too is applicable to M V W E F I H D B O G L K U J sets variables in the same respect.


Prime consecutive step tier base rationals of 2:199 of the 10 digit prime 1,000,000,007

1st tier 46 primes example 10 tiers to 9 divisions of primes with primes (p) or (P) PQ2Q 1Q

3Q does not exist where numbers of p have no decimals path variant of cn

2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 53 59 61 67 71 73 79 83 89 97 101 103 107 109 113 127 131 137 139 149 151 157 163 167 173 179 181 191 193 197 199

After factoring quotients for sets 1Q and 2Q from ordinal prime P base then

if 12nd=(n3/n1) of (Nn) then

(Nn1)1∀P2nd=(Pn3/Pn1)=(5/2)=2.5

(Nn2)1∀P2nd=(Pn4/Pn2)=(7/3)=2.^3 or  2.3

(Nn3)1∀P2nd=(Pn5/Pn3)=(11/5)=2.2

(Nn4)1∀P2nd=(Pn6/Pn4)=(13/7)=1.^857142 or 1.857142

(Nn5)1∀P2nd=(Pn7/Pn5)=(17/11)=1.^54 or 1.54

(Nn6)1∀P2nd=(Pn8/Pn6)=(19/13)=1.^461538 or 1.461538

(Nn7)1∀P2nd=(Pn9/Pn7)=(23/17)=1.^3529411764705882 or 1.3529411764705882

(Nn8)1∀P2nd=(Pn10/Pn8)=(29/19)=1.^526315789473684210 or 1.526315789473684210

(Nn9)1∀P2nd=(Pn11/Pn9)=(31/23)=1.^3478260869565217391304 or 1.3478260869565217391304

(Nn10)1∀P2nd=(Pn12/Pn10)=(37/29)=1.^2758620689655172413793103448 or 1.2758620689655172413793103448

(Nn11)1∀P2nd=(Pn13/Pn11)=(41/31)=1.^322580645161290 or 1.322580645161290

(Nn12)1∀P2nd=(Pn14/Pn12)=(43/37)=1.^162 or 1.162

(Nn13)1∀P2nd=(Pn15/Pn13)=(47/41)=1.^14634 or 1.14634

(Nn14)1∀P2nd=(Pn16/Pn14)=(53/43)=1.^232558139534883720930 or 1.232558139534883720930

(Nn15)1∀P2nd=(Pn17/Pn15)=(59/47)=1.^2553191489361702127659574468085106382978723404 or 1.2553191489361702127659574468085106382978723404

(Nn16)1∀P2nd=(Pn18/Pn16)=(61/53)=1.^1509433962264 or 1.1509433962264

(Nn17)1∀P2nd=(Pn19/Pn17)=(67/59)=1.^1355932203389830508474576271186440677966101694915254237288 or 1.1355932203389830508474576271186440677966101694915254237288

(Nn18)1∀P2nd=(Pn20/Pn18)=(71/61)=1.^163934426229508196721311475409836065573770491803278688524590 or 1.163934426229508196721311475409836065573770491803278688524590

(Nn19)1∀P2nd=(Pn21/Pn19)=(73/67)=1.^089552238805970149253731343283582 or 1.089552238805970149253731343283582

(Nn20)1∀P2nd=(Pn22/Pn20)=(79/71)=1.^11267605633802816901408450704225352 or 1.11267605633802816901408450704225352

(Nn21)1∀P2nd=(Pn23/Pn21)=(83/73)=1.^13698630 or 1.13698630

(Nn22)1∀P2nd=(Pn24/Pn22)=(89/79)=1.^1265822784810 or 1.1265822784810

(Nn23)1∀P2nd=(Pn25/Pn23)=(97/83)=1.^16867469879518072289156626506024096385542 or 1.16867469879518072289156626506024096385542

(Nn24)1∀P2nd=(Pn26/Pn24)=(101/89)=1.^13483146067415730337078651685393258426966292 or 1.13483146067415730337078651685393258426966292

(Nn25)1∀P2nd=(Pn27/Pn25)=(103/97)=1.^061855670103092783505154639175257731958762886597938144329896907216494845360824742268041237113402 or 1.061855670103092783505154639175257731958762886597938144329896907216494845360824742268041237113402

(Nn26)1∀P2nd=(Pn28/Pn26)=(107/101)=1.^0594 or 1.0594

(Nn27)1∀P2nd=(Pn29/Pn27)=(109/103)=1.^0582524271844660194174757281553398 or 1.0582524271844660194174757281553398

(Nn28)1∀P2nd=(Pn30/Pn28)=(113/107)=1.^05607476635514018691588785046728971962616822429906542 or 1.05607476635514018691588785046728971962616822429906542

(Nn29)1∀P2nd=(Pn31/Pn29)=(127/109)=1.^165137614678899082568807339449541284403669724770642201834862385321100917431192660550458715596330275229357798 

or

1.165137614678899082568807339449541284403669724770642201834862385321100917431192660550458715596330275229357798

(Nn30)1∀P2nd=(Pn32/Pn30)=(131/113)=1.^1592920353982300884955752212389380530973451327433628318584070796460176991150442477876106194690265486725663716814

or

1.1592920353982300884955752212389380530973451327433628318584070796460176991150442477876106194690265486725663716814

(Nn31)1∀P2nd=(Pn33/Pn31)=(137/127)=1.^078740157480314960629921259842519685039370 or 1.078740157480314960629921259842519685039370

(Nn32)1∀P2nd=(Pn34/Pn32)=(139/131)=1.^0610687022900763358778625954198473282442748091603053435114503816793893129770992366412213740458015267175572519083969465648854961832

or

1.0610687022900763358778625954198473282442748091603053435114503816793893129770992366412213740458015267175572519083969465648854961832

(Nn33)1∀P2nd=(Pn35/Pn33)=(149/137)=1.^08759124 or 1.08759124

(Nn34)1∀P2nd=(Pn36/Pn34)=(151/139)=1.^0863309352517985611510791366906474820143884892 or 1.0863309352517985611510791366906474820143884892

(Nn35)1∀P2nd=(Pn37/Pn35)=(157/149)=1.^0536912751677852348993288590604026845637583892617449664429530201342281879194630872483221476510067114093959731543624161073825503355704697986577181208

or

1.0536912751677852348993288590604026845637583892617449664429530201342281879194630872483221476510067114093959731543624161073825503355704697986577181208

(Nn36)1∀P2nd=(Pn38/Pn36)=(163/151)=1.^079470198675496688741721854304635761589403973509933774834437086092715231788

or

1.079470198675496688741721854304635761589403973509933774834437086092715231788

(Nn37)1∀P2nd=(Pn39/Pn37)=(167/157)=1.^063694267515923566878980891719745222929936305732484076433121019108280254777070

or

1.063694267515923566878980891719745222929936305732484076433121019108280254777070

(Nn38)1∀P2nd=(Pn40/Pn38)=(173/163)=1.^061349693251533742331288343558282208588957055214723926380368098159509202453987730

or

1.061349693251533742331288343558282208588957055214723926380368098159509202453987730

(Nn39)1∀P2nd=(Pn41/Pn39)=(179/167)=1.^0718562874251497005988023952095808383233532934131736526946107784431137724550898203592814371257485029940119760479041916167664670658682634730538922155688622754491017964

or

1.0718562874251497005988023952095808383233532934131736526946107784431137724550898203592814371257485029940119760479041916167664670658682634730538922155688622754491017964

(Nn40)1∀P2nd=(Pn42/Pn40)=(181/173)=1.^0462427745664739884393063583815028901734104

or

1.0462427745664739884393063583815028901734104

(Nn41)1∀P2nd=(Pn43/Pn41)=(191/179)=1.^0670391061452513966480446927374301675977653631284916201117318435754189944134078212290502793296089385474860335195530726256983240223463687150837988826815642458100558659217877094972

or

1.0670391061452513966480446927374301675977653631284916201117318435754189944134078212290502793296089385474860335195530726256983240223463687150837988826815642458100558659217877094972

(Nn42)1∀P2nd=(Pn44/Pn42)=(193/181)=1.^066298342541436464088397790055248618784530386740331491712707182320441988950276243093922651933701657458563535911602209944751381215469613259668508287292817679558011049723756906077348

or

1.066298342541436464088397790055248618784530386740331491712707182320441988950276243093922651933701657458563535911602209944751381215469613259668508287292817679558011049723756906077348

(Nn43)1∀P2nd=(Pn45/Pn43)=(197/191)=1.^03141361256544502617801047120418848167539267015706806282722513089005235602094240837696335078534

or

1.03141361256544502617801047120418848167539267015706806282722513089005235602094240837696335078534

(Nn44)1∀P2nd=(Pn46/Pn44)=(199/193)=1.^031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341968911917098445595854922279792746113989637305699481865284974093264248704663212435233160621761658

or

1.031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341968911917098445595854922279792746113989637305699481865284974093264248704663212435233160621761658


Prime consecutive step tier base rationals of 2:199 of the 10 digit prime 1,000,000,007

1st tier 46 primes example 10 tiers to 9 divisions of primes with primes (p) or (P) PQ2Q 1Q

3Q does not exist where numbers of p have no decimals path variant of cn

2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 53 59 61 67 71 73 79 83 89 97 101 103 107 109 113 127 131 137 139 149 151 157 163 167 173 179 181 191 193 197 199

After factoring quotients for sets 1Q and 2Q from ordinal prime P base then

if 22nd=(n1/n3) of (Nn) then

(Nn1)2∀P2nd=(Pn1/Pn3)=(2/5)=0.4

(Nn2)2∀P2nd=(Pn2/Pn4)=(3/7)=0.^428571 or 0.428571

(Nn3)2∀P2nd=(Pn3/Pn5)=(5/11)=0.^45 or 0.45

(Nn4)2∀P2nd=(Pn4/Pn6)=(7/13)=0.^538461 or 0.538461

(Nn5)2∀P2nd=(Pn5/Pn7)=(11/17)=0.^6470588235294117 or 0.6470588235294117

(Nn6)2∀P2nd=(Pn6/Pn8)=(13/19)=0.^684210526315789473 or 0.684210526315789473

(Nn7)2∀P2nd=(Pn7/Pn9)=(17/23)=0.^7391304347826086956521 or 0.7391304347826086956521

(Nn8)2∀P2nd=(Pn8/Pn10)=(19/29)=0.^6551724137931034482758620689 or 0.6551724137931034482758620689

(Nn9)2∀P2nd=(Pn9/Pn11)=(23/31)=0.^741935483870967 or 0.741935483870967

(Nn10)2∀P2nd=(Pn10/Pn12)=(29/37)=0.^783 or 0.783

(Nn11)2∀P2nd=(Pn11/Pn13)=(31/41)=0.^75609 or 0.75609

(Nn12)2∀P2nd=(Pn12/Pn14)=(37/43)=0.^860465116279069767441 or 0.860465116279069767441

(Nn13)2∀P2nd=(Pn13/Pn15)=(41/47)=0.^8723404255319148936170212765957446808510638297 or 0.8723404255319148936170212765957446808510638297

(Nn14)2∀P2nd=(Pn14/Pn16)=(43/53)=0.^8113207547169 or 0.8113207547169

(Nn15)2∀P2nd=(Pn15/Pn17)=(47/59)=0.^7966101694915254237288135593220338983050847457627118644067 

or

0.7966101694915254237288135593220338983050847457627118644067

(Nn16)2∀P2nd=(Pn16/Pn18)=(53/61)=0.^868852459016393442622950819672131147540983606557377049180327

or

0.868852459016393442622950819672131147540983606557377049180327

(Nn17)2∀P2nd=(Pn17/Pn19)=(59/67)=0.^880597014925373134328358208955223 or 0.880597014925373134328358208955223

(Nn18)2∀P2nd=(Pn18/Pn20)=(61/71)=0.^85915492957746478873239436619718309 or 0.85915492957746478873239436619718309

(Nn19)2∀P2nd=(Pn19/Pn21)=(67/73)=0.^91780821 or 0.91780821

(Nn20)2∀P2nd=(Pn20/Pn22)=(71/79)=0.^8987341772151 or 0.8987341772151

(Nn21)2∀P2nd=(Pn21/Pn23)=(73/83)=0.^87951807228915662650602409638554216867469 or 0.87951807228915662650602409638554216867469

(Nn22)2∀P2nd=(Pn22/Pn24)=(79/89)=0.^88764044943820224719101123595505617977528089 or 0.88764044943820224719101123595505617977528089

(Nn23)2∀P2nd=(Pn23/Pn25)=(83/97)=0.^855670103092783505154639175257731958762886597938144329896907216494845360824742268041237113402061 

or

0.855670103092783505154639175257731958762886597938144329896907216494845360824742268041237113402061

(Nn24)2∀P2nd=(Pn24/Pn26)=(89/101)=0.^8811 or 0.8811

(Nn25)2∀P2nd=(Pn25/Pn27)=(97/103)=0.^9417475728155339805825242718446601 or 0.9417475728155339805825242718446601

(Nn26)2∀P2nd=(Pn26/Pn28)=(101/107)=0.^94392523364485981308411214953271028037383177570093457 or 0.94392523364485981308411214953271028037383177570093457

(Nn27)2∀P2nd=(Pn27/Pn29)=(103/109)=0.^944954128440366972477064220183486238532110091743119266055045871559633027522935779816513761467889908256880733

or

0.944954128440366972477064220183486238532110091743119266055045871559633027522935779816513761467889908256880733

(Nn28)2∀P2nd=(Pn28/Pn30)=(107/113)=0.^9469026548672566371681415929203539823008849557522123893805309734513274336283185840707964601769911504424778761061

or

0.9469026548672566371681415929203539823008849557522123893805309734513274336283185840707964601769911504424778761061

(Nn29)2∀P2nd=(Pn29/Pn31)=(109/127)=0.^858267716535433070866141732283464566929133 or 0.858267716535433070866141732283464566929133

(Nn30)2∀P2nd=(Pn30/Pn32)=(113/131)=0.^8625954198473282442748091603053435114503816793893129770992366412213740458015267175572519083969465648854961832061068702290076335877

or

0.8625954198473282442748091603053435114503816793893129770992366412213740458015267175572519083969465648854961832061068702290076335877

(Nn31)2∀P2nd=(Pn31/Pn33)=(127/137)=0.^92700729 or 0.92700729

(Nn32)2∀P2nd=(Pn32/Pn34)=(131/139)=0.^9424460431654676258992805755395683453237410071 or 0.9424460431654676258992805755395683453237410071

(Nn33)2∀P2nd=(Pn33/Pn35)=(137/149)=0.^9194630872483221476510067114093959731543624161073825503355704697986577181208053691275167785234899328859060402684563758389261744966442953020134228187

or

0.9194630872483221476510067114093959731543624161073825503355704697986577181208053691275167785234899328859060402684563758389261744966442953020134228187

(Nn34)2∀P2nd=(Pn34/Pn36)=(139/151)=0.^920529801324503311258278145695364238410596026490066225165562913907284768211

or

0.920529801324503311258278145695364238410596026490066225165562913907284768211

(Nn35)2∀P2nd=(Pn35/Pn37)=(149/157)=0.949044585987261146496815286624203821656050955414012738853503184713375796178343

or

0.949044585987261146496815286624203821656050955414012738853503184713375796178343

(Nn36)2∀P2nd=(Pn36/Pn38)=(151/163)=0.926380368098159509202453987730061349693251533742331288343558282208588957055214723

or

0.926380368098159509202453987730061349693251533742331288343558282208588957055214723

(Nn37)2∀P2nd=(Pn37/Pn39)=(157/167)=0.^9401197604790419161676646706586826347305389221556886227544910179640718562874251497005988023952095808383233532934131736526946107784431137724550898203592814371257485029

or

0.9401197604790419161676646706586826347305389221556886227544910179640718562874251497005988023952095808383233532934131736526946107784431137724550898203592814371257485029

(Nn38)2∀P2nd=(Pn38/Pn40)=(163/173)=0.^9421965317919075144508670520231213872832369

or

0.9421965317919075144508670520231213872832369

(Nn39)2∀P2nd=(Pn39/Pn41)=(167/179)=0.^9329608938547486033519553072625698324022346368715083798882681564245810055865921787709497206703910614525139664804469273743016759776536312849162011173184357541899441340782122905027

or

0.9329608938547486033519553072625698324022346368715083798882681564245810055865921787709497206703910614525139664804469273743016759776536312849162011173184357541899441340782122905027

(Nn40)2∀P2nd=(Pn40/Pn42)=(173/181)=0.^955801104972375690607734806629834254143646408839779005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767

or

0.955801104972375690607734806629834254143646408839779005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767

(Nn41)2∀P2nd=(Pn41/Pn43)=(179/191)=0.^93717277486910994764397905759162303664921465968586387434554973821989528795811518324607329842931

or

0.93717277486910994764397905759162303664921465968586387434554973821989528795811518324607329842931

(Nn42)2∀P2nd=(Pn42/Pn44)=(181/193)=0.^937823834196891191709844559585492227979274611398963730569948186528497409326424870466321243523316062176165803108808290155440414507772020725388601036269430051813471502590673575129533678756476683

or

0.937823834196891191709844559585492227979274611398963730569948186528497409326424870466321243523316062176165803108808290155440414507772020725388601036269430051813471502590673575129533678756476683

(Nn43)2∀P2nd=(Pn43/Pn45)=(191/197)=0.^96954314720812182741116751269035532994923857868020304568527918781725888324873096446700507614213197

or

0.96954314720812182741116751269035532994923857868020304568527918781725888324873096446700507614213197

(Nn44)2∀P2nd=(Pn44/Pn46)=(193/199)=0.^969849246231155778894472361809045226130653266331658291457286432160804020100502512562814070351758793

or

0.969849246231155778894472361809045226130653266331658291457286432160804020100502512562814070351758793


Further factoring of For All For Any path functions

If 12nd=(n3/n1) and 22nd=(n1/n3)

then with

12nd=(n3/n1) applied with variables of sets, φ, Θ, 1⅄Q, 2⅄Q

1φ2nd=(φn3cn/φn1cn)

1Θ2nd=(Θn3cn/Θn1cn)

11⅄Q2nd=(1⅄Qn3cn/1⅄Qn1cn)

12⅄Q2nd=(2⅄Qn3cn/2⅄Qn1cn)

and

22nd=(n1/n3) applied with variables of sets, φ, Θ, 1⅄Q, 2⅄Q

2φ2nd=(φn1cn/φn3cn)

2Θ2nd=(Θn1cn/Θn3cn)

21⅄Q2nd=(1⅄Qn1cn/1⅄Qn3cn)

22⅄Q2nd=(2⅄Qn1cn/2⅄Qn3cn)


And If 13rd=(n4/n1) and 23rd=(n1/n4)

then with

13rd=(n4/n1) applied with variables of sets, φ, Θ, 1⅄Q, 2⅄Q

1φ3rd=(φn4cn/φn1cn)

1Θ3rd=(Θn4cn/Θn1cn)

11⅄Q3rd=(1⅄Qn4cn/1⅄Qn1cn)

12⅄Q3rd=(2⅄Qn4cn/2⅄Qn1cn)

and

23rd=(n1/n4) applied with variables of sets, φ, Θ, 1⅄Q, 2⅄Q

2φ3rd=(φn1cn/φn4cn)

2Θ3rd=(Θn1cn/Θn4cn)

21⅄Q3rd=(1⅄Qn1cn/1⅄Qn4cn)

22⅄Q3rd=(2⅄Qn1cn/2⅄Qn4cn)


And so on for further sets from the (For all For any) nn function to consecutive variable sets

Complex further variables factored in ᐱ and ᗑ equations then may be also including variables from any multitude of a variety of (For all For any) nn variable factors each with a definable cn variable factor of potential change.


if

12nd=(n3/n1) then 1φ2nd=(φn3cn/φn1cn)

(Nn1) 1φ2nd=(φn3cn/φn1cn)=(2/0)=0

(Nn2) 1φ2nd=(φn4cn/φn2cn)=(1.5/1)=1.5

(Nn3) 1φ2nd=(φn5cn/φn3cn)=(1.6/2)=0.8 and (Nn3) 1φ2nd=(φn5c2/φn3cn)=(1.66/2)=0.83 and so on for cn variable change factors of (Nn3) 1φ2nd that are φn5cn and φn3cn

(Nn4) 1φ2nd=(φn6cn/φn4cn)=(1.6/1.5)=1.06

(Nn5) 1φ2nd=(φn7cn/φn5cn)=(1.625/1.6)=1.015625 and (Nn5) 1φ2nd=(φn7cn/φn5c2)=(1.625/1.66)=0.9789156626506024096385542168674698795180722  and so on for cn variable change factors of (Nn5) 1φ2nd that are φn7cn and φn5cn

(Nn6) 1φ2nd=(φn8cn/φn6cn)=(1.615384/1.6)=1.009615

(Nn7) 1φ2nd=(φn9cn/φn7cn)=(1.619047/1.625)=0.996336615384


So then for application of quotients from function path (Nn)1φ2nd as variable factors including their potential change use in complex set ᐱ and ᗑ equations with varying paths ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄ the quotient stem cell cycle and accurate quotients must be factored to definable values before practical application of the quotients of a number (Nn)1φ2nd can then be used in complex set ᐱ and ᗑ equations with varying paths ncn  ⅄X  1  2  3ncn  +⅄  1-⅄  2-⅄


(Nn8) 1φ2nd=(φn10cn/φn8cn)=(1.61762941/1.615384)

(Nn9) 1φ2nd=(φn11cn/φn9cn)=(1.618/1.619047)

(Nn10) 1φ2nd=(φn12cn/φn10cn)=(1.61797752808988764044943820224719101123595505/1.61762941)

(Nn11) 1φ2nd=(φn13cn/φn11cn)=(1.61805/1.618)

(Nn12) 1φ2nd=(φn14cn/φn12cn)=(1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/1.61797752808988764044943820224719101123595505)

(Nn13) 1φ2nd=(φn15cn/φn13cn)=(1.61830223896551724135014/1.61805)

(Nn14) 1φ2nd=(φn16cn/φn14cn)=(1.618032786885245901639344262295081967213114754098360655737704918/1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

(Nn15) 1φ2nd=(φn17cn/φn15cn)=(1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843/1.61830223896551724135014)

(Nn16) 1φ2nd=(φn18cn/φn16cn)=(1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.618032786885245901639344262295081967213114754098360655737704918)

(Nn17) 1φ2nd=(φn19cn/φn17cn)=(1.618034055731424148606811145510835913312693/1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843)

(Nn18) 1φ2nd=(φn20cn/φn18cn)=(1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn19) 1φ2nd=(φn21cn/φn19cn)=(1.61803399852/1.618034055731424148606811145510835913312693)

(Nn20) 1φ2nd=(φn22cn/φn20cn)=(1.6180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242)

(Nn21) 1φ2nd=(φn23cn/φn21cn)=(1.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793292304217717802495624188357517983174298458585060132121280560103890237705381401388967308452374230704082208796792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869/1.61803399852)

(Nn22) 1φ2nd=(φn24cn/φn22cn)=(1.6180339882053250514708448197648044107896848937432389991974037756918030498656523711484105105209896360400600202393830477719230903444184666922566912098265694245734026590361866210698956624908399343964825348082492933663677286526852078026311197962103500017447744006699933698572774540251945423456747042607390864361238091914715427295250724081376278047248490770143420455735073455002268206720870991380814460690232752905049377115538960812366960951948913005548382594130578916146142303800118644659245559549150294866873713228879505879889730257877656419025020064905607704923753358690721289737236975259098998499494015423805701922741389538332693582719754335764385664933524095334473252608437729001640087936629793767665840806783682869804934222005094741249956380639983250165753568063649370136441358132393481522839096904770213211431761873189796559304881878773074641448860662316362494329483197822521547963848274418117737376557211152597969082597620127717486129043514673552709634644240499703388351886101127124262832815716927801235300275674355305858952437449837735980737690616603273196775656907561852252503751264961440485745193146526154168266043200614160589035837666189761663816868478905677495899780158425515580835397983040792825487664444987263146875109048400041874585616079840876574658896604669016296192902257738074466971420595317025508601737795303067313396377848344209093764176292005443696130090379313954705656558606972118505077293505949680706284677391213316118225913389398750741529120284747182189342917960707680496911749310814111735352618906375405660048155773458491817008060857731095369368740621837596398785637017133684614579334891998464598527410405834525595840457828802735806260250549603936211047911505042398017936280838887531842132812227378999895313535959800397808563352758488327459259517744355654813832571448511707436228495655511742331716509055379139477265589559269986390759674774051715113235858603482569703737306766235125798234288306521966709704435216526503123146177199288132044526642705098230798757720626722964720661618452734061485849879610566353770457479847855672261576578148445406009003035907457165788463551662770003838503681473985413686010398855427993160484349373625990159472380221237394004955159297902781170394667969431552500261716160100499005478591618103779181351851205639110862965418571378720731409428760861220644170708727361552151306836026101825034023100813064870712216910353491293575740656733084412185504414279233695083225738911958683742192134557001779669888683393237254423003105698433192588198345953868164846285375300973584115573856300380360819346058554628886484977492410231357085528841120843074990403740796315036465784974002861430017098789126565935024601319049446906514987612101755243047074013330076421118749345709599748752486303520954740552046620371985902222842586453571553198171476428097846948389573228181596119621732909934745437414942247967337823219457724116271766060648358167288969536238964301915762291935652720103290644519663607495550825278291516906863942492235753917018529504135115329587884286561747566039711065359249049097951634853613427783787556268974421607286177897197892312523990648009212408835537564992846424957253027183585162438496702376382733712530969745611892382314966674808947203126635726000628118784241197613148619883449070035244442893533866071117004571308929755382629026066929546009700945667725163136406462644380081655441951355689709320584848379104581777576159402589245210594270160868199741773388700840981261122936804271207732840143769410615207453676239662211676030289283595631084900722336601877377255120912865966430540531109327563945981784555257005269218690023379976968977911156087517883937606867432041037093903758244059043165718672575635970269044212583312977631992183410684998429703039397005967128450291377324911888892766165334822207488571727675611543427434832676134975747635830687092158983843389049795861395121610775726698537879052238545556059601493526886973514324597829500645566528247897546847192657989321980667899640576473461981365809400844470809924276791010922287748194158495306556862197717835083923648672226681090135045538611857486826953274941550057577555222109781205290155982831419897407265240604389852392085703318560910074327389468541717555920019541473287503925742401507485082178874271556687720277768084586662944481278570680810971141431412918309662560630910423282269602540391527375510346512195973060683253655302369403636109850996266182782566214188505426248386083679380256132882018355026695048330250898558816345046585476497888822975189308022472694280629514603761733607844505705412290190878319433297274662386153470356282932616812646124856056111944725546986774610042921450256481836898489025369019785741703597724814181526328645706110199951146316781240185643996231287294552814321108280699305579788533342638796803573297972572146421467704225843598422723941794325993649021181561224133719510067348291865861744076490909725372509334543043584464528736434379034790801549359667794954112433262379174372753602959137383536308755277942562026729943818264298426213490595665980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(Nn23) 1φ2nd=(φn25cn/φn23cn)=(1.61803398895790200138026224982746721877156659765355417529330572808833678/1.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793292304217717802495624188357517983174298458585060132121280560103890237705381401388967308452374230704082208796792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869)

(Nn24) 1φ2nd=(φn26cn/φn24cn)=(1.61803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589/1.61803398820532505147084481976480441078968489374323899919740377569180304986565237114841051052098963604006002023938304777192309034441846669225669120982656942457340265903618662106989566249083993439648253480824929336636772865268520780263111979621035000174477440066999336985727745402519454234567470426073908643612380919147154272952507240813762780472484907701434204557350734550022682067208709913808144606902327529050493771155389608123669609519489130055483825941305789161461423038001186446592455595491502948668737132288795058798897302578776564190250200649056077049237533586907212897372369752590989984994940154238057019227413895383326935827197543357643856649335240953344732526084377290016400879366297937676658408067836828698049342220050947412499563806399832501657535680636493701364413581323934815228390969047702132114317618731897965593048818787730746414488606623163624943294831978225215479638482744181177373765572111525979690825976201277174861290435146735527096346442404997033883518861011271242628328157169278012353002756743553058589524374498377359807376906166032731967756569075618522525037512649614404857451931465261541682660432006141605890358376661897616638168684789056774958997801584255155808353979830407928254876644449872631468751090484000418745856160798408765746588966046690162961929022577380744669714205953170255086017377953030673133963778483442090937641762920054436961300903793139547056565586069721185050772935059496807062846773912133161182259133893987507415291202847471821893429179607076804969117493108141117353526189063754056600481557734584918170080608577310953693687406218375963987856370171336846145793348919984645985274104058345255958404578288027358062602505496039362110479115050423980179362808388875318421328122273789998953135359598003978085633527584883274592595177443556548138325714485117074362284956555117423317165090553791394772655895592699863907596747740517151132358586034825697037373067662351257982342883065219667097044352165265031231461771992881320445266427050982307987577206267229647206616184527340614858498796105663537704574798478556722615765781484454060090030359074571657884635516627700038385036814739854136860103988554279931604843493736259901594723802212373940049551592979027811703946679694315525002617161601004990054785916181037791813518512056391108629654185713787207314094287608612206441707087273615521513068360261018250340231008130648707122169103534912935757406567330844121855044142792336950832257389119586837421921345570017796698886833932372544230031056984331925881983459538681648462853753009735841155738563003803608193460585546288864849774924102313570855288411208430749904037407963150364657849740028614300170987891265659350246013190494469065149876121017552430470740133300764211187493457095997487524863035209547405520466203719859022228425864535715531981714764280978469483895732281815961196217329099347454374149422479673378232194577241162717660606483581672889695362389643019157622919356527201032906445196636074955508252782915169068639424922357539170185295041351153295878842865617475660397110653592490490979516348536134277837875562689744216072861778971978923125239906480092124088355375649928464249572530271835851624384967023763827337125309697456118923823149666748089472031266357260006281187842411976131486198834490700352444428935338660711170045713089297553826290260669295460097009456677251631364064626443800816554419513556897093205848483791045817775761594025892452105942701608681997417733887008409812611229368042712077328401437694106152074536762396622116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(Nn25) 1φ2nd=(φn27cn/φn25cn)=(1.6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575/1.61803398895790200138026224982746721877156659765355417529330572808833678)

(Nn26) 1φ2nd=(φn28cn/φn26cn)=(1.6180339887383030068527324379639340589966296367949984217332423708621409443126393711370648311254569336822490810414524127116659369304238919040006516714354081601482552515553564337280697288435886731358633119164231384089034609862639880255373743750572758097526703255302467187324990581311285116435357248317363989043773992200307507458583225569957946827683817165432903298068405135985500310562168436701320652893319349550448533230152022727041309859585170401897993055626266431793420154975613233003085256952010508201895956582390615931330122493865124377602867354315795904652323106843568308403506806911790161797798572432261808999175228339561547312364447250252013562911749432333085562422995855776965451231557189259640155179260556568135303281776619250781496604180879552790477451150098259833620136647354112148581087273060513802197354621266889999898176338217474976835116944475557229989104868189269822521357513058884623608834220896251871009785253897300654726145261635898950198047022167011170055697542995041187671191031371870195195959637100469407080817440356790110885967681169750226557647466118176541864798541885163274241668278874644889979533443981712470343858505839587003227810078506043234326792860124835809345375678400146626072966836033357431599955197588815688989807451455569245181195206142003278721909397305745909234387887057194350823244305511714812288079503915119795538087140689753484914824506918917818122575324053803622885886222240324206539115559673756987648789825779714690099685364885091997678420511358429471840666334042704843751590994715351953486951297742569418281420236434542659023103788858454927756111965298496064515472105407854677269903980286939078903155515278640450467879725890702481442637640134814528200063130670305165514362227494425154517406754981722652710036758341903491533362522783044323839973933142583673594069789937785742650877210846256453074565467523343074463643861560549440478978505024997708967609893186978790131250700037674754859534258571006730544043824904031198769970165667097720168212689264731338268386807726379456057998757751326253194717388426722601798205867079391909091834760561659318392408027777494934272826319380097547067987658972191957967192416173670437536274679510024539502489588530582736816381390707572625726766385972772352839352808805710270952764003299086641753810750542210998991945748353002270667657750308016576892138195073771242961439379282957773727458786872893522996874013583276481788838090195399606960665519453410583551405675650907757944791210581514932440000407294647130100092659532222097771080043580527242920709914569947764461505564663116414992515960858984410797381095418953456404199207811911331955319777209828019835249315235874512519219216161451598122371676730238572839556456129275320999093769410135527293832540805832459346903033326884501420440081866224073150118624565976641651987088759685975827062692828559500656762618497286399413495708132655866570273600179209644737244040770194177723019275219175431986885112362410777016363062448451771222596707022777953140750847681984339520817847651437240986060340701972324328727509698703784785508456455111038703173843537761304972049404840696881141239601258540459632009286317954566282112637334663829180624993636021138592186052194809029722326874319054261829363907584844566180288975552138806015741938111578368581290920384078852243684387377938885438198128481096437190074229449439460741887199747477318779337942551090022299381930372980073109389159852966632386033866549908867822704640104267429665305623720840248857029396491156614974187701738129906627702145424553757802238084085979900009164129560427252084839474997199849300980561862965715973077823824700383875204920119337331609119327149242941074646926452769094482175768004968994694987221130446293109592807176531682432363632660957753362726430367888890020262908694722479609811728049364111232168131230335305318249854901281959901841990041645877669052734474437169709497092934456108910588642588764777158916188943986803653432984756997831156004032217006587990917329368998767933692431447219704915028154242482868168905090164852508425908012503945666894072844647639218401572157337922186357665794377297396368968220835157673940270239998370821411479599629361871111608915679825677891028317160341720208942153977741347534340029936156564062356810475618324186174383203168752354672178720891160687920659002739056501949923123135354193607510513293079045708641774175482898716003624922359457890824669836776670162612387866692461994318239672535103707399525501736093433392051644961256096691749228685761997372949526010854402346017167469376533718905599283161421051023836919223289107922899123298272052459550550356891934547750206192915109613171908888187436996609272062641916728609394251036055758637192110702685089961205184860857966174179555845187304625848954780111802380637212475435041594965838161471962854728181734871549450661344683277500025455915445631255791220763881110692502723782952682544369660621735278844097791444775937032247553686525674836318463684591025262450488244458247207486075614251239703082202242157032451201010090724882648229795639910802472278508079707562443360588133470455864533800364528709181439582930281338777505116639004571882414035373540103249193047480373489191418301784968791047663656080399963343481758290991660642100011200602796077752548137136107688704701198464499180319522650673563522691403028235701412294188923622071296927980124021220051115478214827561628771293873270270545469356168986549094278528444439918948365221110081560753087802543555071327475078658778727000580394872160392632039833416489323789062102251321162011628262175564357645429644940891364335244224052785386268060972008675375983871131973648036330682524004928265230274211121/1.61803398867044318560479840053315561479506831056314561812729090303232255914695101632789070309896701099633455514828390536487837387537487504165278240586471176274575141619460179940019993335554815061646117960679773408863712095968010663112295901366211262912362545818060646451182939020326557814061979340219926691102965678107297567477507497500833055648117294235254915028323892035988003998667110963012329223592135954681772742419193602132622459180273242252582472509163612129290236587804065311562812395868043985338220593135621459513495501499500166611129623458847050983005664778407197600799733422192602465844718427190936354548483838720426524491836054648450516494501832722425858047317560813062312562479173608797067644118627124291902699100299900033322225924691769410196601132955681439520159946684438520493168943685438187270909696767744085304898367210929690103298900366544485171609463512162612462512495834721759413528823725424858380539820059980006664445184938353882039320226591136287904031989336887704098633788737087637454181939353548817060979673442185938020659780073308897034321892702432522492502499166944351882705764745084971676107964011996001332889036987670776407864045318227257580806397867377540819726757747417527490836387870709763412195934688437187604131956014661779406864378540486504498500499833388870376541152949016994335221592802399200266577807397534155281572809063645451516161279573475508163945351549483505498167277574141952682439186937687437520826391202932355881372875708097300899700099966677774075308230589)

(Nn27) 1φ2nd=(φn29cn/φn27cn)=(1.618033988754322537608830405492572629644663022991652271318488032195235533068395996362/1.6180339887802426828565073768668704126267577207911494072969611097839249380112527081462687304869308773982025322712182745298328569192622309358859242295684265155321970789089980476633743296565699834422083645679734416317250582817790152644715922664404043066733666685887983656388753882019556317085828672163963325727183610257593106686547000238893511157974512533671628512352442068323544191180710584630085754532798431540533638677683227204204525796380351420592620661817402980402494377764780506289489509279777252395113392040727224798793999654016294185002430123647986292455083901048660136910695015363324079642153995699916799156458774393910686777656042770176204558747209476658456418409628232270394503801701910324318535665153674429332828087286746352755101200233950886789188832964009456887958943266909953621708006227706704669956257774336246735808489781124117535607489723460166566441228077401497615183742060909607638002191230136828317942550229420147784468626691819132898931569365614162266358027233860272009094428838565650408178395788884037794601006647829776016739021195620834809255887901279315940787360061947558755447183939765884359065184977717001804057894606773042926692642903627062515960557857537090277034095870437339879564719547255607819231751418945079205555509790515103836300280905818292652788875800087319697181880339064031698697618478824973433394017776972313065827518884943942401950689084214081536826670401093967526957897078085227319532427734712874712709958564332375013386274332127882167835048149399059253828474458988574300000823770728130946594943695270732249800235598428245450726153896847429423442867381150478198907680014498364815104660071009036764887596484146532337119932780308584514757852594465908248416300775168255171220745842017249759047062021698120978969133310816933431087459738205662599985172126893642961291013485126819503595759228291581886929229856746270378028387139291392419661759739029433328116118721837338232023263285362417931841209954445478734358653299613651528506586046971406918026574843689504337152883609433822378555600405295198240425724712298073200266901715914426696761757267717248935276333890751526035273862578567133195489031492754936446088324697470200093909863006927911823581260863476477226858220819981382781544240606954272486881451154514675475521652813588921931248095030191197185999192704686431672336955178634682395195769113540319458288369181089519165025989966472531365070473585791602481197433130411143970410155445536398309622465875297587175537304457423409916552025240335109932203669074823095236133879218735841440610249355399405237534289456558450652014531315644229897934806784575716886476155956274249750809354740388655029532180603494435428731475455751155338446203652599408532617201980344830426795614244643430840328519766378621502063545673968021220333956653184285749590174062754854069015511602810705724382789781947888263738436318403861837173477877637096043429192787063504485431614673004209468420749137100162282833441796479203907968334253210646412890364353793052317678943596418244874086644205184812962856177868575)

(Nn28) 1φ2nd=(φn30cn/φn28cn)

(Nn29) 1φ2nd=(φn31cn/φn29cn)

(Nn30) 1φ2nd=(φn32cn/φn30cn)

(Nn31) 1φ2nd=(φn33cn/φn31cn)

(Nn32) 1φ2nd=(φn34cn/φn32cn)

(Nn33) 1φ2nd=(φn35cn/φn33cn)

(Nn34) 1φ2nd=(φn36cn/φn34cn)

(Nn35) 1φ2nd=(φn37cn/φn35cn)

(Nn36) 1φ2nd=(φn38cn/φn36cn)

(Nn37) 1φ2nd=(φn39cn/φn37cn)

(Nn38) 1φ2nd=(φn40cn/φn38cn)

(Nn39) 1φ2nd=(φn41cn/φn39cn)

(Nn40) 1φ2nd=(φn42cn/φn40cn)

(Nn41) 1φ2nd=(φn43cn/φn41cn)

(Nn42) 1φ2nd=(φn44cn/φn42cn)

(Nn43) 1φ2nd=(φn45cn/φn43cn)


And if

13rd=(n4/n1) then 1φ3rd=(φn4cn/φn1cn)

(Nn1) 1φ3rd=(φn4cn/φn1cn)=(1.5/0)=0

(Nn2) 1φ3rd=(φn5cn/φn2cn)=(1.6/1)=1.6 and (Nn2) 1φ3rd=(φn5c2/φn2cn)=(1.66/1)=1.66 and so on for cn of (Nn2) 1φ3rd

(Nn3) 1φ3rd=(φn6cn/φn3cn)=(1.6/2)=0.8

(Nn4) 1φ3rd=(φn7cn/φn4cn)=(1.625/1.5)=1.083


(Nn5) 1φ3rd=(φn8cn/φn5cn)=(1.615384/1.6)=1.009615 and (Nn5) 1φ3rd=(φn8cn/φn5c2)=(1.615384/1.66)=0.973122891566265060240963855421686746987951807 while change variant factor of (Nn5) 1φ3rd=(φn8c2/φn5cn)=(1.615384615384/1.6)=1.009615384615 and so quotients for (Nn5) 1φ3rd rely on the cn definition to each variable and its number of repeated stem decimal cycle loops.


(Nn6) 1φ3rd=(φn9cn/φn6cn)=(1.619047/1.6)=1.011904375 while (Nn6) 1φ3rd=(φn9c2/φn6cn)=(1.619047619047/1.6)=1.011904761904375 and so on for cn variant of (Nn6) 1φ3rd

(Nn7) 1φ3rd=(φn10cn/φn7cn)=(1.61762941/1.625)=0.99546425230769

(Nn8) 1φ3rd=(φn11cn/φn8cn)=(1.618/1.615384)

(Nn9) 1φ3rd=(φn12cn/φn9cn)=(1.61797752808988764044943820224719101123595505/1.619047)

(Nn10) 1φ3rd=(φn13cn/φn10cn)=(1.61805/1.61762941)

(Nn11) 1φ3rd=(φn14cn/φn11cn)=(1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/1.618)

(Nn12) 1φ3rd=(φn15cn/φn12cn)=(1.61830223896551724135014/1.61797752808988764044943820224719101123595505)

(Nn13) 1φ3rd=(φn16cn/φn13cn)=(1.618032786885245901639344262295081967213114754098360655737704918/1.61805)

(Nn14) 1φ3rd=(φn17cn/φn14cn)=(1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843/1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

(Nn15) 1φ3rd=(φn18cn/φn15cn)=(1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.61830223896551724135014)

(Nn16) 1φ3rd=(φn19cn/φn16cn)=(1.618034055731424148606811145510835913312693/1.618032786885245901639344262295081967213114754098360655737704918)

(Nn17) 1φ3rd=(φn20cn/φn17cn)=(1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843)

(Nn18) 1φ3rd=(φn21cn/φn18cn)=(1.61803399852/1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn19) 1φ3rd=(φn22cn/φn19cn)=(1.6180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981/1.618034055731424148606811145510835913312693)

(Nn20) 1φ3rd=(φn23cn/φn20cn)=(1.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793292304217717802495624188357517983174298458585060132121280560103890237705381401388967308452374230704082208796792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869/1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242)

(Nn21) 1φ3rd=(φn24cn/φn21cn)

(Nn22) 1φ3rd=(φn25cn/φn22cn)

(Nn23) 1φ3rd=(φn26cn/φn23cn)

(Nn24) 1φ3rd=(φn27cn/φn24cn)

(Nn25) 1φ3rd=(φn28cn/φn25cn)

(Nn26) 1φ3rd=(φn29cn/φn26cn)

(Nn27) 1φ3rd=(φn30cn/φn27cn)

(Nn28) 1φ3rd=(φn31cn/φn28cn)

(Nn29) 1φ3rd=(φn32cn/φn29cn)

(Nn30) 1φ3rd=(φn33cn/φn30cn)

(Nn31) 1φ3rd=(φn34cn/φn31cn)

(Nn32) 1φ3rd=(φn35cn/φn32cn)

(Nn33) 1φ3rd=(φn36cn/φn33cn)

(Nn34) 1φ3rd=(φn37cn/φn34cn)

(Nn35) 1φ3rd=(φn38cn/φn35cn)

(Nn36) 1φ3rd=(φn39cn/φn36cn)

(Nn37) 1φ3rd=(φn40cn/φn37cn)

(Nn38) 1φ3rd=(φn41cn/φn38cn)

(Nn39) 1φ3rd=(φn42cn/φn39cn)

(Nn40) 1φ3rd=(φn43cn/φn40cn)

(Nn41) 1φ3rd=(φn44cn/φn41cn)

(Nn42) 1φ3rd=(φn45cn/φn42cn)


Then if

12nd=(n3/n1) then 1Θ2nd=(Θn3cn/Θn1cn)

(Nn1) 1Θ2nd=(Θn3cn/Θn1cn)=(0.5/0)=0

(Nn2) 1Θ2nd=(Θn4cn/Θn2cn)=(0.6/1)=0.6 and (Nn2) 1Θ2nd=(Θn4c2/Θn2cn)=(0.66/1)=0.66 

and so on for cn variable factors of (Nn2) 1Θ2nd

(Nn3) 1Θ2nd=(Θn5cn/Θn3cn)=(0.6/0.5)=0.12

(Nn4) 1Θ2nd=(Θn6cn/Θn4cn)=(0.625/0.6)=1.0416

and (Nn4) 1Θ2nd=(Θn6cn/Θn4c2)=(0.625/0.66)=0.9469

(Nn5) 1Θ2nd=(Θn7cn/Θn5cn)=(0.615384/0.6)=1.02564

(Nn6) 1Θ2nd=(Θn8cn/Θn6cn)=(0.619047/0.625)=0.9904752

(Nn7) 1Θ2nd=(Θn9cn/Θn7cn)=(0.61764705882352941/0.615384)=1.00367747426570955695

(Nn8) 1Θ2nd=(Θn10cn/Θn8cn)=(0.618/0.619047)=0.998308690616382924075231767539459847152154844462536770229077921385613693306000

(Nn9) 1Θ2nd=(Θn11cn/Θn9cn)=(0.6179775280878651685393258764044943820224719101123595505/0.61764705882352941)

(Nn10) 1Θ2nd=(Θn12cn/Θn10cn)=(0.61805/0.618)

(Nn11) 1Θ2nd=(Θn13cn/Θn11cn)=(0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566/0.6179775280878651685393258764044943820224719101123595505)

(Nn12) 1Θ2nd=(Θn14cn/Θn12cn)=(0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.61805)

(Nn13) 1Θ2nd=(Θn15cn/Θn13cn)=(0.618032786885245901639344262295081967213114754098360655737749/0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566)

(Nn14) 1Θ2nd=(Θn16cn/Θn14cn)=(0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

(Nn15) 1Θ2nd=(Θn17cn/Θn15cn)=(0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.618032786885245901639344262295081967213114754098360655737749)

(Nn16) 1Θ2nd=(Θn18cn/Θn16cn)=(0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

(Nn17) 1Θ2nd=(Θn19cn/Θn17cn)=(0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn18) 1Θ2nd=(Θn20cn/Θn18cn)=(0.61803399852/0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

(Nn19) 1Θ2nd=(Θn21cn/Θn19cn)=(0.6180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981/0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

(Nn20) 1Θ2nd=(Θn22cn/Θn20cn)=(0.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114/0.61803399852)

(Nn21) 1Θ2nd=(Θn23cn/Θn21cn)

(Nn22) 1Θ2nd=(Θn24cn/Θn22cn)

(Nn23) 1Θ2nd=(Θn25cn/Θn23cn)

(Nn24) 1Θ2nd=(Θn26cn/Θn24cn)

(Nn25) 1Θ2nd=(Θn27cn/Θn25cn)

(Nn26) 1Θ2nd=(Θn28cn/Θn26cn)

(Nn27) 1Θ2nd=(Θn29cn/Θn27cn)

(Nn28) 1Θ2nd=(Θn30cn/Θn28cn)

(Nn29) 1Θ2nd=(Θn31cn/Θn29cn)

(Nn30) 1Θ2nd=(Θn32cn/Θn30cn)

(Nn31) 1Θ2nd=(Θn33cn/Θn31cn)

(Nn32) 1Θ2nd=(Θn34cn/Θn32cn)

(Nn33) 1Θ2nd=(Θn35cn/Θn33cn)

(Nn34) 1Θ2nd=(Θn36cn/Θn34cn)

(Nn35) 1Θ2nd=(Θn37cn/Θn35cn)

(Nn36) 1Θ2nd=(Θn38cn/Θn36cn)

(Nn37) 1Θ2nd=(Θn39cn/Θn37cn)

(Nn38) 1Θ2nd=(Θn40cn/Θn38cn)

(Nn39) 1Θ2nd=(Θn41cn/Θn39cn)

(Nn40) 1Θ2nd=(Θn42cn/Θn40cn)

(Nn41) 1Θ2nd=(Θn43cn/Θn41cn)

(Nn42) 1Θ2nd=(Θn44cn/Θn42cn)

(Nn43) 1Θ2nd=(Θn45cn/Θn43cn)

And if

13rd=(n4/n1) then 1Θ3rd=(Θn4cn/Θn1cn)

(Nn1) 1Θ3rd=(Θn4cn/Θn1cn)=(0.6/0)=0

(Nn2) 1Θ3rd=(Θn5cn/Θn2cn)=(0.6/1)=0.6

(Nn3) 1Θ3rd=(Θn6cn/Θn3cn)=(0.625/0.5)=1.25

(Nn4) 1Θ3rd=(Θn7cn/Θn4cn)=(0.615384/0.6)=1.02564 and (Nn4) 1Θ3rd=(Θn7c2/Θn4cn)=(0.615384615384/0.6)=1.02564102564 while (Nn4) 1Θ3rd=(Θn7cn/Θn4c2)=(0.615384/0.66)=0.9324 and so on for cn of (Nn4) 1Θ3rd

(Nn5) 1Θ3rd=(Θn8cn/Θn5cn)=(0.619047/0.6)=1.031745 and (Nn5) 1Θ3rd=(Θn8cn/Θn5cn)=(0.619047/0.6)=1.031746031745

(Nn6) 1Θ3rd=(Θn9cn/Θn6cn)=(0.61764705882352941/0.625)=0.988235294117647056 and (Nn6) 1Θ3rd=(Θn9c2/Θn6cn)=(0.617647058823529411764705882352941/0.625)=0.9882352941176470588235294117647056 and so on for cn of (Nn6) 1Θ3rd

(Nn7) 1Θ3rd=(Θn10cn/Θn7cn)=(0.618/0.615384)=1.00425 and ((Nn7) 1Θ3rd)c2=1.00425100425

(Nn8) 1Θ3rd=(Θn11cn/Θn8cn)=(0.6179775280878651685393258764044943820224719101123595505/0.619047)=0.9982723897989412250432129974048729450630919948119602396910089217781525473833166140858448550756243063935371627679319987012294704

(Nn9) 1Θ3rd=(Θn12cn/Θn9cn)=(0.61805/0.61764705882352941) and (Nn9) 1Θ3rd=(Θn12c2/Θn9cn)=(0.618055/0.61764705882352941) and (Nn9) 1Θ3rd=(Θn12cn/Θn9c2)=(0.61805/0.617647058823529411764705882352941) and so on for cn variables of (Nn9) 1Θ3rd

(Nn10) 1Θ3rd=(Θn13cn/Θn10cn)=(0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566/0.618)=1.0000416753475832326346931122130088753698070752948317290998236037612678306040529466505548842312874147533925016181229773462783171521035598705

(Nn11) 1Θ3rd=(Θn14cn/Θn11cn)=(0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6179775280878651685393258764044943820224719101123595505)

(Nn12) 1Θ3rd=(Θn15cn/Θn12cn)=(0.618032786885245901639344262295081967213114754098360655737749/0.61805)

(Nn13) 1Θ3rd=(Θn16cn/Θn13cn)=(0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566)

(Nn14) 1Θ3rd=(Θn17cn/Θn14cn)=(0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

(Nn15) 1Θ3rd=(Θn18cn/Θn15cn)=(0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/0.618032786885245901639344262295081967213114754098360655737749)

(Nn16) 1Θ3rd=(Θn19cn/Θn16cn)=(0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

(Nn17) 1Θ3rd=(Θn20cn/Θn17cn)=(0.61803399852/0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn18) 1Θ3rd=(Θn21cn/Θn18cn)=(0.6180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981/0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

(Nn19) 1Θ3rd=(Θn22cn/Θn19cn)=(0.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114/0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

(Nn20) 1Θ3rd=(Θn23cn/Θn20cn)

(Nn21) 1Θ3rd=(Θn24cn/Θn21cn)

(Nn22) 1Θ3rd=(Θn25cn/Θn22cn)

(Nn23) 1Θ3rd=(Θn26cn/Θn23cn)

(Nn24) 1Θ3rd=(Θn27cn/Θn24cn)

(Nn25) 1Θ3rd=(Θn28cn/Θn25cn)

(Nn26) 1Θ3rd=(Θn29cn/Θn26cn)

(Nn27) 1Θ3rd=(Θn30cn/Θn27cn)

(Nn28) 1Θ3rd=(Θn31cn/Θn28cn)

(Nn29) 1Θ3rd=(Θn32cn/Θn29cn)

(Nn30) 1Θ3rd=(Θn33cn/Θn30cn)

(Nn31) 1Θ3rd=(Θn34cn/Θn31cn)

(Nn32) 1Θ3rd=(Θn35cn/Θn32cn)

(Nn33) 1Θ3rd=(Θn36cn/Θn33cn)

(Nn34) 1Θ3rd=(Θn37cn/Θn34cn)

(Nn35) 1Θ3rd=(Θn38cn/Θn35cn)

(Nn36) 1Θ3rd=(Θn39cn/Θn36cn)

(Nn37) 1Θ3rd=(Θn40cn/Θn37cn)

(Nn38) 1Θ3rd=(Θn41cn/Θn38cn)

(Nn39) 1Θ3rd=(Θn42cn/Θn39cn)

(Nn40) 1Θ3rd=(Θn43cn/Θn40cn)

(Nn41) 1Θ3rd=(Θn44cn/Θn41cn)

(Nn42) 1Θ3rd=(Θn45cn/Θn42cn)


Then if

12nd=(n3/n1) then 1(1⅄Q)2nd=(1⅄Qn3cn/1⅄Qn1cn)

(Nn1) 1(1⅄Q)2nd=(1⅄Qn3cn/1⅄Qn1cn)=(1.4/1.5)=0.93 


(Nn2) 1(1⅄Q)2nd=(1⅄Qn4cn/1⅄Qn2cn)=(1.571428/1.6)=0.9821425 and (Nn2) 1(1⅄Q)2nd=(1⅄Qn4cn/1⅄Qn2c2)=(1.571428/1.66)=0.946643373493975903614457831325301204819277108 and (Nn2) 1(1⅄Q)2nd=(1⅄Qn4c2/1⅄Qn2cn)=(1.571428571428/1.6)=0.9821428571425 while (Nn2) 1(1⅄Q)2nd=(1⅄Qn4cn/1⅄Qn2cn)=(1.571428571428/1.66)=0.946643717727710843373493975903614457831325301204819 and so on for cn variables of (Nn2) 1(1⅄Q)2nd


(Nn3) 1(1⅄Q)2nd=(1⅄Qn5cn/1⅄Qn3cn)=(1.18/1.4)=0.84285714 and (Nn3) 1(1⅄Q)2nd=(1⅄Qn5c2/1⅄Qn3cn)=(1.1818/1.4)=0.844142857 and (Nn3) 1(1⅄Q)2nd=(1⅄Qn5c3/1⅄Qn3cn)=(1.181818/1.4)=0.84415571428 and so on for cn variables of (Nn3) 1(1⅄Q)2nd


(Nn4) 1(1⅄Q)2nd=(1⅄Qn6cn/1⅄Qn4cn)=(1.307692/1.571428)

(Nn5) 1(1⅄Q)2nd=(1⅄Qn7cn/1⅄Qn5cn)=(1.1176470588235294/1.18)

(Nn6) 1(1⅄Q)2nd=(1⅄Qn8cn/1⅄Qn6cn)=(1.210526315789473684/1.307692)

(Nn7) 1(1⅄Q)2nd=(1⅄Qn9cn/1⅄Qn7cn)=(1.2608695652173913043478/1.1176470588235294)

(Nn8) 1(1⅄Q)2nd=(1⅄Qn10cn/1⅄Qn8cn)=(1.0689655172413793103448275862/1.210526315789473684)

(Nn9) 1(1⅄Q)2nd=(1⅄Qn11cn/1⅄Qn9cn)=(1.193548387096774/1.2608695652173913043478)

(Nn10) 1(1⅄Q)2nd=(1⅄Qn12cn/1⅄Qn10cn)=(1.^108/1.0689655172413793103448275862)

(Nn11) 1(1⅄Q)2nd=(1⅄Qn13cn/1⅄Qn11cn)=(1.^04878/1.193548387096774)

(Nn12) 1(1⅄Q)2nd=(1⅄Qn14cn/1⅄Qn12cn)=(1.093023255813953488372/1.108)

(Nn13) 1(1⅄Q)2nd=(1⅄Qn15cn/1⅄Qn13cn)=(1.12765957446808510638297872340425531914893610702/1.04878)

(Nn14) 1(1⅄Q)2nd=(1⅄Qn16cn/1⅄Qn14cn)=(1.1132075471698/1.093023255813953488372)

(Nn15) 1(1⅄Q)2nd=(1⅄Qn17cn/1⅄Qn15cn)=(1.0338983050847457627118644067796610169491525423728813559322/1.12765957446808510638297872340425531914893610702)

(Nn16) 1(1⅄Q)2nd=(1⅄Qn18cn/1⅄Qn16cn)=(1.098360655737704918032786885245901639344262295081967213114754/1.1132075471698)

(Nn17) 1(1⅄Q)2nd=(1⅄Qn19cn/1⅄Qn17cn)=(1.059701492537313432835820895522388/1.0338983050847457627118644067796610169491525423728813559322)

(Nn18) 1(1⅄Q)2nd=(1⅄Qn20cn/1⅄Qn18cn)=(1.02816901408450704225352112676056338/1.098360655737704918032786885245901639344262295081967213114754)

(Nn19) 1(1⅄Q)2nd=(1⅄Qn21cn/1⅄Qn19cn)=(1.08219178/1.059701492537313432835820895522388)

(Nn20) 1(1⅄Q)2nd=(1⅄Qn22cn/1⅄Qn20cn)=(1.0506329113924/1.02816901408450704225352112676056338)

(Nn21) 1(1⅄Q)2nd=(1⅄Qn23cn/1⅄Qn21cn)=(1.07228915662650602409638554216867469879518/1.08219178)

(Nn22) 1(1⅄Q)2nd=(1⅄Qn24cn/1⅄Qn22cn)=(1.08988764044943820224719101123595505617977528/1.0506329113924)

(Nn23) 1(1⅄Q)2nd=(1⅄Qn25cn/1⅄Qn23cn)=(1.04123092783505154639175257731958762886597938144329896907216494845360820618/1.07228915662650602409638554216867469879518)

(Nn24) 1(1⅄Q)2nd=(1⅄Qn26cn/1⅄Qn24cn)=(1.0198/1.08988764044943820224719101123595505617977528)

(Nn25) 1(1⅄Q)2nd=(1⅄Qn27cn/1⅄Qn25cn)=(1.0388349514563106796111662136504854368932/1.04123092783505154639175257731958762886597938144329896907216494845360820618)

(Nn26) 1(1⅄Q)2nd=(1⅄Qn28cn/1⅄Qn26cn)=(1.01869158878504672897196261682242990654205607476635514/1.0198)

(Nn27) 1(1⅄Q)2nd=(1⅄Qn29cn/1⅄Qn27cn)=(1.0366972477064220183486238532110091743119266055045871559633027522935779816513758712844/1.0388349514563106796111662136504854368932)

(Nn28) 1(1⅄Q)2nd=(1⅄Qn30cn/1⅄Qn28cn)=(1.^123893805308849557522/1.^01869158878504672897196261682242990654205607476635514)

(Nn29) 1(1⅄Q)2nd=(1⅄Qn31cn/1⅄Qn29cn)=(1.031496062992125984251968503937007874015748/1.0366972477064220183486238532110091743119266055045871559633027522935779816513758712844)

(Nn30) 1(1⅄Q)2nd=(1⅄Qn32cn/1⅄Qn30cn)=(1.045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374/1.123893805308849557522)

(Nn31) 1(1⅄Q)2nd=(1⅄Qn33cn/1⅄Qn31cn)=(1.01459854/1.031496062992125984251968503937007874015748)

(Nn32) 1(1⅄Q)2nd=(1⅄Qn34cn/1⅄Qn32cn)=(1.071942446043165474820143884892086330935251798561151080291955395683453237410/1.045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374)

(Nn33) 1(1⅄Q)2nd=(1⅄Qn35cn/1⅄Qn33cn)=(1.01343624295302/1.01459854)

(Nn34) 1(1⅄Q)2nd=(1⅄Qn36cn/1⅄Qn34cn)=(1.0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894/1.071942446043165474820143884892086330935251798561151080291955395683453237410)

(Nn35) 1(1⅄Q)2nd=(1⅄Qn37cn/1⅄Qn35cn)=(1.038216560509554140127388535031847133757961783439490445859872611464968152866242/1.01343624295302)

(Nn36) 1(1⅄Q)2nd=(1⅄Qn38cn/1⅄Qn36cn)=(1.024539877300613496932515337423312883435582822085889570552147239263803680981595092/1.0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894)

(Nn37) 1(1⅄Q)2nd=(1⅄Qn39cn/1⅄Qn37cn)=(1.0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982/1.038216560509554140127388535031847133757961783439490445859872611464968152866242)

(Nn38) 1(1⅄Q)2nd=(1⅄Qn40cn/1⅄Qn38cn)=(1.034682080924554913294797687861271676300578/1.024539877300613496932515337423312883435582822085889570552147239263803680981595092)

(Nn39) 1(1⅄Q)2nd=(1⅄Qn41cn/1⅄Qn39cn)=(1.0111731843575418994413407821229050279329608936536312849162/1.0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982)

(Nn40) 1(1⅄Q)2nd=(1⅄Qn42cn/1⅄Qn40cn)=(1.005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779/1.034682080924554913294797687861271676300578)

(Nn41) 1(1⅄Q)2nd=(1⅄Qn43cn/1⅄Qn41cn)=(1.01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178/1.0111731843575418994413407821229050279329608936536312849162)

(Nn42) 1(1⅄Q)2nd=(1⅄Qn44cn/1⅄Qn42cn)=(1.02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772/1.005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779)

(Nn43) 1(1⅄Q)2nd=(1⅄Qn45cn/1⅄Qn43cn)=(1.01015228426395939086294416243654822335025380710659898477157360406091370558375634517766497461928934/1.01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178)


And if

13rd=(n4/n1) then 1(1⅄Q)3rd=(1⅄Qn4cn/1⅄Qn1cn)

(Nn1) 1(1⅄Q)3rd=(1⅄Qn4cn/1⅄Qn1cn)=(1.571428/1.5)=1.0476186 and (Nn1) 1(1⅄Q)3rd=(1⅄Qn4c2/1⅄Qn1cn)=(1.571428571428/1.5)=1.0476190476186 and so on for cn variable of (Nn1) 1(1⅄Q)3rd


(Nn2) 1(1⅄Q)3rd=(1⅄Qn5cn/1⅄Qn2cn)=(1.18/1.6)=0.7375 and (Nn2) 1(1⅄Q)3rd=(1⅄Qn5c2/1⅄Qn2cn)=(1.1818/1.6)=0.738625  and so on for cn variable of (Nn2) 1(1⅄Q)3rd


(Nn3) 1(1⅄Q)3rd=(1⅄Qn6cn/1⅄Qn3cn)=(1.307692/1.4)=0.93406571428 and (Nn3) 1(1⅄Q)3rd=(1⅄Qn6c2/1⅄Qn3cn)=(1.307692307692/1.4)=0.934065934065714285  and so on for cn variable of (Nn3) 1(1⅄Q)3rd

(Nn4) 1(1⅄Q)3rd=(1⅄Qn7cn/1⅄Qn4cn)=(1.1176470588235294/1.571428)

(Nn5) 1(1⅄Q)3rd=(1⅄Qn8cn/1⅄Qn5cn)=(1.210526315789473684/1.18)

(Nn6) 1(1⅄Q)3rd=(1⅄Qn9cn/1⅄Qn6cn)=(1.2608695652173913043478/1.307692)

(Nn7) 1(1⅄Q)3rd=(1⅄Qn10cn/1⅄Qn7cn)=(1.0689655172413793103448275862/1.1176470588235294)

(Nn8) 1(1⅄Q)3rd=(1⅄Qn11cn/1⅄Qn8cn)=(1.193548387096774/1.210526315789473684)

(Nn9) 1(1⅄Q)3rd=(1⅄Qn12cn/1⅄Qn9cn)=(1.108/1.2608695652173913043478)

(Nn10) 1(1⅄Q)3rd=(1⅄Qn13cn/1⅄Qn10cn)=(1.04878/1.0689655172413793103448275862)

(Nn11) 1(1⅄Q)3rd=(1⅄Qn14cn/1⅄Qn11cn)=(1.093023255813953488372/1.193548387096774)

(Nn12) 1(1⅄Q)3rd=(1⅄Qn15cn/1⅄Qn12cn)=(1.12765957446808510638297872340425531914893610702/1.108)

(Nn13) 1(1⅄Q)3rd=(1⅄Qn16cn/1⅄Qn13cn)=(1.1132075471698/1.0338983050847457627118644067796610169491525423728813559322)

(Nn14) 1(1⅄Q)3rd=(1⅄Qn17cn/1⅄Qn14cn)=(1.0338983050847457627118644067796610169491525423728813559322/1.093023255813953488372)

(Nn15) 1(1⅄Q)3rd=(1⅄Qn18cn/1⅄Qn15cn)=(1.098360655737704918032786885245901639344262295081967213114754/1.12765957446808510638297872340425531914893610702)

(Nn16) 1(1⅄Q)3rd=(1⅄Qn19cn/1⅄Qn16cn)=(1.059701492537313432835820895522388/1.1132075471698)

(Nn17) 1(1⅄Q)3rd=(1⅄Qn20cn/1⅄Qn17cn)=(1.02816901408450704225352112676056338/1.0338983050847457627118644067796610169491525423728813559322)

(Nn18) 1(1⅄Q)3rd=(1⅄Qn21cn/1⅄Qn18cn)=(1.08219178/1.098360655737704918032786885245901639344262295081967213114754)

(Nn19) 1(1⅄Q)3rd=(1⅄Qn22cn/1⅄Qn19cn)=(1.0506329113924/1.059701492537313432835820895522388)

(Nn20) 1(1⅄Q)3rd=(1⅄Qn23cn/1⅄Qn20cn)=(1.07228915662650602409638554216867469879518/1.02816901408450704225352112676056338)

(Nn21) 1(1⅄Q)3rd=(1⅄Qn24cn/1⅄Qn21cn)=(1.08988764044943820224719101123595505617977528/1.08219178)

(Nn22) 1(1⅄Q)3rd=(1⅄Qn25cn/1⅄Qn22cn)=(1.04123092783505154639175257731958762886597938144329896907216494845360820618/1.0506329113924)

(Nn23) 1(1⅄Q)3rd=(1⅄Qn26cn/1⅄Qn23cn)=(1.0198/1.07228915662650602409638554216867469879518)

(Nn24) 1(1⅄Q)3rd=(1⅄Qn27cn/1⅄Qn24cn)=(1.0388349514563106796111662136504854368932/1.08988764044943820224719101123595505617977528)

(Nn25) 1(1⅄Q)3rd=(1⅄Qn28cn/1⅄Qn25cn)=(1.01869158878504672897196261682242990654205607476635514/1.04123092783505154639175257731958762886597938144329896907216494845360820618)

(Nn26) 1(1⅄Q)3rd=(1⅄Qn29cn/1⅄Qn26cn)=(1.0366972477064220183486238532110091743119266055045871559633027522935779816513758712844/1.0198)

(Nn27) 1(1⅄Q)3rd=(1⅄Qn30cn/1⅄Qn27cn)=(1.123893805308849557522/1.0388349514563106796111662136504854368932)

(Nn28) 1(1⅄Q)3rd=(1⅄Qn31cn/1⅄Qn28cn)=(1.031496062992125984251968503937007874015748/1.01869158878504672897196261682242990654205607476635514)

(Nn29) 1(1⅄Q)3rd=(1⅄Qn32cn/1⅄Qn29cn)=(1.045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374/1.0366972477064220183486238532110091743119266055045871559633027522935779816513758712844)

(Nn30) 1(1⅄Q)3rd=(1⅄Qn33cn/1⅄Qn30cn)=(1.01459854/1.123893805308849557522)

(Nn31) 1(1⅄Q)3rd=(1⅄Qn34cn/1⅄Qn31cn)=(1.071942446043165474820143884892086330935251798561151080291955395683453237410/1.031496062992125984251968503937007874015748)

(Nn32) 1(1⅄Q)3rd=(1⅄Qn35cn/1⅄Qn32cn)=(1.01343624295302/1.045801526717557251908396946564885496183206106870229007633587786259541984732824427480916030534351145038167938931297099236641221374)

(Nn33) 1(1⅄Q)3rd=(1⅄Qn36cn/1⅄Qn33cn)=(1.0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894/1.01459854)

(Nn34) 1(1⅄Q)3rd=(1⅄Qn37cn/1⅄Qn34cn)=(1.038216560509554140127388535031847133757961783439490445859872611464968152866242/1.071942446043165474820143884892086330935251798561151080291955395683453237410)

(Nn35) 1(1⅄Q)3rd=(1⅄Qn38cn/1⅄Qn35cn)=(1.024539877300613496932515337423312883435582822085889570552147239263803680981595092/1.01343624295302)

(Nn36) 1(1⅄Q)3rd=(1⅄Qn39cn/1⅄Qn36cn)=(1.0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982/1.0397350993377483443708609271523178807284768211920529801324503311258278145695364238410596026490066225165562913907218543046357615894)

(Nn37) 1(1⅄Q)3rd=(1⅄Qn40cn/1⅄Qn37cn)=(1.034682080924554913294797687861271676300578/1.038216560509554140127388535031847133757961783439490445859872611464968152866242)

(Nn38) 1(1⅄Q)3rd=(1⅄Qn41cn/1⅄Qn38cn)=(1.0111731843575418994413407821229050279329608936536312849162/1.024539877300613496932515337423312883435582822085889570552147239263803680981595092)

(Nn39) 1(1⅄Q)3rd=(1⅄Qn42cn/1⅄Qn39cn)=(1.005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779/1.0359281437125748502994011976047904191616766467065868263473053892215568862275449101796407185628742514970059880239520958083832335329341317365269461077844311377245508982)

(Nn40) 1(1⅄Q)3rd=(1⅄Qn43cn/1⅄Qn40cn)=(1.01047120418848167539267015706806282722513089005235602094240837696335078534031413612565445026178/1.034682080924554913294797687861271676300578)

(Nn41) 1(1⅄Q)3rd=(1⅄Qn44cn/1⅄Qn41cn)=(1.02072538860103626943005181347150259067357512953367875647668393782383419689119170984455958549222797927461139896373069948186528497409326424870466321243523316062176165803108808290155440414507772/1.0111731843575418994413407821229050279329608936536312849162)

(Nn42) 1(1⅄Q)3rd=(1⅄Qn45cn/1⅄Qn42cn)=(1.01015228426395939086294416243654822335025380710659898477157360406091370558375634517766497461928934/1.005524861878453038674033149171270718232044198895027624309392265193370165745856353591160220994475138121546961325966850828729281767955801104972375690607734806629834254143646408839779)


Then if

12nd=(n3/n1) then 1(2⅄Q)2nd=(2⅄Qn3cn/2⅄Qn1cn)

(Nn1) 1(2⅄Q)2nd=(2⅄Qn3cn/2⅄Qn1cn)=(0.714285/0.6)

(Nn2) 1(2⅄Q)2nd=(2⅄Qn4cn/2⅄Qn2cn)=(0.63/0.6)

(Nn3) 1(2⅄Q)2nd=(2⅄Qn5cn/2⅄Qn3cn)=(0.846153/0.714285)

(Nn4) 1(2⅄Q)2nd=(2⅄Qn6cn/2⅄Qn4cn)=(0.7647058823529411/0.63)

(Nn5) 1(2⅄Q)2nd=(2⅄Qn7cn/2⅄Qn5cn)=(0.894736842105263157/0.846153)

(Nn6) 1(2⅄Q)2nd=(2⅄Qn8cn/2⅄Qn6cn)=(0.8260869565217391304347/0.7647058823529411 )

(Nn7) 1(2⅄Q)2nd=(2⅄Qn9cn/2⅄Qn7cn)=(0.7931034482758620689655172413/0.894736842105263157)

(Nn8) 1(2⅄Q)2nd=(2⅄Qn10cn/2⅄Qn8cn)=(0.935483870967741/0.8260869565217391304347)

(Nn9) 1(2⅄Q)2nd=(2⅄Qn11cn/2⅄Qn9cn)=(0.837/0.7931034482758620689655172413)

(Nn10) 1(2⅄Q)2nd=(2⅄Qn12cn/2⅄Qn10cn)=(0.9024390243/0.935483870967741)

(Nn11) 1(2⅄Q)2nd=(2⅄Qn13cn/2⅄Qn11cn)=(0.953488372093023255813/0.837)

(Nn12) 1(2⅄Q)2nd=(2⅄Qn14cn/2⅄Qn12cn)=(0.9148936170212765957446808510638297872340425531/0.9024390243)

(Nn13) 1(2⅄Q)2nd=(2⅄Qn15cn/2⅄Qn13cn)=(0.88679245283018867924528301/0.953488372093023255813)

(Nn14) 1(2⅄Q)2nd=(2⅄Qn16cn/2⅄Qn14cn)=(0.8983050847457627118644067796610169491525423728813559322033/0.9148936170212765957446808510638297872340425531)

(Nn15) 1(2⅄Q)2nd=(2⅄Qn17cn/2⅄Qn15cn)=(0.967213114754098360655737704918032786885245901639344262295081/0.88679245283018867924528301)

(Nn16) 1(2⅄Q)2nd=(2⅄Qn18cn/2⅄Qn16cn)=(0.910447761194029850746268656716417/0.8983050847457627118644067796610169491525423728813559322033)

(Nn17) 1(2⅄Q)2nd=(2⅄Qn19cn/2⅄Qn17cn)=(0.94366197183098591549295774647887323/0.967213114754098360655737704918032786885245901639344262295081)

(Nn18) 1(2⅄Q)2nd=(2⅄Qn20cn/2⅄Qn18cn)=(0.97260273/0.910447761194029850746268656716417)

(Nn19) 1(2⅄Q)2nd=(2⅄Qn21cn/2⅄Qn19cn)=(0.9240506329113/0.94366197183098591549295774647887323)

(Nn20) 1(2⅄Q)2nd=(2⅄Qn22cn/2⅄Qn20cn)=(0.95180722891566265060240963855421686746987/0.97260273)

(Nn21) 1(2⅄Q)2nd=(2⅄Qn23cn/2⅄Qn21cn)=(0.93258426966292134831460674157303370786516853/0.9240506329113)

(Nn22) 1(2⅄Q)2nd=(2⅄Qn24cn/2⅄Qn22cn)=(0.917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463/0.95180722891566265060240963855421686746987)

(Nn23) 1(2⅄Q)2nd=(2⅄Qn25cn/2⅄Qn23cn)=(0.9603/0.93258426966292134831460674157303370786516853)

(Nn24) 1(2⅄Q)2nd=(2⅄Qn26cn/2⅄Qn24cn)=(0.9805825242718446601941747572815533/0.917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463)

(Nn25) 1(2⅄Q)2nd=(2⅄Qn27cn/2⅄Qn25cn)=(0.96261682242990654205607476635514018691588785046728971/0.9603)

(Nn26) 1(2⅄Q)2nd=(2⅄Qn28cn/2⅄Qn26cn)=(0.0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577/0.9805825242718446601941747572815533)

(Nn27) 1(2⅄Q)2nd=(2⅄Qn29cn/2⅄Qn27cn)=(0.9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707/0.96261682242990654205607476635514018691588785046728971)

(Nn28) 1(2⅄Q)2nd=(2⅄Qn30cn/2⅄Qn28cn)=(0.88976377952755905511811023622047244094481/0.0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577)

(Nn29) 1(2⅄Q)2nd=(2⅄Qn31cn/2⅄Qn29cn)=(0.969465648854961832061068015267175572519083/0.9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707)

(Nn30) 1(2⅄Q)2nd=(2⅄Qn32cn/2⅄Qn30cn)=(0.95620437/0.88976377952755905511811023622047244094481)

(Nn31) 1(2⅄Q)2nd=(2⅄Qn33cn/2⅄Qn31cn)=(0.9856115107913669064748201438848920863309352517/0.969465648854961832061068015267175572519083)

(Nn32) 1(2⅄Q)2nd=(2⅄Qn34cn/2⅄Qn32cn)=(0.932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489/0.95620437)

(Nn33) 1(2⅄Q)2nd=(2⅄Qn35cn/2⅄Qn33cn)=(0.986754966887417218543046357615894039735099337748344370860927152317880794701/0.9856115107913669064748201438848920863309352517)

(Nn34) 1(2⅄Q)2nd=(2⅄Qn36cn/2⅄Qn34cn)=(0.961783439490445859872611464968152866242038216560509554140127388535031847133757/0.932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489)

(Nn35) 1(2⅄Q)2nd=(2⅄Qn37cn/2⅄Qn35cn)=(0.963190184049079754601226993865030674846625766871165644171779141104294478527607361/0.986754966887417218543046357615894039735099337748344370860927152317880794701)

(Nn36) 1(2⅄Q)2nd=(2⅄Qn38cn/2⅄Qn36cn)=(0.9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011/0.961783439490445859872611464968152866242038216560509554140127388535031847133757)

(Nn37) 1(2⅄Q)2nd=(2⅄Qn39cn/2⅄Qn37cn)=(0.9653179190751445086705202312138728323699421/0.963190184049079754601226993865030674846625766871165644171779141104294478527607361)

(Nn38) 1(2⅄Q)2nd=(2⅄Qn40cn/2⅄Qn38cn)=(0.96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513/0.9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011)

(Nn39) 1(2⅄Q)2nd=(2⅄Qn41cn/2⅄Qn39cn)=(0.^9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441/0.^9653179190751445086705202312138728323699421)

(Nn40) 1(2⅄Q)2nd=(2⅄Qn42cn/2⅄Qn40cn)=(0.94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109/0.96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513)

(Nn41) 1(2⅄Q)2nd=(2⅄Qn43cn/2⅄Qn41cn)=(0.989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113/0.9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441)

(Nn42) 1(2⅄Q)2nd=(2⅄Qn44cn/2⅄Qn42cn)=(0.979695431/0.94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109)

(Nn43) 1(2⅄Q)2nd=(2⅄Qn45cn/2⅄Qn43cn)=(0.989949748743718592964824120603015075025125628140703517587939698492462311557763819095477386934673366834170854271356783919597/0.989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113)


And if

13rd=(n4/n1) then 1(2⅄Q)3rd=(2⅄Qn4cn/2⅄Qn1cn)

(Nn1) 1(2⅄Q)3rd=(2⅄Qn4cn/2⅄Qn1cn)=(0.63/0.6)

(Nn2) 1(2⅄Q)3rd=(2⅄Qn5cn/2⅄Qn2cn)=(0.846153/0.6)

(Nn3) 1(2⅄Q)3rd=(2⅄Qn6cn/2⅄Qn3cn)=(0.7647058823529411/0.714285)

(Nn4) 1(2⅄Q)3rd=(2⅄Qn7cn/2⅄Qn4cn)=(0.894736842105263157/0.63)

(Nn5) 1(2⅄Q)3rd=(2⅄Qn8cn/2⅄Qn5cn)=(0.8260869565217391304347/0.846153)

(Nn6) 1(2⅄Q)3rd=(2⅄Qn9cn/2⅄Qn6cn)=(0.7931034482758620689655172413/0.7647058823529411)

(Nn7) 1(2⅄Q)3rd=(2⅄Qn10cn/2⅄Qn7cn)=(0.935483870967741/0.894736842105263157)

(Nn8) 1(2⅄Q)3rd=(2⅄Qn11cn/2⅄Qn8cn)=(0.837/0.8260869565217391304347)

(Nn9) 1(2⅄Q)3rd=(2⅄Qn12cn/2⅄Qn9cn)=(0.9024390243/0.7931034482758620689655172413)

(Nn10) 1(2⅄Q)3rd=(2⅄Qn13cn/2⅄Qn10cn)=(0.953488372093023255813/0.935483870967741)

(Nn11) 1(2⅄Q)3rd=(2⅄Qn14cn/2⅄Qn11cn)=(0.9148936170212765957446808510638297872340425531/0.837)

(Nn12) 1(2⅄Q)3rd=(2⅄Qn15cn/2⅄Qn12cn)=(0.88679245283018867924528301/0.9024390243)

(Nn13) 1(2⅄Q)3rd=(2⅄Qn16cn/2⅄Qn13cn)=(0.8983050847457627118644067796610169491525423728813559322033/0.953488372093023255813)

(Nn14) 1(2⅄Q)3rd=(2⅄Qn17cn/2⅄Qn14cn)=(0.967213114754098360655737704918032786885245901639344262295081/0.9148936170212765957446808510638297872340425531)

(Nn15) 1(2⅄Q)3rd=(2⅄Qn18cn/2⅄Qn15cn)=(0.910447761194029850746268656716417/0.88679245283018867924528301)

(Nn16) 1(2⅄Q)3rd=(2⅄Qn19cn/2⅄Qn16cn)=(0.94366197183098591549295774647887323/0.8983050847457627118644067796610169491525423728813559322033)

(Nn17) 1(2⅄Q)3rd=(2⅄Qn20cn/2⅄Qn17cn)=(0.97260273/0.967213114754098360655737704918032786885245901639344262295081)

(Nn18) 1(2⅄Q)3rd=(2⅄Qn21cn/2⅄Qn18cn)=(0.9240506329113/0.910447761194029850746268656716417)

(Nn19) 1(2⅄Q)3rd=(2⅄Qn22cn/2⅄Qn19cn)=(0.95180722891566265060240963855421686746987/0.94366197183098591549295774647887323)

(Nn20) 1(2⅄Q)3rd=(2⅄Qn23cn/2⅄Qn20cn)=(0.93258426966292134831460674157303370786516853/0.97260273)

(Nn21) 1(2⅄Q)3rd=(2⅄Qn24cn/2⅄Qn21cn)=(0.917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463/0.9240506329113)

(Nn22) 1(2⅄Q)3rd=(2⅄Qn25cn/2⅄Qn22cn)=(0.9603/0.95180722891566265060240963855421686746987)

(Nn23) 1(2⅄Q)3rd=(2⅄Qn26cn/2⅄Qn23cn)=(0.9805825242718446601941747572815533/0.93258426966292134831460674157303370786516853)

(Nn24) 1(2⅄Q)3rd=(2⅄Qn27cn/2⅄Qn24cn)=(0.96261682242990654205607476635514018691588785046728971/0.917525773195876288659793814432989690721649484536082474226804123711340206185567010309278350515463)

(Nn25) 1(2⅄Q)3rd=(2⅄Qn28cn/2⅄Qn25cn)=(0.0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577/0.9603)

(Nn26) 1(2⅄Q)3rd=(2⅄Qn29cn/2⅄Qn26cn)=(0.9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707/0.9805825242718446601941747572815533)

(Nn27) 1(2⅄Q)3rd=(2⅄Qn30cn/2⅄Qn27cn)=(0.88976377952755905511811023622047244094481/0.96261682242990654205607476635514018691588785046728971)

(Nn28) 1(2⅄Q)3rd=(2⅄Qn31cn/2⅄Qn28cn)=(0.969465648854961832061068015267175572519083/0.0981651376146788990825688073394495412844036697247706422018348623853211009174311926605504587155963302752293577)

(Nn29) 1(2⅄Q)3rd=(2⅄Qn32cn/2⅄Qn29cn)=(0.95620437/0.9646017699115044247787610619469026548672566371681415929203539823008849557522123893805309734513274336283185840707)

(Nn30) 1(2⅄Q)3rd=(2⅄Qn33cn/2⅄Qn30cn)=(0.9856115107913669064748201438848920863309352517/0.88976377952755905511811023622047244094481)

(Nn31) 1(2⅄Q)3rd=(2⅄Qn34cn/2⅄Qn31cn)=(0.932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489/0.969465648854961832061068015267175572519083)

(Nn32) 1(2⅄Q)3rd=(2⅄Qn35cn/2⅄Qn32cn)=(0.986754966887417218543046357615894039735099337748344370860927152317880794701/0.95620437)

(Nn33) 1(2⅄Q)3rd=(2⅄Qn36cn/2⅄Qn33cn)=(0.961783439490445859872611464968152866242038216560509554140127388535031847133757/0.9856115107913669064748201438848920863309352517)

(Nn34) 1(2⅄Q)3rd=(2⅄Qn37cn/2⅄Qn34cn)=(0.963190184049079754601226993865030674846625766871165644171779141104294478527607361/0.932885906040268456375838926174496651006711409395973154362416107382550335570469798657718120805369127516778523489)

(Nn35) 1(2⅄Q)3rd=(2⅄Qn38cn/2⅄Qn35cn)=(0.9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011/0.986754966887417218543046357615894039735099337748344370860927152317880794701)

(Nn36) 1(2⅄Q)3rd=(2⅄Qn39cn/2⅄Qn36cn)=(0.9653179190751445086705202312138728323699421/0.961783439490445859872611464968152866242038216560509554140127388535031847133757)

(Nn37) 1(2⅄Q)3rd=(2⅄Qn40cn/2⅄Qn37cn)=(0.96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513/0.963190184049079754601226993865030674846625766871165644171779141104294478527607361)

(Nn38) 1(2⅄Q)3rd=(2⅄Qn41cn/2⅄Qn38cn)=(0.9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441/0.9760479041916167664670658682634730538922155688622754491017964071856287425149700598802395209580838323353293413173652694610778443113772455089820359281437125748502994011)

(Nn39) 1(2⅄Q)3rd=(2⅄Qn42cn/2⅄Qn39cn)=(0.94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109/0.9653179190751445086705202312138728323699421)

(Nn40) 1(2⅄Q)3rd=(2⅄Qn43cn/2⅄Qn40cn)=(0.989637304699481864284974093264248704663212435233160621761658031088082901554404145077720207253886010362694300518134715025906735751295336787564766839378238341917098445595854922279792746113/0.96648044692737430167597765363128491620111731843575418994413407821229050279329608938547486033519553072625698324022346336871508379888268156424581005586592178770949720670391061452513)

(Nn41) 1(2⅄Q)3rd=(2⅄Qn44cn/2⅄Qn41cn)=(0.979695431/0.9889502762430939226519337016574585635359116022099447513812154696132596685082877292817679558011049723756906077348066298342541436464088397790055248618784530386740331491712707182320441)

(Nn42) 1(2⅄Q)3rd=(2⅄Qn45cn/2⅄Qn42cn)=(0.989949748743718592964824120603015075025125628140703517587939698492462311557763819095477386934673366834170854271356783919597/0.94764397905759162303664921465968586387434554973821989528795811518324607329842931937172774869109)


ALTERNATE PATH

if

22nd=(n1/n3) then 2φ2nd=(φn1cn/φn3cn) rather than 12nd=(n3/n1) being 1φ2nd=(φn3cn/φn1cn)

so

(Nn1) 2φ2nd=(φn1cn/φn3cn)=(0/2)=0

(Nn2) 2φ2nd=(φn2cn/φn4cn)=(1/1.5)=0.6 or 0.66 or 0.666 or 0.6666 . . . and so on

(Nn3) 2φ2nd=(φn3cn/φn5cn)=(2/1.6)=1.25 and (Nn3) 2φ2nd=(φn3cn/φn5c2)=(2/1.66)=1.204819277108433734939759036144578313253012048192771084337349397590361445783132530 

or 1.2048192771084337349397590361445783132530120481927710843373493975903614457831325301204819277108433734939759036144578313253012048192771084337349397590361445783132530 

and (Nn3) 2φ2nd=(φn3cn/φn5c3)=(2/1.666)=1.20048019207683073229291716686674669867947178871548619447779111644657863145258103241296518607442977190876350540216086434573829531812725090036014405762304921968787515006002400960384153661464585834333733493397358943577430972388955582232893157262905162064825930372148859543817527010804321728691476590636254501800720288115246098439375750300

or

1.20048019207683073229291716686674669867947178871548619447779111644657863145258103241296518607442977190876350540216086434573829531812725090036014405762304921968787515006002400960384153661464585834333733493397358943577430972388955582232893157262905162064825930372148859543817527010804321728691476590636254501800720288115246098439375750300120048019207683073229291716686674669867947178871548619447779111644657863145258103241296518607442977190876350540216086434573829531812725090036014405762304921968787515006002400960384153661464585834333733493397358943577430972388955582232893157262905162064825930372148859543817527010804321728691476590636254501800720288115246098439375750300 . . . and so on

(Nn4) 2φ2nd=(φn4cn/φn6cn)=(1.5/1.6)=0.9375

(Nn5) 2φ2nd=(φn5cn/φn7cn)=(1.6/1.625)=0.9846153 and (Nn5) 2φ2nd=(φn5c2/φn7cn)=(1.66/1.625)=1.02153846 and  (Nn5) 2φ2nd=(φn5c3/φn7cn)=(1.666/1.625)=1.025230769 and so on for cn variable of (Nn5) 2φ2nd

(Nn6) 2φ2nd=(φn6cn/φn8cn)=(1.6/1.615384)

(Nn7) 2φ2nd=(φn7cn/φn9cn)=(1.625/1.619047)

(Nn8) 2φ2nd=(φn8cn/φn10cn)=(1.615384/1.61762941)

(Nn9) 2φ2nd=(φn9cn/φn11cn)=(1.619047/1.618)

(Nn10) 2φ2nd=(φn10cn/φn12cn)=(1.61762941/1.61797752808988764044943820224719101123595505)

(Nn11) 2φ2nd=(φn11cn/φn13cn)=(1.618/1.61805)

(Nn12) 2φ2nd=(φn12cn/φn14cn)=(1.61797752808988764044943820224719101123595505/1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

(Nn13) 2φ2nd=(φn13cn/φn15cn)=(1.61805/1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

(Nn14) 2φ2nd=(φn14cn/φn16cn)=(1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/1.618032786885245901639344262295081967213114754098360655737704918)

(Nn15) 2φ2nd=(φn15cn/φn17cn)=(1.61830223896551724135014/1.618032786885245901639344262295081967213114754098360655737704918)

(Nn16) 2φ2nd=(φn16cn/φn18cn)=(1.618032786885245901639344262295081967213114754098360655737704918/1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn17) 2φ2nd=(φn17cn/φn19cn)=(1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843/1.618034055731424148606811145510835913312693)

(Nn18) 2φ2nd=(φn18cn/φn20cn)=(1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242)

(Nn19) 2φ2nd=(φn19cn/φn21cn)=(1.618034055731424148606811145510835913312693/1.61803399852)

(Nn20) 2φ2nd=(φn20cn/φn22cn)=(1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.6180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981)

(Nn21) 2φ2nd=(φn21cn/φn23cn)=(1.61803399852/1.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793292304217717802495624188357517983174298458585060132121280560103890237705381401388967308452374230704082208796792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869)

(Nn22) 2φ2nd=(φn22cn/φn24cn)

(Nn23) 2φ2nd=(φn23cn/φn25cn)

(Nn24) 2φ2nd=(φn24cn/φn26cn)

(Nn25) 2φ2nd=(φn25cn/φn27cn)

(Nn26) 2φ2nd=(φn26cn/φn28cn)

(Nn27) 2φ2nd=(φn27cn/φn29cn)

(Nn28) 2φ2nd=(φn28cn/φn30cn)

(Nn29) 2φ2nd=(φn29cn/φn31cn)

(Nn30) 2φ2nd=(φn30cn/φn32cn)

(Nn31) 2φ2nd=(φn31cn/φn33cn)

(Nn32) 2φ2nd=(φn32cn/φn34cn)

(Nn33) 2φ2nd=(φn33cn/φn35cn)

(Nn34) 2φ2nd=(φn34cn/φn36cn)

(Nn35) 2φ2nd=(φn35cn/φn37cn)

(Nn36) 2φ2nd=(φn36cn/φn38cn)

(Nn37) 2φ2nd=(φn37cn/φn39cn)

(Nn38) 2φ2nd=(φn38cn/φn40cn)

(Nn39) 2φ2nd=(φn39cn/φn41cn)

(Nn40) 2φ2nd=(φn40cn/φn42cn)

(Nn41) 2φ2nd=(φn41cn/φn43cn)

(Nn42) 2φ2nd=(φn42cn/φn44cn)

(Nn43) 2φ2nd=(φn43cn/φn45cn)


And if

23rd=(n1/n4) then 2φ3rd=(φn1cn/φn4cn)

(Nn1) 2φ3rd=(φn1cn/φn4cn)=(0/1.5)=0

(Nn2) 2φ3rd=(φn2cn/φn5cn)=(1/1.6)=0.625 and (Nn2) 2φ3rd=(φn2cn/φn5c2)=(1/1.66)=0.6024096385542168674698795180722891566265

(Nn3) 2φ3rd=(φn3cn/φn6cn)=(2/1.6)=1.25

(Nn4) 2φ3rd=(φn4cn/φn7cn)=(1.5/1.625)=0.923076

(Nn5) 2φ3rd=(φn5cn/φn8cn)=(1.6/1.615384)

(Nn6) 2φ3rd=(φn6cn/φn9cn)=(1.6/1.619047)

(Nn7) 2φ3rd=(φn7cn/φn10cn)=(1.625/1.61762941)

(Nn8) 2φ3rd=(φn8cn/φn11cn)=(1.615384/1.618)

(Nn9) 2φ3rd=(φn9cn/φn12cn)=(1.619047/1.61797752808988764044943820224719101123595505)

(Nn10) 2φ3rd=(φn10cn/φn13cn)=(1.61762941/1.61805)

(Nn11) 2φ3rd=(φn11cn/φn14cn)=(1.618/1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832)

(Nn12) 2φ3rd=(φn12cn/φn15cn)=(1.61797752808988764044943820224719101123595505/1.61830223896551724135014)

(Nn13) 2φ3rd=(φn13cn/φn16cn)=(1.61805/1.618032786885245901639344262295081967213114754098360655737704918)

(Nn14) 2φ3rd=(φn14cn/φn17cn)=(1.61802575107296137339055793991416738197424034334763948497854077253214592274678111587982832/1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843)

(Nn15) 2φ3rd=(φn15cn/φn18cn)=(1.61830223896551724135014/1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn16) 2φ3rd=(φn16cn/φn19cn)=(1.618032786885245901639344262295081967213114754098360655737704918/1.618034055731424148606811145510835913312693)

(Nn17) 2φ3rd=(φn17cn/φn20cn)=(1.6180344478216818642350572441742654508601925025329280648429584599797365754812563323201418439716312056737588652482269503546099290780141843/1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242)

(Nn18) 2φ3rd=(φn18cn/φn21cn)=(1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/1.61803399852)

(Nn19) 2φ3rd=(φn19cn/φn22cn)=(1.618034055731424148606811145510835913312693/1.6180339985010049351361227845806687374385163530970217431207747140526219623606797003471770509775260369084598940279554176959619952494246310067604604606248876201845441458249607162433948492782751690115110542682258359217979170473415128814180522565320665083135391923990498995066691028686278092454048985930933674403617759848364701260734516627078384799926913941183994154944291065229307509492545240288598574823679883062305865164445660515253974056276265302393568427005298739265485291430842335099579755161702905171752247414776521152932578110725379133930202813813265119678421523844346811620683354651927644821852731591449132103051342974604423716426274440178896400694319386077105773798647926365795724284672026310981)

(Nn20) 2φ3rd=(φn20cn/φn23cn)=(1.61803396316670629036115761779478593637885673283903372398947620186558239655584788327911265247548433389141353743123654628079406840468787371442238722793590050227218368811289165271466156421908634298014828988280315713944032525711552260224826596508012437215977038985864625687634537192059315953121262855776130112413298254006218607986127720640994977278163118631906242/1.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793292304217717802495624188357517983174298458585060132121280560103890237705381401388967308452374230704082208796792953531703461125853989046355372367455253797075263960250691660549940714810005081587713850149624527130032183388854384280955338490203828129411100446050477104624244819603636158319631867201174411382756479024335158940771272090791033820789339958218056575009880864999153068713229066681723222855852295183784088984247078087064536163965896900231494551408729038450680368132798825588617245152729941844051719270509852633956298345660324092371972220653830987894528823894754672237592456665349218000112924171418892213878380667381853085652984021229744226751736209135565467788380102760995991191914629326407217486307944215459319067246344079950313364575687425893512506351984642312687030688912540229236067980351194173112754785161763875557563096380780306024504545197899610411608604821862119586697532606854497205126757382417706510078482299136130094291434701597877025577324826379086443453221161989723900400880808537067359268251369205578454068093275365592004968663542431257410648749364801535768731296934108745977076393201964880582688724521483823612444243690361921969397549528541584326125007057760713680763367398791711365817853311501326859014171983513070972841736773755642256224944949466433290045734289424651346620744170289650499689458528598046411834453164699904014454293941618203376432725424877194963581954717407261024222234769352375876912653153407486872565072553780136639376658573767714979391338716052170967195528202811811868330416135571678617808141832759302128620631246118231607475580147930664558748800169386257156565363107673197447913725933035966347596917170120264242561120207780475410761673536220427982609677601490599062729377223197624809440460730619389080232623793122917980589464174806617356445147083733273107108576590819264863644063011687651741798882050702952967082604031392919654452035458189825532155157811529563548077465981593360058720569137823951216757947038563604539551691039466997910902828750494043249957653435317915419795607249731805092880130992038844785726384732652024165772683642933769973462819715995708881486082095872621534639789582745186607193269713737225453108237818305008187002427869)

(Nn21) 2φ3rd=(φn21cn/φn24cn)

(Nn22) 2φ3rd=(φn22cn/φn25cn)

(Nn23) 2φ3rd=(φn23cn/φn26cn)

(Nn24) 2φ3rd=(φn24cn/φn27cn)

(Nn25) 2φ3rd=(φn25cn/φn28cn)

(Nn26) 2φ3rd=(φn26cn/φn29cn)

(Nn27) 2φ3rd=(φn27cn/φn30cn)

(Nn28) 2φ3rd=(φn28cn/φn31cn)

(Nn29) 2φ3rd=(φn29cn/φn32cn)

(Nn30) 2φ3rd=(φn30cn/φn33cn)

(Nn31) 2φ3rd=(φn31cn/φn34cn)

(Nn32) 2φ3rd=(φn32cn/φn35cn)

(Nn33) 2φ3rd=(φn33cn/φn36cn)

(Nn34) 2φ3rd=(φn34cn/φn37cn)

(Nn35) 2φ3rd=(φn35cn/φn38cn)

(Nn36) 2φ3rd=(φn36cn/φn39cn)

(Nn37) 2φ3rd=(φn37cn/φn40cn)

(Nn38) 2φ3rd=(φn38cn/φn41cn)

(Nn39) 2φ3rd=(φn39cn/φn42cn)

(Nn40) 2φ3rd=(φn40cn/φn43cn)

(Nn41) 2φ3rd=(φn41cn/φn44cn)

(Nn42) 2φ3rd=(φn42cn/φn45cn)


Then if

22nd=(n1/n3) then 2Θ2nd=(Θn1cn/Θn3cn)

(Nn1) 2Θ2nd=(Θn1cn/Θn3cn)=(0/0.5)=0

(Nn2) 2Θ2nd=(Θn2cn/Θn4cn)=(1/0.6)

(Nn3) 2Θ2nd=(Θn3cn/Θn5cn)=(0.5/0.6)

(Nn4) 2Θ2nd=(Θn4cn/Θn6cn)=(0.6/0.625)

(Nn5) 2Θ2nd=(Θn5cn/Θn7cn)=(0.6/0.615384)

(Nn6) 2Θ2nd=(Θn6cn/Θn8cn)=(0.625/0.619047)

(Nn7) 2Θ2nd=(Θn7cn/Θn9cn)=(0.615384/0.61764705882352941)

(Nn8) 2Θ2nd=(Θn8cn/Θn10cn)=(0.619047/0.618)

(Nn9) 2Θ2nd=(Θn9cn/Θn11cn)=(0.61764705882352941/0.6179775280878651685393258764044943820224719101123595505)

(Nn10) 2Θ2nd=(Θn10cn/Θn12cn)=(0.618/0.61805)

(Nn11) 2Θ2nd=(Θn11cn/Θn13cn)=(0.6179775280878651685393258764044943820224719101123595505/0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566)

(Nn12) 2Θ2nd=(Θn12cn/Θn14cn)=(0.61805/0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

(Nn13) 2Θ2nd=(Θn13cn/Θn15cn)=(0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566/0.618032786885245901639344262295081967213114754098360655737749)

(Nn14) 2Θ2nd=(Θn14cn/Θn16cn)=(0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

(Nn15) 2Θ2nd=(Θn15cn/Θn17cn)=(0.618032786885245901639344262295081967213114754098360655737749/0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn16) 2Θ2nd=(Θn16cn/Θn18cn)=(0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

(Nn17) 2Θ2nd=(Θn17cn/Θn19cn)=(0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

(Nn18) 2Θ2nd=(Θn18cn/Θn20cn)=(0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/0.61803399852)

(Nn19) 2Θ2nd=(Θn19cn/Θn21cn)=(0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/0.6180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981)

(Nn20) 2Θ2nd=(Θn20cn/Θn22cn)=(0.61803399852/0.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114)

(Nn21) 2Θ2nd=(Θn21cn/Θn23cn)

(Nn22) 2Θ2nd=(Θn22cn/Θn24cn)

(Nn23) 2Θ2nd=(Θn23cn/Θn25cn)

(Nn24) 2Θ2nd=(Θn24cn/Θn26cn)

(Nn25) 2Θ2nd=(Θn25cn/Θn27cn)

(Nn26) 2Θ2nd=(Θn26cn/Θn28cn)

(Nn27) 2Θ2nd=(Θn27cn/Θn29cn)

(Nn28) 2Θ2nd=(Θn28cn/Θn30cn)

(Nn29) 2Θ2nd=(Θn29cn/Θn31cn)

(Nn30) 2Θ2nd=(Θn30cn/Θn32cn)

(Nn31) 2Θ2nd=(Θn31cn/Θn33cn)

(Nn32) 2Θ2nd=(Θn32cn/Θn34cn)

(Nn33) 2Θ2nd=(Θn33cn/Θn35cn)

(Nn34) 2Θ2nd=(Θn34cn/Θn36cn)

(Nn35) 2Θ2nd=(Θn35cn/Θn37cn)

(Nn36) 2Θ2nd=(Θn36cn/Θn38cn)

(Nn37) 2Θ2nd=(Θn37cn/Θn39cn)

(Nn38) 2Θ2nd=(Θn38cn/Θn40cn)

(Nn39) 2Θ2nd=(Θn39cn/Θn41cn)

(Nn40) 2Θ2nd=(Θn40cn/Θn42cn)

(Nn41) 2Θ2nd=(Θn41cn/Θn43cn)

(Nn42) 2Θ2nd=(Θn42cn/Θn44cn)

(Nn43) 2Θ2nd=(Θn43cn/Θn45cn)

And if

23rd=(n1/n4) then 2Θ3rd=(Θn1cn/Θn4cn)

(Nn1) 2Θ3rd=(Θn1cn/Θn4cn)=(0/0.6)

(Nn2) 2Θ3rd=(Θn2cn/Θn5cn)=(1/0.6)

(Nn3) 2Θ3rd=(Θn3cn/Θn6cn)=(0.5/0.625)

(Nn4) 2Θ3rd=(Θn4cn/Θn7cn)=(0.6/0.615384)

(Nn5) 2Θ3rd=(Θn5cn/Θn8cn)=(0.6/0.619047)

(Nn6) 2Θ3rd=(Θn6cn/Θn9cn)=(0.625/0.61764705882352941)

(Nn7) 2Θ3rd=(Θn7cn/Θn10cn)=(0.615384/0.618)

(Nn8) 2Θ3rd=(Θn8cn/Θn11cn)=(0.619047/0.6179775280878651685393258764044943820224719101123595505)

(Nn9) 2Θ3rd=(Θn9cn/Θn12cn)=(0.61764705882352941/0.61805)

(Nn10) 2Θ3rd=(Θn10cn/Θn13cn)=(0.618/0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566)

(Nn11) 2Θ3rd=(Θn11cn/Θn14cn)=(0.6179775280878651685393258764044943820224719101123595505/0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257)

(Nn12) 2Θ3rd=(Θn12cn/Θn15cn)=(0.61805/0.618032786885245901639344262295081967213114754098360655737749)

(Nn13) 2Θ3rd=(Θn13cn/Θn16cn)=(0.618025755364806437768240343347639484978540772532206008583690987124463519313304721030042918454935622317596566/0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870)

(Nn14) 2Θ3rd=(Θn14cn/Θn17cn)=(0.610079575596814323607427055702917771827585941644562334217506631294429708196286206893896551724137931034482493368673740053050397875331564986472148514588567639257/0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129)

(Nn15) 2Θ3rd=(Θn15cn/Θn18cn)=(0.618032786885245901639344262295081967213114754098360655737749/0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743)

(Nn16) 2Θ3rd=(Θn16cn/Θn19cn)=(0.618034447821681864235055724417426545086119554204660587639311043566362715298885511651469098277608915906788247213779128672745684022289766870/0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936)

(Nn17) 2Θ3rd=(Θn17cn/Θn20cn)=(0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129/0.61803399852)

(Nn18) 2Θ3rd=(Θn18cn/Θn21cn)=(0.618034055727554179566563467492260061919504643962848297213622291021671826625386996904024767801857585139318885448916408668730650154798761609907120743/0.6180339850173579389731408733784030696144710396491869175954686643522748035812168828795907180705280467750776539375114196966928558377489493879042572629270966563128083318107071076192216334734149460990316097204458249588890919057189841037822035446738534624520372738900054814544125708021194957061940434862050063950301479992691394116572263840672391741275351726658139959802667641147451123698154577014434496619769778914672026310981)

(Nn19) 2Θ3rd=(Θn19cn/Θn22cn)=(0.618033963166706529538387945467591485290600334848122458741927768476441042812724228653432193255202104759626883520688830423343697679980865821573786175556087060511839272901219803874671131308299449892370246352547237502989715379095910069361396795025113609184405644582635733078210954317149007414494140157856972016264051662281750777325998564936/0.618033990175597086556377392580881937778781548190390153012252272598949805205804302410931059793348766303427248602563378691208853255039241149568065044322737281915193947264411947377336118796228332674609000056462085709446106939190333690926542826492010614872113375868104567782733894190051380497995595957314663203658743153972107729659533623172039975156682287843712946756253175992321156343515329456270114)

(Nn20) 2Θ3rd=(Θn20cn/Θn23cn)

(Nn21) 2Θ3rd=(Θn21cn/Θn24cn)

(Nn22) 2Θ3rd=(Θn22cn/Θn25cn)

(Nn23) 2Θ3rd=(Θn23cn/Θn26cn)

(Nn24) 2Θ3rd=(Θn24cn/Θn27cn)

(Nn25) 2Θ3rd=(Θn25cn/Θn28cn)

(Nn26) 2Θ3rd=(Θn26cn/Θn29cn)

(Nn27) 2Θ3rd=(Θn27cn/Θn30cn)

(Nn28) 2Θ3rd=(Θn28cn/Θn31cn)

(Nn29) 2Θ3rd=(Θn29cn/Θn32cn)

(Nn30) 2Θ3rd=(Θn30cn/Θn33cn)

(Nn31) 2Θ3rd=(Θn31cn/Θn34cn)

(Nn32) 2Θ3rd=(Θn32cn/Θn35cn)

(Nn33) 2Θ3rd=(Θn33cn/Θn36cn)

(Nn34) 2Θ3rd=(Θn34cn/Θn37cn)

(Nn35) 2Θ3rd=(Θn35cn/Θn38cn)

(Nn36) 2Θ3rd=(Θn36cn/Θn39cn)

(Nn37) 2Θ3rd=(Θn37cn/Θn40cn)

(Nn38) 2Θ3rd=(Θn38cn/Θn41cn)

(Nn39) 2Θ3rd=(Θn39cn/Θn42cn)

(Nn40) 2Θ3rd=(Θn40cn/Θn43cn)

(Nn41) 2Θ3rd=(Θn40cn/Θn44cn)

(Nn42) 2Θ3rd=(Θn41cn/Θn45cn)


Then if

22nd=(n1/n3) then 2(1⅄Q)2nd=(1⅄Qn1cn/1⅄Qn3cn)

(Nn1) 2(1⅄Q)2nd=(1⅄Qn1cn/1⅄Qn3cn)

(Nn2) 2(1⅄Q)2nd=(1⅄Qn2cn/1⅄Qn4cn)

(Nn3) 2(1⅄Q)2nd=(1⅄Qn3cn/1⅄Qn5cn)

(Nn4) 2(1⅄Q)2nd=(1⅄Qn4cn/1⅄Qn6cn)

(Nn5) 2(1⅄Q)2nd=(1⅄Qn5cn/1⅄Qn7cn)

(Nn6) 2(1⅄Q)2nd=(1⅄Qn6cn/1⅄Qn8cn)

(Nn7) 2(1⅄Q)2nd=(1⅄Qn7cn/1⅄Qn9cn)

(Nn8) 2(1⅄Q)2nd=(1⅄Qn8cn/1⅄Qn10cn)

(Nn9) 2(1⅄Q)2nd=(1⅄Qn9cn/1⅄Qn11cn)

(Nn10) 2(1⅄Q)2nd=(1⅄Qn10cn/1⅄Qn12cn)

(Nn11) 2(1⅄Q)2nd=(1⅄Qn11cn/1⅄Qn13cn)

(Nn12) 2(1⅄Q)2nd=(1⅄Qn12cn/1⅄Qn14cn)

(Nn13) 2(1⅄Q)2nd=(1⅄Qn13cn/1⅄Qn15cn)

(Nn14) 2(1⅄Q)2nd=(1⅄Qn14cn/1⅄Qn16cn)

(Nn15) 2(1⅄Q)2nd=(1⅄Qn15cn/1⅄Qn17cn)

(Nn16) 2(1⅄Q)2nd=(1⅄Qn16cn/1⅄Qn18cn)

(Nn17) 2(1⅄Q)2nd=(1⅄Qn17cn/1⅄Qn19cn)

(Nn18) 2(1⅄Q)2nd=(1⅄Qn18cn/1⅄Qn20cn)

(Nn19) 2(1⅄Q)2nd=(1⅄Qn19cn/1⅄Qn21cn)

(Nn20) 2(1⅄Q)2nd=(1⅄Qn20cn/1⅄Qn22cn)

(Nn21) 2(1⅄Q)2nd=(1⅄Qn21cn/1⅄Qn23cn)

(Nn22) 2(1⅄Q)2nd=(1⅄Qn22cn/1⅄Qn24cn)

(Nn23) 2(1⅄Q)2nd=(1⅄Qn23cn/1⅄Qn25cn)

(Nn24) 2(1⅄Q)2nd=(1⅄Qn24cn/1⅄Qn26cn)

(Nn25) 2(1⅄Q)2nd=(1⅄Qn25cn/1⅄Qn27cn)

(Nn26) 2(1⅄Q)2nd=(1⅄Qn26cn/1⅄Qn28cn)

(Nn27) 2(1⅄Q)2nd=(1⅄Qn27cn/1⅄Qn29cn)

(Nn28) 2(1⅄Q)2nd=(1⅄Qn28cn/1⅄Qn30cn)

(Nn29) 2(1⅄Q)2nd=(1⅄Qn29cn/1⅄Qn31cn)

(Nn30) 2(1⅄Q)2nd=(1⅄Qn30cn/1⅄Qn32cn)

(Nn31) 2(1⅄Q)2nd=(1⅄Qn31cn/1⅄Qn33cn)

(Nn32) 2(1⅄Q)2nd=(1⅄Qn32cn/1⅄Qn34cn)

(Nn33) 2(1⅄Q)2nd=(1⅄Qn33cn/1⅄Qn35cn)

(Nn34) 2(1⅄Q)2nd=(1⅄Qn34cn/1⅄Qn36cn)

(Nn35) 2(1⅄Q)2nd=(1⅄Qn35cn/1⅄Qn37cn)

(Nn36) 2(1⅄Q)2nd=(1⅄Qn36cn/1⅄Qn38cn)

(Nn37) 2(1⅄Q)2nd=(1⅄Qn37cn/1⅄Qn39cn)

(Nn38) 2(1⅄Q)2nd=(1⅄Qn38cn/1⅄Qn40cn)

(Nn39) 2(1⅄Q)2nd=(1⅄Qn39cn/1⅄Qn41cn)

(Nn40) 2(1⅄Q)2nd=(1⅄Qn40cn/1⅄Qn42cn)

(Nn41) 2(1⅄Q)2nd=(1⅄Qn41cn/1⅄Qn43cn)

(Nn42) 2(1⅄Q)2nd=(1⅄Qn42cn/1⅄Qn44cn)

(Nn43) 2(1⅄Q)2nd=(1⅄Qn43cn/1⅄Qn45cn)

And if

23rd=(n1/n4) then 2(1⅄Q)3rd=(1⅄Qn1cn/1⅄Qn4cn)

(Nn1) 2(1⅄Q)3rd=(1⅄Qn1cn/1⅄Qn4cn)

(Nn2) 2(1⅄Q)3rd=(1⅄Qn2cn/1⅄Qn5cn)

(Nn3) 2(1⅄Q)3rd=(1⅄Qn3cn/1⅄Qn6cn)

(Nn4) 2(1⅄Q)3rd=(1⅄Qn4cn/1⅄Qn7cn)

(Nn5) 2(1⅄Q)3rd=(1⅄Qn5cn/1⅄Qn8cn)

(Nn6) 2(1⅄Q)3rd=(1⅄Qn6cn/1⅄Qn9cn)

(Nn7) 2(1⅄Q)3rd=(1⅄Qn7cn/1⅄Qn10cn)

(Nn8) 2(1⅄Q)3rd=(1⅄Qn8cn/1⅄Qn11cn)

(Nn9) 2(1⅄Q)3rd=(1⅄Qn9cn/1⅄Qn12cn)

(Nn10) 2(1⅄Q)3rd=(1⅄Qn10cn/1⅄Qn13cn)

(Nn11) 2(1⅄Q)3rd=(1⅄Qn11cn/1⅄Qn14cn)

(Nn12) 2(1⅄Q)3rd=(1⅄Qn12cn/1⅄Qn15cn)

(Nn13) 2(1⅄Q)3rd=(1⅄Qn13cn/1⅄Qn16cn)

(Nn14) 2(1⅄Q)3rd=(1⅄Qn14cn/1⅄Qn17cn)

(Nn15) 2(1⅄Q)3rd=(1⅄Qn15cn/1⅄Qn18cn)

(Nn16) 2(1⅄Q)3rd=(1⅄Qn16cn/1⅄Qn19cn)

(Nn17) 2(1⅄Q)3rd=(1⅄Qn17cn/1⅄Qn20cn)

(Nn18) 2(1⅄Q)3rd=(1⅄Qn18cn/1⅄Qn21cn)

(Nn19) 2(1⅄Q)3rd=(1⅄Qn19cn/1⅄Qn22cn)

(Nn20) 2(1⅄Q)3rd=(1⅄Qn20cn/1⅄Qn23cn)

(Nn21) 2(1⅄Q)3rd=(1⅄Qn21cn/1⅄Qn24cn)

(Nn22) 2(1⅄Q)3rd=(1⅄Qn22cn/1⅄Qn25cn)

(Nn23) 2(1⅄Q)3rd=(1⅄Qn23cn/1⅄Qn26cn)

(Nn24) 2(1⅄Q)3rd=(1⅄Qn24cn/1⅄Qn27cn)

(Nn25) 2(1⅄Q)3rd=(1⅄Qn25cn/1⅄Qn28cn)

(Nn26) 2(1⅄Q)3rd=(1⅄Qn26cn/1⅄Qn29cn)

(Nn27) 2(1⅄Q)3rd=(1⅄Qn27cn/1⅄Qn30cn)

(Nn28) 2(1⅄Q)3rd=(1⅄Qn28cn/1⅄Qn31cn)

(Nn29) 2(1⅄Q)3rd=(1⅄Qn29cn/1⅄Qn32cn)

(Nn30) 2(1⅄Q)3rd=(1⅄Qn30cn/1⅄Qn33cn)

(Nn31) 2(1⅄Q)3rd=(1⅄Qn31cn/1⅄Qn34cn)

(Nn32) 2(1⅄Q)3rd=(1⅄Qn32cn/1⅄Qn35cn)

(Nn33) 2(1⅄Q)3rd=(1⅄Qn33cn/1⅄Qn36cn)

(Nn34) 2(1⅄Q)3rd=(1⅄Qn34cn/1⅄Qn37cn)

(Nn35) 2(1⅄Q)3rd=(1⅄Qn35cn/1⅄Qn38cn)

(Nn36) 2(1⅄Q)3rd=(1⅄Qn36cn/1⅄Qn39cn)

(Nn37) 2(1⅄Q)3rd=(1⅄Qn37cn/1⅄Qn40cn)

(Nn38) 2(1⅄Q)3rd=(1⅄Qn38cn/1⅄Qn41cn)

(Nn39) 2(1⅄Q)3rd=(1⅄Qn39cn/1⅄Qn42cn)

(Nn40) 2(1⅄Q)3rd=(1⅄Qn40cn/1⅄Qn43cn)

(Nn41) 2(1⅄Q)3rd=(1⅄Qn41cn/1⅄Qn44cn)

(Nn42) 2(1⅄Q)3rd=(1⅄Qn42cn/1⅄Qn45cn)


Then if

22nd=(n1/n3) then 2(2⅄Q)2nd=(2⅄Qn1cn/2⅄Qn3cn)

(Nn1) 2(2⅄Q)2nd=(2⅄Qn1cn/2⅄Qn3cn)

(Nn2) 2(2⅄Q)2nd=(2⅄Qn2cn/2⅄Qn4cn)

(Nn3) 2(2⅄Q)2nd=(2⅄Qn3cn/2⅄Qn5cn)

(Nn4) 2(2⅄Q)2nd=(2⅄Qn4cn/2⅄Qn6cn)

(Nn5) 2(2⅄Q)2nd=(2⅄Qn5cn/2⅄Qn7cn)

(Nn6) 2(2⅄Q)2nd=(2⅄Qn6cn/2⅄Qn8cn)

(Nn7) 2(2⅄Q)2nd=(2⅄Qn7cn/2⅄Qn9cn)

(Nn8) 2(2⅄Q)2nd=(2⅄Qn8cn/2⅄Qn10cn)

(Nn9) 2(2⅄Q)2nd=(2⅄Qn9cn/2⅄Qn11cn)

(Nn10) 2(2⅄Q)2nd=(2⅄Qn10cn/2⅄Qn12cn)

(Nn11) 2(2⅄Q)2nd=(2⅄Qn11cn/2⅄Qn13cn)

(Nn12) 2(2⅄Q)2nd=(2⅄Qn12cn/2⅄Qn14cn)

(Nn13) 2(2⅄Q)2nd=(2⅄Qn13cn/2⅄Qn15cn)

(Nn14) 2(2⅄Q)2nd=(2⅄Qn14cn/2⅄Qn16cn)

(Nn15) 2(2⅄Q)2nd=(2⅄Qn15cn/2⅄Qn17cn)

(Nn16) 2(2⅄Q)2nd=(2⅄Qn16cn/2⅄Qn18cn)

(Nn17) 2(2⅄Q)2nd=(2⅄Qn17cn/2⅄Qn19cn)

(Nn18) 2(2⅄Q)2nd=(2⅄Qn18cn/2⅄Qn20cn)

(Nn19) 2(2⅄Q)2nd=(2⅄Qn19cn/2⅄Qn21cn)

(Nn20) 2(2⅄Q)2nd=(2⅄Qn20cn/2⅄Qn22cn)

(Nn21) 2(2⅄Q)2nd=(2⅄Qn21cn/2⅄Qn23cn)

(Nn22) 2(2⅄Q)2nd=(2⅄Qn22cn/2⅄Qn24cn)

(Nn23) 2(2⅄Q)2nd=(2⅄Qn23cn/2⅄Qn25cn)

(Nn24) 2(2⅄Q)2nd=(2⅄Qn24cn/2⅄Qn26cn)

(Nn25) 2(2⅄Q)2nd=(2⅄Qn25cn/2⅄Qn27cn)

(Nn26) 2(2⅄Q)2nd=(2⅄Qn26cn/2⅄Qn28cn)

(Nn27) 2(2⅄Q)2nd=(2⅄Qn27cn/2⅄Qn29cn)

(Nn28) 2(2⅄Q)2nd=(2⅄Qn28cn/2⅄Qn30cn)

(Nn29) 2(2⅄Q)2nd=(2⅄Qn29cn/2⅄Qn31cn)

(Nn30) 2(2⅄Q)2nd=(2⅄Qn30cn/2⅄Qn32cn)

(Nn31) 2(2⅄Q)2nd=(2⅄Qn31cn/2⅄Qn33cn)

(Nn32) 2(2⅄Q)2nd=(2⅄Qn32cn/2⅄Qn34cn)

(Nn33) 2(2⅄Q)2nd=(2⅄Qn33cn/2⅄Qn35cn)

(Nn34) 2(2⅄Q)2nd=(2⅄Qn34cn/2⅄Qn36cn)

(Nn35) 2(2⅄Q)2nd=(2⅄Qn35cn/2⅄Qn37cn)

(Nn36) 2(2⅄Q)2nd=(2⅄Qn36cn/2⅄Qn38cn)

(Nn37) 2(2⅄Q)2nd=(2⅄Qn37cn/2⅄Qn39cn)

(Nn38) 2(2⅄Q)2nd=(2⅄Qn38cn/2⅄Qn40cn)

(Nn39) 2(2⅄Q)2nd=(2⅄Qn39cn/2⅄Qn41cn)

(Nn40) 2(2⅄Q)2nd=(2⅄Qn40cn/2⅄Qn42cn)

(Nn41) 2(2⅄Q)2nd=(2⅄Qn41cn/2⅄Qn43cn)

(Nn42) 2(2⅄Q)2nd=(2⅄Qn42cn/2⅄Qn44cn)

(Nn43) 2(2⅄Q)2nd=(2⅄Qn43cn/2⅄Qn45cn)

And if

23rd=(n1/n4) then 2(2⅄Q)3rd=(2⅄Qn1cn/2⅄Qn4cn)

(Nn1) 2(2⅄Q)3rd=(2⅄Qn1cn/2⅄Qn4cn)

(Nn2) 2(2⅄Q)3rd=(2⅄Qn2cn/2⅄Qn5cn)

(Nn3) 2(2⅄Q)3rd=(2⅄Qn3cn/2⅄Qn6cn)

(Nn4) 2(2⅄Q)3rd=(2⅄Qn4cn/2⅄Qn7cn)

(Nn5) 2(2⅄Q)3rd=(2⅄Qn5cn/2⅄Qn8cn)

(Nn6) 2(2⅄Q)3rd=(2⅄Qn6cn/2⅄Qn9cn)

(Nn7) 2(2⅄Q)3rd=(2⅄Qn7cn/2⅄Qn10cn)

(Nn8) 2(2⅄Q)3rd=(2⅄Qn8cn/2⅄Qn11cn)

(Nn9) 2(2⅄Q)3rd=(2⅄Qn9cn/2⅄Qn12cn)

(Nn10) 2(2⅄Q)3rd=(2⅄Qn10cn/2⅄Qn13cn)

(Nn11) 2(2⅄Q)3rd=(2⅄Qn11cn/2⅄Qn14cn)

(Nn12) 2(2⅄Q)3rd=(2⅄Qn12cn/2⅄Qn15cn)

(Nn13) 2(2⅄Q)3rd=(2⅄Qn13cn/2⅄Qn16cn)

(Nn14) 2(2⅄Q)3rd=(2⅄Qn14cn/2⅄Qn17cn)

(Nn15) 2(2⅄Q)3rd=(2⅄Qn15cn/2⅄Qn18cn)

(Nn16) 2(2⅄Q)3rd=(2⅄Qn16cn/2⅄Qn19cn)

(Nn17) 2(2⅄Q)3rd=(2⅄Qn17cn/2⅄Qn20cn)

(Nn18) 2(2⅄Q)3rd=(2⅄Qn18cn/2⅄Qn21cn)

(Nn19) 2(2⅄Q)3rd=(2⅄Qn19cn/2⅄Qn22cn)

(Nn20) 2(2⅄Q)3rd=(2⅄Qn20cn/2⅄Qn23cn)

(Nn21) 2(2⅄Q)3rd=(2⅄Qn21cn/2⅄Qn241n)

(Nn22) 2(2⅄Q)3rd=(2⅄Qn22cn/2⅄Qn25cn)

(Nn23) 2(2⅄Q)3rd=(2⅄Qn23cn/2⅄Qn26cn)

(Nn24) 2(2⅄Q)3rd=(2⅄Qn24cn/2⅄Qn27cn)

(Nn25) 2(2⅄Q)3rd=(2⅄Qn25cn/2⅄Qn28cn)

(Nn26) 2(2⅄Q)3rd=(2⅄Qn26cn/2⅄Qn29cn)

(Nn27) 2(2⅄Q)3rd=(2⅄Qn27cn/2⅄Qn30cn)

(Nn28) 2(2⅄Q)3rd=(2⅄Qn28cn/2⅄Qn31cn)

(Nn29) 2(2⅄Q)3rd=(2⅄Qn29cn/2⅄Qn32cn)

(Nn30) 2(2⅄Q)3rd=(2⅄Qn30cn/2⅄Qn33cn)

(Nn31) 2(2⅄Q)3rd=(2⅄Qn31cn/2⅄Qn34cn)

(Nn32) 2(2⅄Q)3rd=(2⅄Qn32cn/2⅄Qn35cn)

(Nn33) 2(2⅄Q)3rd=(2⅄Qn33cn/2⅄Qn36cn)

(Nn34) 2(2⅄Q)3rd=(2⅄Qn34cn/2⅄Qn37cn)

(Nn35) 2(2⅄Q)3rd=(2⅄Qn35cn/2⅄Qn38cn)

(Nn36) 2(2⅄Q)3rd=(2⅄Qn36cn/2⅄Qn39cn)

(Nn37) 2(2⅄Q)3rd=(2⅄Qn37cn/2⅄Qn40cn)

(Nn38) 2(2⅄Q)3rd=(2⅄Qn38cn/2⅄Qn41cn)

(Nn39) 2(2⅄Q)3rd=(2⅄Qn39cn/2⅄Qn42cn)

(Nn40) 2(2⅄Q)3rd=(2⅄Qn40cn/2⅄Qn43cn)

(Nn41) 2(2⅄Q)3rd=(2⅄Qn41cn/2⅄Qn44cn)

(Nn42) 2(2⅄Q)3rd=(2⅄Qn42cn/2⅄Qn45cn)


Ψ represents unique whole numbers that are not prime numbers nor are they fibonacci numbers

4 6 9 10 12 14 15 16 18 20 22 24 25 26 27 28 30 32 33 35 36 38 39 40 42 44 45 46 48 49 50 51 52 54 56 57 58 60 62 63 64 65 66 68 69 70 72 74 75 76 77 78 80 81 82 84 85 86 87 88 90 91 92 93 94 95 96 98 99 100 and so on . . .

These whole numbers are variables that are neither Y base fibonacci numerals nor are they P prime numbers.


if 12nd=(n3/n1) of (Nn) then (Nn1)1Ψ2nd=(Ψn3/Ψn1)

if 13rd=(n4/n1) of (Nn) then (Nn1)1Ψ3rd=(Ψn4/Ψn1)

and

if 22nd=(n1/n3) of (Nn) then (Nn1)2Ψ2nd=(Ψn1/Ψn3)

if 23rd=(n1/n4) of (Nn) then (Nn1)2Ψ3rd=(Ψn1/Ψn4)


and so on for (Nn)nΨ4th, (Nn)nΨ5th, (Nn)nΨ6th, (Nn)nΨ7th, . . . . .(Nn)nΨnth,


Whole numbers of psi Ψ differ from ratios of psi paths 1Ψ and 2Ψ variables just as paths 1Q and 2Q differ from P prime numbers being quotients of prime numbers, and Y base numerals of phi φ and theta Θ ratios differ based on paths to those ratio values. 


So then an equation of for all for any applied to psi divided path ratios 1Ψ are

if 12nd=(n3/n1) of (Nn) then (Nn1)1∀(1Ψ2nd)=(1Ψn3/1Ψn1)

if 13rd=(n4/n1) of (Nn) then (Nn1)1∀(1Ψ3rd)=(1Ψn4/1Ψn1)

and

if 22nd=(n1/n3) of (Nn) then (Nn1)2∀(1Ψ2nd)=(1Ψn1/1Ψn3)

if 23rd=(n1/n4) of (Nn) then (Nn1)2∀(1Ψ3rd)=(1Ψn1/1Ψn4)


while an entirely different path set of equations of for all for any applied to psi divided path ratios 2Ψ are

if 12nd=(n3/n1) of (Nn) then (Nn1)1∀(2Ψ2nd)=(2Ψn3/2Ψn1)

if 13rd=(n4/n1) of (Nn) then (Nn1)1∀(2Ψ3rd)=(2Ψn4/2Ψn1)

and

if 22nd=(n1/n3) of (Nn) then (Nn1)2∀(2Ψ2nd)=(2Ψn1/2Ψn3)

if 23rd=(n1/n4) of (Nn) then (Nn1)2∀(2Ψ3rd)=(2Ψn1/2Ψn4)


and so on for (Nn)nnΨ4th, (Nn)nnΨ5th, (Nn)nnΨ6th, (Nn)nnΨ7th, . . . . .(Nn)nnΨnth,


More complex path set of equations of for all for any applied to psi divided path ratios are using variables of 2Ψ that are quotients of paths 1Ψ and 2Ψ variables such that n2Ψ=(Ψ/Ψ) and are quotients of ratios divided by ratios from a 3rd set of psi base numerals set ∈Ψ


Ψ∉n2Ψ

Psi variable whole numbers are not of the same set of variables of quotients derived from psi whole numbers and the quotients are defined by the exact numerals that produce variable quotients differing to the path of later to previous or previous to later while for all for any applied then alters those quotients and decimal ratio stem to a cn factor entirely unique to the definition of each. While some variables may equal one another, the paths that the quotients were derived are not equal.


Alternate path of Q bases division examples 3(11Qn1)/(21Qn1)cn

With variants of both pairs of Q base paths new tier sets and variables can be factored for example

if 21Qn1=(pn1/pn2)=(2/3)=0.^6 and 11Qn1=(pn2/pn1)=(3/2)=1.5

then (21Qn1)/(11Qn1)=(0.^6/1.5)=0.4 while (21Qn1c2)/(11Qn1)=(0.^66/1.5)=0.44

and

(11Qn1)/(21Qn1)=(1.5/0.^6)=2.5 while (11Qn1)/(21Qn1c2)=(1.5/0.^66)=2.^27

so

3(11Qn1)/(21Qn1) has base variants from only one change in cn of 21Qn1 applicable to functions with φ variables

with the definition that 11Qn1 and 21Qn1 are factors that 1(11Qn2)/(21Qn1) and 2(11Qn1)/(21Qn2) differ sets paths to tiers and variants dependent of cn each.

with this 

(21Qn1)/(11Qn1)=(0.^6/1.5)=0.4 

(21Qn1c2)/(11Qn1)=(0.^66/1.5)=0.44

and

(11Qn1)/(21Qn1)=(1.5/0.^6)=2.5

(11Qn1)/(21Qn1c2)=(1.5/0.^66)=2.^27


each have potential variable change dependent of the stem shell cycle cn of the example.

(11Qn1)/(21Qn1c2)=(1.5/0.^66)=2.^27 specifically of this example 

then are other variant sets determined with cn

Alternate path of Q bases division examples 1(11Qn2)/(21Qn1)

Alternate path of Q bases division examples 2(11Qn1)/(21Qn2)

and

Alternate path of Q bases division examples 1(21Qn2)/(11Qn1)

Alternate path of Q bases division examples 2(21Qn1)/(11Qn2)

with the examples assuming c1 for cn

Alternate path of φ and Q bases division examples

Examples of the variable set application with function to 1φn21=1.6^1803399852

(1φn21)/((21Qn1)/(11Qn1))=(1.6^1803399852/(0.^6/1.5)=(1.6^1803399852/0.4)=4.0450849963

(1φn21)/((21Qn1c2)/(11Qn1))=(1.6^1803399852/(0.^66/1.5))=(1.6^1803399852//0.44)=3.677349996^63

(1φn21)/((11Qn1)/(21Qn1))=(1.6^1803399852/(1.5/0.^6)=(1.6^1803399852/2.5)=0.647213599408

(1φn21)/((11Qn1)/(21Qn1c2))=(1.6^1803399852/(1.5/0.^66)=(1.6^1803399852/2.^27)=0.712790307^71806167400881057268722466960352422907488986784140969162995594713656387665198237885462555066079295154185022026431

and

(1φn21)/((11Qn1)/(21Qn1c2)c2)=(1.6^1803399852/(1.5/0.^66)c2)=(1.6^1803399852/2.^2727) for c2 of (11Qn1)/(21Qn1c2) and so on . . . for cn

An Alternate Path of 1φn21c2 for 1φn21c3 of the mentioned base example uses c21.6^18033998521803399852 c31.6^180339985218033998521803399852

meaning

(1φn21c2)/((21Qn1)/(11Qn1))=(1.6^18033998521803399852/(0.^6/1.5)=(1.6^1803399852/0.4)

(1φn21c2)/((21Qn1c2)/(11Qn1))=(1.6^18033998521803399852/(0.^66/1.5))=(1.6^1803399852//0.44)

(1φn21c2)/((11Qn1)/(21Qn1))=(1.6^18033998521803399852/(1.5/0.^6)=(1.6^1803399852/2.5)

(1φn21c2)/((11Qn1)/(21Qn1c2))=(1.6^18033998521803399852/(1.5/0.^66)=(1.6^1803399852/2.^27)

and

(1φn21c3)/((21Qn1)/(11Qn1))=(1.6^180339985218033998521803399852/(0.^6/1.5)=(1.6^1803399852/0.4)

(1φn21c3)/((21Qn1c2)/(11Qn1))=(1.6^180339985218033998521803399852/(0.^66/1.5))=(1.6^1803399852//0.44)

(1φn21c3)/((11Qn1)/(21Qn1))=(1.6^180339985218033998521803399852/(1.5/0.^6)=(1.6^1803399852/2.5)

(1φn21c3)/((11Qn1)/(21Qn1c2))=(1.6^180339985218033998521803399852/(1.5/0.^66)=(1.6^1803399852/2.^27)

while alternate sequences of these variables factor completely different and produce quotients very different.

Given the extent of numeral decimal a short version of the quotient example shell is displayed of the example

((21Qn1)/(11Qn1))/(1φn21)=(0.4/1.6^1803399852)=0.247213593991 extended shell (23242510668/161803399852)

((21Qn1c2)/(11Qn1))/(1φn21)=(0.44/1.6^1803399852)

((11Qn1)/(21Qn1)))/(1φn21)=(2.5/1.6^1803399852)

((11Qn1)/(21Qn1c2))/(1φn21)=(2.^27/1.6^1803399852)

and

((11Qn1)/(21Qn1c2)c2)/(1φn21)=(2.^2727/1.6^1803399852) for c2 of (11Qn1)/(21Qn1c2) and so on . . .

while other variants of (1φn21c2) formulate

(1φn21c2)/((21Qn1)/(11Qn1))=(1.6^18033998521803399852/0.4)

(1φn21c2)/((21Qn1c2)/(11Qn1))=(1.6^18033998521803399852/0.44)

(1φn21c2)/((11Qn1)/(21Qn1))=(1.6^18033998521803399852/2.5)

(1φn21c2)/((11Qn1)/(21Qn1c2))=(1.6^18033998521803399852/2.^27)

and

(1φn21c2)/((11Qn1)/(21Qn1c2)c2)=(1.6^18033998521803399852/2.^2727) and so on . . .

then with c2 applied to 1φn21 the variable a different set path of the stem cycle are functions of 1φn21c2 rather than 1φn21c1 functions

((21Qn1)/(11Qn1))/(1φn21c2)=(0.4/1.6^18033998521803399852)

((21Qn1c2)/(11Qn1))/(1φn21c2)=(0.44/1.6^18033998521803399852)

((11Qn1)/(21Qn1)))/(1φn21c2)=(2.5/1.6^18033998521803399852)

((11Qn1)/(21Qn1c2))/(1φn21c2)=(2.^27/1.6^18033998521803399852)

and

((11Qn1)/(21Qn1c2)c2)/(1φn21c2)=(2.^2727/1.6^18033998521803399852) and so on . . .

so 3(11Qn1)/(21Qn1) and 3(21Qn1)/(21Qn1) are not of the same set and have similar factors

then

3(11Qn1)/(21Qn1

3(21Qn1)/(21Qn1

2(21Qn1)/(11Qn2)

2(11Qn1)/(21Qn2)

1(21Qn2)/(11Qn1)

1(11Qn2)/(21Qn1)

each have variable potential change dependent of cn

Before moving forward to functions of 1⅄, 2⅄, 3⅄, of more complex equations and variable tier paths

(11Qncn)/(11φncn

or (11φncn)/(11Qncn

or (11Qncn)/(11φncn

or (11φncn)/(11Qncn) bases and roasting a computers data storage limit with decimal variables, a base of phi and prime and a base of prime phi can be factored for a completely different tier set bases as the equations mentioned will also differ from tier set bases of φ/y and y/φ as well as y/p and p/y base tier sets. These decimal variables have potential change in decimal cycle stem cell yet are numbers that can be factored to a base numeral that will equal what the definitions explain. Quantum Fractal Polarization for Field Application to closed systems and open systems.

Forward path of the phi and prime variables combined functions of same path, later divided by previous from the two number bases would be sets

1(11Qncn)/(11φncn)

1(11φncn)/(11Qncn)

1(11Qncn)/(11φncn)

1(11φncn)/(11Qncn)

and

2(11Qncn)/(11φncn)

2(11φncn)/(11Qncn)

2(11Qncn)/(11φncn)

2(11φncn)/(11Qncn)

and

3(11Qncn)/(11φncn)

3(11φncn)/(11Qncn)

3(11Qncn)/(11φncn)

3(11φncn)/(11Qncn)

After the base of these sets would be alternate pairings of a n2 and n1 of paths with tiers to its pairing progress

11φn2/1Qn1 and 11Qn2/1φn1

12φn2/2Qn1 and 12Qn2/2φn1 pairing and so on . . .

as well as pairing sets

12φn2/1Qn1 and 12Qn2/1φn1

as 

32φncn/2Qncn and 32Qncn/2φncn 

is a path of the second tier of two stem paths φ and Q of a third divide based from y and p variables.

Regardless of the symbols, these arc values are a core and numeral constant that do have a very extremely precise quanta and they can be expressed with symbols of many kinds.

Where / for division can be replaced with x for multiplication + for addition - for subtraction and n°′ for exponential square cube or other factoring can be applied to these numbers in study of these scale relations. 

For ⅄ a notation of split paths that is sometimes a given of a notation outside brackets as a subset 1(n2/n1), 2(n2/n1). . . just as two symbols next to one another express multiplication 1X⅄ where the expression would be assumed (1X)x(1⅄)in these notations the X is quite literal. The expression here of 1X⅄ is a multiplied path of 1⅄ or 2⅄ or 3⅄ of the tier and set path that is provided by variables of n(nncn) to each potential ⅄nncn


Path functions 1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc n, ⅄ncn with any variables for set definitions listed below


Functions then proceed for example with

1=(n2/n1)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

Function path 1=(nn2cn/nn1cn) is nn2cn later number in a set of consecutive variables divided by nn1cn previous number in a set of consecutive variables, such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant.

1ᐱ(An2/An1), ∈1ᐱ(An2/Bn1), ∈1ᐱ(An2/Dn1), ∈1ᐱ(An2/En1), ∈1ᐱ(An2/Fn1), ∈1ᐱ(An2/Gn1), ∈1ᐱ(An2/Hn1), ∈1ᐱ(An2/In1), ∈1ᐱ(An2/Jn1), ∈1ᐱ(An2/Kn1), ∈1ᐱ(An2/Ln1), ∈1ᐱ(An2/Mn1), ∈1ᐱ(An2/Nn1), ∈1ᐱ(An2/On1), ∈1ᐱ(An2/Pn1), ∈1ᐱ(An2/Qn1), ∈1ᐱ(An2/Rn1), ∈1ᐱ(An2Sn1), ∈1ᐱ(An2/Tn1), ∈1ᐱ(An2/Un1),  ∈1ᐱ(An2/Vn1), ∈1ᐱ(An2/Wn1), ∈1ᐱ(An2/Yn1), ∈1ᐱ(An2/Zn1), ∈1ᐱ(An2n1), ∈1ᐱ(An2n1), 2ᐱ(An2cn/n1cn), ∈1ᐱ(An2cn/n1cn), ∈1ᐱ(An2cn/∘⧊°n1cn), ∈1ᐱ(An2cn/∘∇°n1cn)

1ᐱ(Bn2/An1), 2ᐱ(Bn2/Bn1), ∈1ᐱ(Bn2/Dn1), ∈1ᐱ(Bn2/En1), ∈1ᐱ(Bn2/Fn1), ∈1ᐱ(Bn2/Gn1), ∈1ᐱ(Bn2/Hn1), ∈1ᐱ(Bn2/In1), ∈1ᐱ(Bn2/Jn1), ∈1ᐱ(Bn2/Kn1), ∈1ᐱ(Bn2/Ln1), ∈1ᐱ(Bn2/Mn1), ∈1ᐱ(Bn2/Nn1), ∈1ᐱ(Bn2/On1), ∈1ᐱ(Bn2/Pn1), ∈1ᐱ(Bn2/Qn1), ∈1ᐱ(Bn2/Rn1), ∈1ᐱ(Bn2/Sn1), ∈1ᐱ(Bn2/Tn1), ∈1ᐱ(Bn2/Un1), ∈1ᐱ(Bn2/Vn1), ∈1ᐱ(Bn2/Wn1), ∈1ᐱ(Bn2/Yn1), ∈1ᐱ(Bn2/Zn1), ∈1ᐱ(Bn2n1), ∈1ᐱ(Bn2n1),1ᐱ(Bn2cn/n1cn), ∈1ᐱ(Bn2cn/n1cn), ∈1ᐱ(Bn2cn/∘⧊°n1cn), ∈1ᐱ(Bn2cn/∘∇°n1cn)

1ᐱ(Dn2/An1), ∈1ᐱ(Dn2/Bn1), 1ᐱ(Dn2/Dn1), ∈1ᐱ(Dn2/En1), ∈1ᐱ(Dn2/Fn1), ∈1ᐱ(Dn2/Gn1), ∈1ᐱ(Dn2/Hn1), ∈1ᐱ(Dn2/In1), ∈1ᐱ(Dn2/Jn1), ∈1ᐱ(Dn2/Kn1), ∈1ᐱ(Dn2/Ln1), ∈1ᐱ(Dn2/Mn1), ∈1ᐱ(Dn2/Nn1), ∈1ᐱ(Dn2/On1), ∈1ᐱ(Dn2/Pn1), ∈1ᐱ(Dn2/Qn1), ∈1ᐱ(Dn2/Rn1), ∈1ᐱ(Dn2/Sn1), ∈1ᐱ(Dn2/Tn1), ∈1ᐱ(Dn2/Un1),  ∈1ᐱ(Dn2/Vn1), ∈1ᐱ(Dn2/Wn1), ∈1ᐱ(Dn2/Yn1), ∈1ᐱ(Dn2/Zn1), ∈1ᐱ(Dn2n1), ∈1ᐱ(Dn2n1), 1ᐱ(Dn2cn/n1cn), ∈1ᐱ(Dn2cn/n1cn), ∈1ᐱ(Dn2cn/∘⧊°n1cn), ∈1ᐱ(Dn2cn/∘∇°n1cn)

1ᐱ(En2/An1), ∈1ᐱ(En2/Bn1), ∈1ᐱ(En2/Dn1), 1ᐱ(En2/En1), ∈1ᐱ(En2/Fn1), ∈1ᐱ(En2/Gn1), ∈1ᐱ(En2/Hn1), ∈1ᐱ(En2/In1), ∈1ᐱ(En2/Jn1), ∈1ᐱ(En2/Kn1), ∈1ᐱ(En2/Ln1), ∈1ᐱ(En2/Mn1), ∈1ᐱ(En2/Nn1), ∈1ᐱ(En2/On1), ∈1ᐱ(En2/Pn1), ∈1ᐱ(En2/Qn1), ∈1ᐱ(En2/Rn1), ∈1ᐱ(En2/Sn1), ∈1ᐱ(En2/Tn1),∈1ᐱ(En2/Un1), ∈1ᐱ(En2/Vn1), ∈1ᐱ(En2/Wn1), ∈1ᐱ(En2/Yn1), ∈1ᐱ(En2/Zn1), ∈1ᐱ(En2n1), ∈1ᐱ(En2n1),1ᐱ(En2cn/n1cn), ∈1ᐱ(En2cn/n1cn), ∈1ᐱ(En2cn/∘⧊°n1cn), ∈1ᐱ(En2cn/∘∇°n1cn)

1ᐱ(Fn2/An1), ∈1ᐱ(Fn2/Bn1), ∈1ᐱ(Fn2/Dn1), ∈1ᐱ(Fn2/En1), 1ᐱ(Fn2/Fn1), ∈1ᐱ(Fn2/Gn1), ∈1ᐱ(Fn2/Hn1), ∈1ᐱ(Fn2/In1), ∈1ᐱ(Fn2/Jn1), ∈1ᐱ(Fn2/Kn1), ∈1ᐱ(Fn2/Ln1), ∈1ᐱ(Fn2/Mn1), ∈1ᐱ(Fn2/Nn1), ∈1ᐱ(Fn2/On1), ∈1ᐱ(Fn2/Pn1), ∈1ᐱ(Fn2/Qn1), ∈1ᐱ(Fn2/Rn1), ∈1ᐱ(Fn2/Sn1), ∈1ᐱ(Fn2/Tn1),∈1ᐱ(Fn2/Un1),  ∈1ᐱ(Fn2/Vn1), ∈1ᐱ(Fn2/Wn1), ∈1ᐱ(Fn2/Yn1), ∈1ᐱ(Fn2/Zn1), ∈1ᐱ(Fn2n1), ∈1ᐱ(Fn2n1),1ᐱ(Fn2cn/n1cn), ∈1ᐱ(Fn2cn/n1cn), ∈1ᐱ(Fn2cn/∘⧊°n1cn), ∈1ᐱ(Fn2cn/∘∇°n1cn)

1ᐱ(Gn2/An1), ∈1ᐱ(Gn2/Bn1), ∈1ᐱ(Gn2/Dn1), ∈1ᐱ(Gn2/En1), ∈1ᐱ(Gn2/Fn1), 1ᐱ(Gn2/Gn1), ∈1ᐱ(Gn2/Hn1), ∈1ᐱ(Gn2/In1), ∈1ᐱ(Gn2/Jn1), ∈1ᐱ(Gn2/Kn1), ∈1ᐱ(Gn2/Ln1), ∈1ᐱ(Gn2/Mn1), ∈1ᐱ(Gn2/Nn1), ∈1ᐱ(Gn2/On1), ∈1ᐱ(Gn2/Pn1), ∈1ᐱ(Gn2/Qn1), ∈1ᐱ(Gn2/Rn1), ∈1ᐱ(Gn2/Sn1), ∈1ᐱ(Gn2/Tn1),∈1ᐱ(Gn2/Un1),  ∈1ᐱ(Gn2Vn1), ∈1ᐱ(Gn2/Wn1), ∈1ᐱ(Gn2/Yn1), ∈1ᐱ(Gn2/Zn1), ∈1ᐱ(Gn2n1), ∈1ᐱ(Gn2n1),1ᐱ(Gn2cn/n1cn), ∈1ᐱ(Gn2cn/n1cn), ∈1ᐱ(Gn2cn/∘⧊°n1cn), ∈1ᐱ(Gn2cn/∘∇°n1cn)

1ᐱ(Hn2/An1), ∈1ᐱ(Hn2/Bn1), ∈1ᐱ(Hn2/Dn1), ∈1ᐱ(Hn2/En1), ∈1ᐱ(Hn2/Fn1), ∈1ᐱ(Hn2/Gn1), 1ᐱ(Hn2/Hn1), ∈1ᐱ(Hn2/In1), ∈1ᐱ(Hn2/Jn1), ∈1ᐱ(Hn2/Kn1), ∈1ᐱ(Hn2/Ln1), ∈1ᐱ(Hn2/Mn1), ∈1ᐱ(Hn2/Nn1), ∈1ᐱ(Hn2/On1), ∈1ᐱ(Hn2/Pn1), ∈1ᐱ(Hn2/Qn1), ∈1ᐱ(Hn2/Rn1), ∈1ᐱ(Hn2/Sn1), ∈1ᐱ(Hn2/Tn1), ∈1ᐱ(Hn2/Un1),  ∈1ᐱ(Hn2/Vn1), ∈1ᐱ(Hn2/Wn1), ∈1ᐱ(Hn2/Yn1), ∈1ᐱ(Hn2/Zn1), ∈1/⅄ᐱ(Hn2n1), ∈1ᐱ(Hn2n1),1ᐱ(Hn2cn/n1cn), ∈1⅄Xᐱ(Hn2cn/n1cn), ∈1ᐱ(Hn2cn/∘⧊°n1cn), ∈1ᐱ(Hn2cn/∘∇°n1cn)

1ᐱ(In2/An1), ∈1ᐱ(In2/Bn1), ∈1ᐱ(In2/Dn1), ∈1ᐱ(In2/En1), ∈1ᐱ(In2/Fn1), ∈1ᐱ(In2-/Gn1), ∈1ᐱ(In2/Hn1), 1ᐱ(In2/In1), ∈1ᐱ(In2/Jn1), ∈1ᐱ(In2/Kn1), ∈1ᐱ(In2/Ln1), ∈1ᐱ(In2/Mn1), ∈1ᐱ(In2/Nn1), ∈1ᐱ(In2/On1), ∈1ᐱ(In2/Pn1), ∈1ᐱ(In2/Qn1), ∈1ᐱ(In2/Rn1), ∈1ᐱ(In2/Sn1), ∈1ᐱ(In2/Tn1),∈1ᐱ(In2/Un1),  ∈1ᐱ(In2/Vn1), ∈1ᐱ(In2/Wn1), ∈1ᐱ(In2/Yn1), ∈1ᐱ(In2/Zn1), ∈1ᐱ(In2n1), ∈1ᐱ(In2n1),1ᐱ(In2cn/n1cn), ∈1ᐱ(In2cn/n1cn), ∈1ᐱ(In2cn/∘⧊°n1cn), ∈1ᐱ(In2cn/∘∇°n1cn)

1ᐱ(Jn2/An1), ∈1ᐱ(Jn2/Bn1), ∈1ᐱ(Jn2/Dn1), ∈1ᐱ(Jn2/En1), ∈1ᐱ(Jn2/Fn1), ∈1ᐱ(Jn2/Gn1), ∈1ᐱ(Jn2/Hn1), ∈1ᐱ(Jn2/In1), 1ᐱ(Jn2/Jn1), ∈1ᐱ(Jn2/Kn1), ∈1ᐱ(Jn2/Ln1), ∈1ᐱ(Jn2/Mn1), ∈1ᐱ(Jn2/Nn1), ∈1ᐱ(Jn2/On1), ∈1ᐱ(Jn2/Pn1), ∈1ᐱ(Jn2/Qn1), ∈1ᐱ(Jn2/Rn1), ∈1/⅄ᐱ(Jn2/Sn1), ∈1ᐱ(Jn2/Tn1),∈1ᐱ(Jn2/Un1),  ∈1ᐱ(Jn2/Vn1), ∈1ᐱ(Jn2/Wn1), ∈1ᐱ(Jn2/Yn1), ∈1ᐱ(Jn2/Zn1), ∈1ᐱ(Jn2n1), ∈1ᐱ(Jn2n1),1ᐱ(Jn2cn/n1cn), ∈1ᐱ(Jn2cn/n1cn), ∈1ᐱ(Jn2cn/∘⧊°n1cn), ∈1ᐱ(Jn2cn/∘∇°n1cn)

1ᐱ(Kn2/An1), ∈1ᐱ(Kn2/Bn1), ∈1ᐱ(Kn2/Dn1), ∈1ᐱ(Kn2/En1), ∈1ᐱ(Kn2/Fn1), ∈1ᐱ(Kn2/Gn1), ∈1ᐱ(Kn2/Hn1), ∈1ᐱ(Kn2/In1), ∈1ᐱ(Kn2/Jn1), 1ᐱ(Kn2/Kn1), ∈1ᐱ(Kn2/Ln1), ∈1ᐱ(Kn2/Mn1), ∈1ᐱ(Kn2/Nn1), ∈1ᐱ(Kn2/On1), ∈1ᐱ(Kn2/Pn1), ∈1ᐱ(Kn2/Qn1), ∈1ᐱ(Kn2/Rn1), ∈1ᐱ(Kn2/Sn1), ∈1ᐱ(Kn2/Tn1),∈1ᐱ(Kn2/Un1), ∈1ᐱ(Kn2/Vn1), ∈1ᐱ(Kn2/Wn1), ∈1ᐱ(Kn2/Yn1), ∈1ᐱ(Kn2/Zn1), ∈1ᐱ(Kn2n1), ∈1ᐱ(Kn2n1),1ᐱ(Kn2cn/n1cn), ∈1ᐱ(Kn2cn/n1cn), ∈1ᐱ(Kn2cn/∘⧊°n1cn), ∈1ᐱ(Kn2cn/∘∇°n1cn)

1ᐱ(Ln2/An1), ∈1ᐱ(Ln2/Bn1), ∈1ᐱ(Ln2/Dn1), ∈1ᐱ(Ln2/En1), ∈1ᐱ(Ln2/Fn1), ∈1ᐱ(Ln2/Gn1), ∈1ᐱ(Ln2/Hn1), ∈1ᐱ(Ln2/In1), ∈1ᐱ(Ln2/Jn1), ∈1ᐱ(Ln2/Kn1), 1ᐱ(Ln2/Ln1), ∈1ᐱ(Ln2/Mn1), ∈1ᐱ(Ln2/Nn1), ∈1ᐱ(Ln2/On1), ∈1ᐱ(Ln2/Pn1), ∈1ᐱ(Ln2/Qn1), ∈1ᐱ(Ln2/Rn1), ∈1ᐱ(Ln2/Sn1), ∈1ᐱ(Ln2/Tn1),∈1ᐱ(Ln2/Un1),  ∈1ᐱ(Ln2/Vn1), ∈1ᐱ(Ln2/Wn1), ∈1ᐱ(Ln2/Yn1), ∈1ᐱ(Ln1/Zn1), ∈1ᐱ(Ln2n1), ∈1ᐱ(Ln2n1)),1ᐱ(Ln2cn/n1cn), ∈1ᐱ(Ln2cn/n1cn), ∈1ᐱ(Ln2cn/∘⧊°n1cn), ∈1ᐱ(Ln2cn/∘∇°n1cn)

1ᐱ(Mn2/An1), ∈1ᐱ(Mn2/Bn1), ∈1ᐱ(Mn2/Dn1), ∈1ᐱ(Mn2/En1), ∈1ᐱ(Mn2/Fn1), ∈1ᐱ(Mn2/Gn1), ∈1ᐱ(Mn2/Hn1), ∈1ᐱ(Mn2/In1), ∈1ᐱ(Mn2/Jn1), ∈1ᐱ(Mn2/Kn1), ∈1ᐱ(Mn2/Ln1), 1ᐱ(Mn2/Mn1), ∈1ᐱ(Mn2/Nn1), ∈1ᐱ(Mn2/On1), ∈1ᐱ(Mn2/Pn1), ∈1ᐱ(Mn2/Qn1), ∈1ᐱ(Mn2/Rn1), ∈1ᐱ(Mn2/Sn1), ∈1ᐱ(Mn2/Tn1),∈1ᐱ(Mn2/Un1),  ∈1ᐱ(Mn2/Vn1), ∈1ᐱ(Mn2/Wn1), ∈1ᐱ(Mn2/Yn1), ∈1ᐱ(Mn2/Zn1), ∈1ᐱ(Mn2n1), ∈1ᐱ(Mn2n1),1ᐱ(Mn2cn/n1cn), ∈1ᐱ(Mn2cn/n1cn), ∈1ᐱ(Mn2cn/∘⧊°n1cn), ∈1ᐱ(Mn2cn/∘∇°n1cn)

1ᐱ(Nn2/An1), ∈1ᐱ(Nn2/Bn1), ∈1ᐱ(Nn2/Dn1), ∈1ᐱ(Nn2/En1), ∈1ᐱ(Nn2/Fn1), ∈1ᐱ(Nn2/Gn1), ∈1ᐱ(Nn2/Hn1), ∈1ᐱ(Nn2/In1), ∈1ᐱ(Nn2/Jn1), ∈1ᐱ(Nn2/Kn1), ∈1ᐱ(Nn2/Ln1), ∈1ᐱ(Nn2/Mn1), 1ᐱ(Nn2/Nn1), ∈1ᐱ(Nn2/On1), ∈1ᐱ(Nn2/Pn1), ∈1ᐱ(Nn2/Qn1), ∈1ᐱ(Nn2/Rn1), ∈1ᐱ(Nn2/Sn1), ∈1ᐱ(Nn2/Tn1),∈1ᐱ(Nn2/Un1),  ∈1ᐱ(Nn2/Vn1), ∈1ᐱ(Nn2/Wn1), ∈1ᐱ(Nn2/Yn1), ∈1ᐱ(Nn2/Zn1), ∈1ᐱ(Nn2n1), ∈1ᐱ(Nn2n1),1ᐱ(Nn2cn/n1cn), ∈1ᐱ(Nn2cn/n1cn), ∈1-ᐱ(Nn2cn/∘⧊°n1cn), ∈1ᐱ(Nn2cn/∘∇°n1cn)

1ᐱ(On2/An1), ∈1ᐱ(On2/Bn1), ∈1ᐱ(On2/Dn1), ∈1ᐱ(On2/En1), ∈1ᐱ(On2/Fn1), ∈1ᐱ(On2/Gn1), ∈1ᐱ(On2/Hn1), ∈1ᐱ(On2/In1), ∈1ᐱ(On2/Jn1), ∈1ᐱ(On2/Kn1), ∈1ᐱ(On2/Ln1), ∈1ᐱ(On2/Mn1), ∈1ᐱ(On2/Nn1), 1ᐱ(On2/On1), ∈1ᐱ(On2/Pn1), ∈1ᐱ(On2/Qn1), ∈1ᐱ(On2/Rn1), ∈1ᐱ(On2/Sn1), ∈1ᐱ(On2/Tn1),∈1ᐱ(On2/Un1),  ∈1ᐱ(On2/Vn1), ∈1ᐱ(On2/Wn1), ∈1ᐱ(On2/Yn1), ∈1ᐱ(On2/Zn1), ∈1ᐱ(On2n1), ∈1ᐱ(On2n1),1ᐱ(On2cn/n1cn), ∈1ᐱ(On2cn/n1cn), ∈1ᐱ(On2cn/∘⧊°n1cn), ∈1ᐱ(On2cn/∘∇°n1cn)

1ᐱ(Pn2/An1), ∈1ᐱ(Pn2/Bn1), ∈1ᐱ(Pn2/Dn1), ∈1ᐱ(Pn2/En1), ∈1ᐱ(Pn2/Fn1), ∈1ᐱ(Pn2/Gn1), ∈1ᐱ(Pn2/Hn1), ∈1ᐱ(Pn2/In1), ∈1ᐱ(Pn2/Jn1), ∈1ᐱ(Pn2/Kn1), ∈1ᐱ(Pn2/Ln1), ∈1ᐱ(Pn2/Mn1), ∈1ᐱ(Pn2/Nn1), ∈1ᐱ(Pn2/On1), 1ᐱ(Pn2/Pn1), ∈1ᐱ(Pn2/Qn1), ∈1ᐱ(Pn2/Rn1), ∈1ᐱ(Pn2/Sn1), ∈1ᐱ(Pn2/Tn1),∈1ᐱ(Pn2/Un1),  ∈1ᐱ(Pn2/Vn1), ∈1ᐱ(Pn2/Wn1), ∈1ᐱ(Pn2/Yn1), ∈1ᐱ(Pn2/Zn1), ∈1ᐱ(Pn2n1), ∈1ᐱ(Pn2n1),1ᐱ(Pn2cn/n1cn), ∈1ᐱ(Pn2cn/n1cn), ∈1ᐱ(Pn2cn/∘⧊°n1cn), ∈1ᐱ(Pn2cn/∘∇°n1cn)

1ᐱ(Qn2/An1), ∈1ᐱ(Qn2/Bn1), ∈1ᐱ(Qn2/Dn1), ∈1ᐱ(Qn2/En1), ∈1ᐱ(Qn2/Fn1), ∈1ᐱ(Qn2/Gn1), ∈1ᐱ(Qn2/Hn1), ∈1ᐱ(Qn2/In1), ∈1ᐱ(Qn2/Jn1), ∈1ᐱ(Qn2/Kn1), ∈1ᐱ(Qn2/Ln1), ∈1ᐱ(Qn2/Mn1), ∈1ᐱ(Qn2/Nn1), ∈1ᐱ(Qn2/On1), ∈1ᐱ(Qn2/Pn1), 1ᐱ(Qn2/Qn1), ∈1ᐱ(Qn2/Rn1), ∈1ᐱ(Qn2/Sn1), ∈1ᐱ(Qn2/Tn1), ∈1ᐱ(Qn2/Un1),  ∈1ᐱ(Qn2/Vn1), ∈1ᐱ(Qn2/Wn1), ∈1ᐱ(Qn2/Yn1), ∈1ᐱ(Qn2/Zn1), ∈1ᐱ(Qn2n1), ∈1ᐱ(Qn2n1),1ᐱ(Qn2cn/n1cn), ∈1ᐱ(Qn2cn/n1cn), ∈1ᐱ(Qn1cn/∘⧊°n1cn), ∈1ᐱ(Qn2cn/∘∇°n1cn)

1ᐱ(Rn2/An1), ∈1ᐱ(Rn2/Bn1), ∈1ᐱ(Rn2/Dn1), ∈1ᐱ(Rn2/En1), ∈1ᐱ(Rn2/Fn1), ∈1ᐱ(Rn2/Gn1), ∈1ᐱ(Rn2/Hn1), ∈1ᐱ(Rn2/In1), ∈1ᐱ(Rn2/Jn1), ∈1ᐱ(Rn2/Kn1), ∈1ᐱ(Rn2/Ln1), ∈1ᐱ(Rn2/Mn1), ∈1ᐱ(Rn2/Nn1), ∈1ᐱ(Rn2/On1), ∈1ᐱ(Rn2/Pn1), ∈1ᐱ(Rn2/Qn1), 1ᐱ(Rn2/Rn1), ∈1ᐱ(Rn2/Sn1), ∈1ᐱ(Rn2/Tn1),∈1ᐱ(Rn2/Un1),  ∈1ᐱ(Rn2/Vn1), ∈1ᐱ(Rn2/Wn1), ∈1ᐱ(Rn2/Yn1), ∈1ᐱ(Rn2/Zn1), ∈1ᐱ(Rn2n1), ∈1ᐱ(Rn2n1),1ᐱ(Rn2cn/n1cn), ∈1ᐱ(Rn2cn/n1cn), ∈1ᐱ(Rn2cn/∘⧊°n1cn), ∈1ᐱ(Rn2cn/∘∇°n1cn)

1ᐱ(Sn2/An1), ∈1ᐱ(Sn2/Bn1), ∈1ᐱ(Sn2/Dn1), ∈1ᐱ(Sn2/En1), ∈1ᐱ(Sn2/Fn1), ∈1ᐱ(Sn2/Gn1), ∈1ᐱ(Sn2/Hn1), ∈1ᐱ(Sn2/In1), ∈1ᐱ(Sn2/Jn1), ∈1ᐱ(Sn2/Kn1), ∈1ᐱ(Sn2/Ln1), ∈1ᐱ(Sn2/Mn1), ∈1ᐱ(Sn2/Nn1), ∈1ᐱ(Sn2/On1), ∈1ᐱ(Sn2/Pn1), ∈1ᐱ(Sn2/Qn1), ∈1ᐱ(Sn2/Rn1), 1ᐱ(Sn2/Sn1), ∈1ᐱ(Sn2/Tn1),∈1ᐱ(Sn2/Un1),  ∈1ᐱ(Sn2/Vn1), ∈1ᐱ(Sn2/Wn1), ∈1ᐱ(Sn2/Yn1), ∈1ᐱ(Sn2/Zn1), ∈1ᐱ(Sn2n1), ∈1ᐱ(Sn2n1),1ᐱ(Sn2cn/n1cn), ∈1ᐱ(Sn2cn/n1cn), ∈1ᐱ(Sn2cn/∘⧊°n1cn), ∈1ᐱ(Sn2cn/∘∇°n1cn)

1ᐱ(Tn2/An1), ∈1ᐱ(Tn2/Bn1), ∈1ᐱ(Tn2/Dn1), ∈1ᐱ(Tn2/En1), ∈1ᐱ(Tn2/Fn1), ∈1ᐱ(Tn2/Gn1), ∈1ᐱ(Tn2/Hn1), ∈1ᐱ(Tn2/In1), ∈1ᐱ(Tn2/Jn1), ∈1ᐱ(Tn2/Kn1), ∈1ᐱ(Tn2/Ln1), ∈1ᐱ(Tn2/Mn1), ∈1ᐱ(Tn2/Nn1), ∈1ᐱ(Tn2/On1), ∈1ᐱ(Tn2/Pn1), ∈1ᐱ(Tn2/Qn1), ∈1ᐱ(Tn2/Rn1), ∈1ᐱ(Tn2/Sn1), 1ᐱ(Tn2/Tn1),∈1ᐱ(Tn2/Un1),  ∈1ᐱ(Tn2/Vn1), ∈1ᐱ(Tn2/Wn1), ∈1ᐱ(Tn2/Yn1), ∈1ᐱ(Tn2/Zn1), ∈1ᐱ(Tn2n1), ∈1ᐱ(Tn2n1),1ᐱ(Tn2cn/n1cn), ∈1ᐱ(Tn2cn/n1cn), ∈1ᐱ(Tn2cn/∘⧊°n1cn), ∈1ᐱ(Tn2cn/∘∇°n1cn)

1ᐱ(Un2/An1), ∈1ᐱ(Un2/Bn1), ∈1ᐱ(Un2/Dn1), ∈1ᐱ(Un2/En1), ∈1ᐱ(Un2/Fn1), ∈1ᐱ(Un2/Gn1), ∈1ᐱ(Un1/Hn1), ∈1ᐱ(Un1/In1), ∈1ᐱ(Un2/Jn1), ∈1ᐱ(Un2/Kn1), ∈1ᐱ(Un2/Ln1), ∈1ᐱ(Un2/Mn1), ∈1ᐱ(Un2/Nn1), ∈1ᐱ(Un2/On1), ∈1ᐱ(Un1/Pn1), ∈1ᐱ(Un2/Qn1), ∈n1ᐱ(Un2/Rn1), ∈1ᐱ(Un2/Sn1), ∈1ᐱ(Un2/Tn1), 1ᐱ(Un2/Un1),  ∈1ᐱ(Un2/Vn1), ∈1ᐱ(Un2/Wn1), ∈1ᐱ(Un2/Yn1), ∈1ᐱ(Un2/Zn1), ∈1ᐱ(Un2n1), ∈1ᐱ(Un2n1),1ᐱ(Un2cn/n1cn), ∈1ᐱ(Un2cn/n1cn), ∈1ᐱ(Un2cn/∘⧊°n1cn), ∈1ᐱ(Un2cn/∘∇°n1cn)

1ᐱ(Vn2/An1), ∈1ᐱ(Vn2/Bn1), ∈1ᐱ(Vn2/Dn1), ∈1ᐱ(Vn2/En1), ∈1ᐱ(Vn2/Fn1), ∈1ᐱ(Vn2/Gn1), ∈1ᐱ(Vn2/Hn1), ∈1ᐱ(Vn2/In1), ∈1ᐱ(Vn2/Jn1), ∈1ᐱ(Vn2/Kn1), ∈1ᐱ(Vn2/Ln1), ∈1ᐱ(Vn2/Mn1), ∈1ᐱ(Vn2/Nn1), ∈1ᐱ(Vn2/On1), ∈1ᐱ(Vn2/Pn1), ∈1ᐱ(Vn2/Qn1), ∈1ᐱ(Vn2/Rn1), ∈1ᐱ(Vn2/Sn1), ∈1ᐱ(Vn2/Tn1),∈1ᐱ(Vn2/Un1),  1ᐱ(Vn2/Vn1), ∈1ᐱ(Vn2/Wn1), ∈1ᐱ(Vn2/Yn1), ∈1ᐱ(Vn2/Zn1), ∈1ᐱ(Vn2n1), ∈1ᐱ(Vn2n1),1ᐱ(Vn2cn/n1cn), ∈1ᐱ(Vn2cn/n1cn), ∈1ᐱ(Vn2cn/∘⧊°n1cn), ∈1ᐱ(Vn2cn/∘∇°n1cn)

1ᐱ(Wn2/An1), ∈1ᐱ(Wn2/Bn1), ∈1ᐱ(Wn2/Dn1), ∈1ᐱ(Wn2/En1), ∈1ᐱ(Wn2/Fn1), ∈1ᐱ(Wn2/Gn1), ∈1ᐱ(Wn2/Hn1), ∈1ᐱ(Wn2/In1), ∈1ᐱ(Wn2/Jn1), ∈1ᐱ(Wn2/Kn1), ∈1ᐱ(Wn2/Ln1), ∈1ᐱ(Wn2/Mn1), ∈1ᐱ(Wn2/Nn1), ∈1ᐱ(Wn2/On1), ∈1ᐱ(Wn2/Pn1), ∈1ᐱ(Wn2/Qn1), ∈1ᐱ(Wn2/Rn1), ∈1ᐱ(Wn2/Sn1), ∈1ᐱ(Wn2/Tn1),∈1ᐱ(Wn2/Un1),  ∈1ᐱ(Wn2/Vn1), 1ᐱ(Wn2/Wn1), ∈1ᐱ(Wn2/Yn1), ∈1ᐱ(Wn2/Zn1), ∈1ᐱ(Wn2n1), ∈1ᐱ(Wn2n1),1ᐱ(Wn2cn/n1cn), ∈1ᐱ(Wn2cn/n1cn), ∈1ᐱ(Wn2cn/∘⧊°n1cn), ∈1ᐱ(Wn2cn/∘∇°n1cn)

1ᐱ(Yn2/An1), ∈1ᐱ(Yn2/Bn1), ∈1ᐱ(Yn2/Dn1), ∈1ᐱ(Yn2/En1), ∈1ᐱ(Yn2/Fn1), ∈1ᐱ(Yn2/Gn1), ∈1ᐱ(Yn2/Hn1), ∈1ᐱ(Yn2/In1), ∈1ᐱ(Yn2/Jn1), ∈1ᐱ(Yn2/Kn1), ∈1ᐱ(Yn2/Ln1), ∈1ᐱ(Yn2/Mn1), ∈1ᐱ(Yn2/Nn1), ∈1ᐱ(Yn2/On1), ∈1ᐱ(Yn2/Pn1), ∈1ᐱ(Yn2/Qn1), ∈1ᐱ(Yn2/Rn1), ∈1ᐱ(Yn2/Sn1), ∈1ᐱ(Yn2/Tn1),∈1ᐱ(Yn2/Un1),  ∈1ᐱ(Yn2/Vn1), ∈1ᐱ(Yn2Wn1), 1ᐱ(Yn2/Yn1), ∈1ᐱ(Yn2/Zn1), ∈1ᐱ(Yn2n1), ∈1ᐱ(Yn2n1),1ᐱ(Yn2cn/n1cn), ∈1ᐱ(Yn2cn/n1cn), ∈1ᐱ(Yn2cn/∘⧊°n1cn), ∈1ᐱ(Yn2cn/∘∇°n1cn)

1ᐱ(Zn2/An1), ∈1ᐱ(Zn2/Bn1), ∈1ᐱ(Zn2/Dn1), ∈1ᐱ(Zn2/En1), ∈1ᐱ(Zn2/Fn1), ∈1ᐱ(Zn2/Gn1), ∈1ᐱ(Zn2/Hn1), ∈1ᐱ(Zn2/In1), ∈1ᐱ(Zn2/Jn1), ∈1ᐱ(Zn2/Kn1), ∈1ᐱ(Zn2/Ln1), ∈1ᐱ(Zn2/Mn1), ∈1ᐱ(Zn2/Nn1), ∈1ᐱ(Zn2/On1), ∈1ᐱ(Zn2/Pn1), ∈1ᐱ(Zn2/Qn1), ∈1ᐱ(Zn2/Rn1), ∈1ᐱ(Zn2/Sn1), ∈1ᐱ(Zn2/Tn1),∈1ᐱ(Zn2/Un1),  ∈1ᐱ(Zn2/Vn1), ∈1ᐱ(Zn2/Wn1), ∈1ᐱ(Zn2/Yn1), 1ᐱ(Zn2/Zn1), ∈1ᐱ(Zn2n1), ∈1ᐱ(Zn2n1),1ᐱ(Zn2cn/n1cn), ∈1ᐱ(Zn2cn/n1cn), ∈1ᐱ(Zn2cn/∘⧊°n1cn), ∈1ᐱ(Zn2cn/∘∇°n1cn)

1ᐱ(φn2/An1), ∈1ᐱ(φn2/Bn1), ∈1ᐱ(φn2/Dn1), ∈1ᐱ(φn2/En1), ∈1ᐱ(φn2/Fn1), ∈1ᐱ(φn2/Gn1), ∈1ᐱ(φn2/Hn1), ∈1ᐱ(φn2/In1), ∈1ᐱ(φn2/Jn1), ∈1ᐱ(φn2/Kn1), ∈1ᐱ(φn2/Ln1), ∈1ᐱ(φn2/Mn1), ∈1ᐱ(φn2/Nn1), ∈1ᐱ(φn2/On1), ∈1ᐱ(φn2/Pn1), ∈1ᐱ(φn2/Qn1), ∈1ᐱ(φn2/Rn1), ∈1ᐱ(φn2/Sn1), ∈1ᐱ(φn2/Tn1),∈1ᐱ(φn2/Un1),  ∈1ᐱ(φn2/Vn1), ∈1ᐱ(φn2/Wn1), ∈1ᐱ(φn2/Yn1), ∈1ᐱ(φn2/Zn1), 1ᐱ(φn2/φn1), ∈1ᐱ(φn2n1),1ᐱ(φn2cn/n1cn), ∈1ᐱ(φn2cn/n1cn), ∈1ᐱ(φn2cn/∘⧊°n1cn), ∈1ᐱ(φn2cn/∘∇°n1cn)

1ᐱ(Θn2/An1), ∈1ᐱ(Θn2/Bn1), ∈1ᐱ(Θn2/Dn1), ∈1ᐱ(Θn2/En1), ∈1ᐱ(Θn2/Fn1), ∈1ᐱ(Θn2/Gn1), ∈1ᐱ(Θn2/Hn1), ∈1ᐱ(Θn2/In1), ∈1ᐱ(Θn2/Jn1), ∈1ᐱ(Θn2/Kn1), ∈1ᐱ(Θn2/Ln1), ∈1ᐱ(Θn2/Mn1), ∈1ᐱ(Θn2/Nn1), ∈1ᐱ(Θn2/On1), ∈1ᐱ(Θn2/Pn1), ∈1ᐱ(Θn2/Qn1), ∈1ᐱ(Θn2/Rn1), ∈1ᐱ(Θn2/Sn1), ∈1ᐱ(Θn2/Tn1),∈1ᐱ(Θn2/Un1),  ∈1ᐱ(Θn2/Vn1), ∈1ᐱ(Θn2/Wn1), ∈1ᐱ(Θn2/Yn1), ∈1ᐱ(Θn2/Zn1), ∈1ᐱ(Θn2n1), 1ᐱ(Θn2/Θn1), ∈1ᐱ(Θn2cn/n1cn), ∈1ᐱ(Θn2cn/n1cn), ∈1ᐱ(Θn2cn/∘⧊°n1cn), ∈1ᐱ(Θn2cn/∘∇°n1cn)


2=(n1/n2)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

Function path 2=(nn1cn/nn2cn) is nn1cn previous number in a set of consecutive variables divided by nn2cn later number in a set of consecutive variables, such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant.

2ᐱ(An1/An2), ∈2ᐱ(An1/Bn2), ∈2ᐱ(An1/Dn2), ∈2ᐱ(An1/En2), ∈2ᐱ(An1/Fn2), ∈2ᐱ(An1/Gn2), ∈2ᐱ(An1/Hn2), ∈2ᐱ(An1/In2), ∈2ᐱ(An1/Jn2), ∈2ᐱ(An1/Kn2), ∈2ᐱ(An1/Ln2), ∈2ᐱ(An1/Mn2), ∈2ᐱ(An1/Nn2), ∈2ᐱ(An1/On2), ∈2ᐱ(An1/Pn2), ∈2ᐱ(An1/Qn2), ∈2ᐱ(An1/Rn2), ∈2ᐱ(An1/Sn2), ∈2ᐱ(An1/Tn2),∈2ᐱ(An1/Un2),  ∈2ᐱ(An1/Vn2), ∈2ᐱ(An1/Wn2), ∈2ᐱ(An1/Yn2), ∈2ᐱ(An1/Zn2), ∈2ᐱ(An1n2), ∈2ᐱ(An1n2), 2ᐱ(An1cn/ᐱn2cn), ∈2ᐱ(An1cn/ᗑn2cn), ∈2ᐱ(An1cn/∘⧊°n2cn), ∈2ᐱ(An1cn/∘∇°n2cn)

2ᐱ(Bn1/An2), 2ᐱ(Bn1/Bn2), ∈2ᐱ(Bn1/Dn2), ∈2ᐱ(Bn1/En2), ∈2ᐱ(Bn1/Fn2), ∈2ᐱ(Bn1/Gn2), ∈2ᐱ(Bn1/Hn2), ∈2ᐱ(Bn1/In2), ∈2ᐱ(Bn1/Jn2), ∈2ᐱ(Bn1/Kn2), ∈2ᐱ(Bn1/Ln2), ∈2ᐱ(Bn1/Mn2), ∈2ᐱ(Bn1/Nn2), ∈2ᐱ(Bn1/On2), ∈2ᐱ(Bn1/Pn2), ∈2ᐱ(Bn1/Qn2), ∈2ᐱ(Bn1/Rn2), ∈2ᐱ(Bn1/Sn2), ∈2ᐱ(Bn1/Tn2),∈2ᐱ(Bn1/Un2),  ∈2ᐱ(Bn1/Vn2), ∈2ᐱ(Bn1/Wn2), ∈2ᐱ(Bn1/Yn2), ∈2ᐱ(Bn1/Zn2), ∈2ᐱ(Bn1n2), ∈2ᐱ(Bn1n2),2ᐱ(Bn1cn/ᐱn2cn), ∈2ᐱ(Bn1cn/ᗑn2cn), ∈2ᐱ(Bn1cn/∘⧊°n2cn), ∈2ᐱ(Bn1cn/∘∇°n2cn)

2ᐱ(Dn1/An2), ∈2ᐱ(Dn1/Bn2), 2ᐱ(Dn1/Dn2), ∈2ᐱ(Dn1/En2), ∈2ᐱ(Dn1/Fn2), ∈2ᐱ(Dn1/Gn2), ∈2ᐱ(Dn1/Hn2), ∈2ᐱ(Dn1/In2), ∈2ᐱ(Dn1/Jn2), ∈2ᐱ(Dn1/Kn2), ∈2ᐱ(Dn1/Ln2), ∈2ᐱ(Dn1/Mn2), ∈2ᐱ(Dn1/Nn2), ∈2ᐱ(Dn1/On2), ∈2ᐱ(Dn1/Pn2), ∈2ᐱ(Dn1/Qn2), ∈2ᐱ(Dn1/Rn2), ∈2ᐱ(Dn1/Sn2), ∈2ᐱ(Dn1/Tn2),∈2ᐱ(Dn1/Un2),  ∈2ᐱ(Dn1/Vn2), ∈2ᐱ(Dn1/Wn2), ∈2ᐱ(Dn1/Yn2), ∈2ᐱ(Dn1/Zn2), ∈2ᐱ(Dn1n2), ∈2ᐱ(Dn1n2), 2ᐱ(Dn1cn/ᐱn2cn), ∈2ᐱ(Dn1cn/ᗑn2cn), ∈2ᐱ(Dn1cn/∘⧊°n2cn), ∈2ᐱ(Dn1cn/∘∇°n2cn)

2ᐱ(En1/An2), ∈2ᐱ(En1/Bn2), ∈2ᐱ(En1/Dn2), 2ᐱ(En1/En2), ∈2ᐱ(En1/Fn2), ∈2ᐱ(En1/Gn2), ∈2ᐱ(En1/Hn2), ∈2ᐱ(En1/In2), ∈2ᐱ(En1/Jn2), ∈2ᐱ(En1/Kn2), ∈2ᐱ(En1/Ln2), ∈2ᐱ(En1/Mn2), ∈2ᐱ(En1/Nn2), ∈2ᐱ(En1/On2), ∈2ᐱ(En1/Pn2), ∈2ᐱ(En1/Qn2), ∈2ᐱ(En1/Rn2), ∈2ᐱ(En1/Sn2), ∈2ᐱ(En1/Tn2),∈2ᐱ(En1/Un2),  ∈2ᐱ(En1/Vn2), ∈2ᐱ(En1/Wn2), ∈2ᐱ(En1/Yn2), ∈2ᐱ(En1/Zn2), ∈2ᐱ(En1n2), ∈2ᐱ(En1n2),2ᐱ(En1cn/ᐱn2cn), ∈2ᐱ(En1cn/ᗑn2cn), ∈2ᐱ(En1cn/∘⧊°n2cn), ∈2ᐱ(En1cn/∘∇°n2cn)

2ᐱ(Fn1/An2), ∈2ᐱ(Fn1/Bn2), ∈2ᐱ(Fn1/Dn2), ∈2ᐱ(Fn1/En2), 2ᐱ(Fn1/Fn2), ∈2ᐱ(Fn1/Gn2), ∈2ᐱ(Fn1/Hn2), ∈2ᐱ(Fn1/In2), ∈2ᐱ(Fn1/Jn2), ∈2ᐱ(Fn1/Kn2), ∈2ᐱ(Fn1/Ln2), ∈2ᐱ(Fn1/Mn2), ∈2ᐱ(Fn1/Nn2), ∈2ᐱ(Fn1/On2), ∈2ᐱ(Fn1/Pn2), ∈2ᐱ(Fn1/Qn2), ∈2ᐱ(Fn1/Rn2), ∈2ᐱ(Fn1/Sn2), ∈2ᐱ(Fn1/Tn2),∈2ᐱ(Fn1/Un2),  ∈2ᐱ(Fn1/Vn2), ∈2ᐱ(Fn1/Wn2), ∈2ᐱ(Fn1/Yn2), ∈2ᐱ(Fn1/Zn2), ∈2ᐱ(Fn1n2), ∈2ᐱ(Fn1n2),2ᐱ(Fn1cn/ᐱn2cn), ∈2ᐱ(Fn1cn/ᗑn2cn), ∈2ᐱ(Fn1cn/∘⧊°n2cn), ∈2ᐱ(Fn1cn/∘∇°n2cn)

2ᐱ(Gn1/An2), ∈2ᐱ(Gn1/Bn2), ∈2ᐱ(Gn1/Dn2), ∈2ᐱ(Gn1/En2), ∈2ᐱ(Gn1/Fn2), 2ᐱ(Gn1/Gn2), ∈2ᐱ(Gn1/Hn2), ∈2ᐱ(Gn1/In2), ∈2ᐱ(Gn1/Jn2), ∈2ᐱ(Gn1/Kn2), ∈2ᐱ(Gn1/Ln2), ∈2ᐱ(Gn1/Mn2), ∈2ᐱ(Gn1/Nn2), ∈2ᐱ(Gn1/On2), ∈2ᐱ(Gn1/Pn2), ∈2ᐱ(Gn1/Qn2), ∈2ᐱ(Gn1/Rn2), ∈2ᐱ(Gn1/Sn2), ∈2ᐱ(Gn1/Tn2),∈2ᐱ(Gn1/Un2),  ∈2ᐱ(Gn1/Vn2), ∈2ᐱ(Gn1/Wn2), ∈2ᐱ(Gn1/Yn2), ∈2ᐱ(Gn1/Zn2), ∈2ᐱ(Gn1n2), ∈2ᐱ(Gn1n2),2ᐱ(Gn1cn/ᐱn2cn), ∈2ᐱ(Gn1cn/ᗑn2cn), ∈2ᐱ(Gn1cn/∘⧊°n2cn), ∈2ᐱ(Gn1cn/∘∇°n2cn)

2ᐱ(Hn1/An2), ∈2ᐱ(Hn1/Bn2), ∈2ᐱ(Hn1/Dn2), ∈2ᐱ(Hn1/En2), ∈2ᐱ(Hn1/Fn2), ∈2ᐱ(Hn1/Gn2), 2ᐱ(Hn1/Hn2), ∈2ᐱ(Hn1/In2), ∈2ᐱ(Hn1/Jn2), ∈2ᐱ(Hn1/Kn2), ∈2ᐱ(Hn1/Ln2), ∈2ᐱ(Hn1/Mn2), ∈2ᐱ(Hn1/Nn2), ∈2ᐱ(Hn1/On2), ∈2ᐱ(Hn1/Pn2), ∈2ᐱ(Hn1/Qn2), ∈2ᐱ(Hn1/Rn2), ∈2ᐱ(Hn1/Sn2), ∈2ᐱ(Hn1/Tn2),∈2ᐱ(Hn1/Un2),  ∈2ᐱ(Hn1/Vn2), ∈2ᐱ(Hn1/Wn2), ∈2ᐱ(Hn1/Yn2), ∈2ᐱ(Hn1/Zn2), ∈2ᐱ(Hn1n2), ∈2ᐱ(Hn1n2),2ᐱ(Hn1cn/ᐱn2cn), ∈2⅄Xᐱ(Hn1cn/ᗑn2cn), ∈2ᐱ(Hn1cn/∘⧊°n2cn), ∈2ᐱ(Hn1cn/∘∇°n2cn)

2ᐱ(In1/An2), ∈2ᐱ(In1/Bn2), ∈2ᐱ(In1/Dn2), ∈2ᐱ(In1/En2), ∈2ᐱ(In1/Fn2), ∈2ᐱ(In1/Gn2), ∈2ᐱ(In1/Hn2), 2ᐱ(In1/In2), ∈2ᐱ(In1/Jn2), ∈2ᐱ(In1/Kn2), ∈2ᐱ(In1/Ln2), ∈2ᐱ(In1/Mn2), ∈2ᐱ(In1/Nn2), ∈2ᐱ(In1/On2), ∈2ᐱ(In1/Pn2), ∈2ᐱ(In1/Qn2), ∈2ᐱ(In1/Rn2), ∈2ᐱ(In1/Sn2), ∈2ᐱ(In1/Tn2),∈2ᐱ(In1/Un2),  ∈2ᐱ(In1/Vn2), ∈2ᐱ(In1/Wn2), ∈2ᐱ(In1/Yn2), ∈2ᐱ(In1/Zn2), ∈2ᐱ(In1n2), ∈2ᐱ(In1n2),2ᐱ(In1cn/ᐱn2cn), ∈2ᐱ(In1cn/ᗑn2cn), ∈2ᐱ(In1cn/∘⧊°n2cn), ∈2ᐱ(In1cn/∘∇°n2cn)

2ᐱ(Jn1/An2), ∈2ᐱ(Jn1/Bn2), ∈2ᐱ(Jn1/Dn2), ∈2ᐱ(Jn1/En2), ∈2ᐱ(Jn1/Fn2), ∈2ᐱ(Jn1/Gn2), ∈2ᐱ(Jn1/Hn2), ∈2ᐱ(Jn1/In2), 2ᐱ(Jn1/Jn2), ∈2ᐱ(Jn1/Kn2), ∈2ᐱ(Jn1/Ln2), ∈2ᐱ(Jn1/Mn2), ∈2ᐱ(Jn1/Nn2), ∈2ᐱ(Jn1/On2), ∈2ᐱ(Jn1/Pn2), ∈2ᐱ(Jn1/Qn2), ∈2ᐱ(Jn1/Rn2), ∈2ᐱ(Jn1/Sn2), ∈2ᐱ(Jn1/Tn2),∈2ᐱ(Jn1/Un2),  ∈2ᐱ(Jn1/Vn2), ∈2ᐱ(Jn1/Wn2), ∈2ᐱ(Jn1/Yn2), ∈2ᐱ(Jn1/Zn2), ∈2ᐱ(Jn1n2), ∈2ᐱ(Jn1n2),2ᐱ(Jn1cn/ᐱn2cn), ∈2ᐱ(Jn1cn/ᗑn2cn), ∈2ᐱ(Jn1cn/∘⧊°n2cn), ∈2ᐱ(Jn1cn/∘∇°n2cn)

2ᐱ(Kn1/An2), ∈2ᐱ(Kn1/Bn2), ∈2ᐱ(Kn1/Dn2), ∈2ᐱ(Kn1/En2), ∈2ᐱ(Kn1/Fn2), ∈2ᐱ(Kn1/Gn2), ∈2ᐱ(Kn1/Hn2), ∈2ᐱ(Kn1/In2), ∈2ᐱ(Kn1/Jn2), 2ᐱ(Kn1/Kn2), ∈2ᐱ(Kn1/Ln2), ∈2ᐱ(Kn1/Mn2), ∈2ᐱ(Kn1/Nn2), ∈2ᐱ(Kn1/On2), ∈2ᐱ(Kn1/Pn2), ∈2ᐱ(Kn1/Qn2), ∈2ᐱ(Kn1/Rn2), ∈2ᐱ(Kn1/Sn2), ∈2ᐱ(Kn1/Tn2),∈2ᐱ(Kn1/Un2),  ∈2ᐱ(Kn1/Vn2), ∈2ᐱ(Kn1/Wn2), ∈2ᐱ(Kn1/Yn2), ∈2ᐱ(Kn1/Zn2), ∈2ᐱ(Kn1n2), ∈2ᐱ(Kn1n2),2ᐱ(Kn1cn/ᐱn2cn), ∈2ᐱ(Kn1cn/ᗑn2cn), ∈2ᐱ(Kn1cn/∘⧊°n2cn), ∈2ᐱ(Kn1cn/∘∇°n2cn)

2ᐱ(Ln1/An2), ∈2ᐱ(Ln1/Bn2), ∈2ᐱ(Ln1/Dn2), ∈2ᐱ(Ln1/En2), ∈2ᐱ(Ln1/Fn2), ∈2ᐱ(Ln1/Gn2), ∈2ᐱ(Ln1/Hn2), ∈2ᐱ(Ln1/In2), ∈2ᐱ(Ln1/Jn2), ∈2ᐱ(Ln1/Kn2), 2ᐱ(Ln1/Ln2), ∈2ᐱ(Ln1/Mn2), ∈2ᐱ(Ln1/Nn2), ∈2ᐱ(Ln1/On2), ∈2ᐱ(Ln1/Pn2), ∈2ᐱ(Ln1/Qn2), ∈2ᐱ(Ln1/Rn2), ∈2ᐱ(Ln1/Sn2), ∈2ᐱ(Ln1/Tn2),∈2ᐱ(Ln1/Un2),  ∈2ᐱ(Ln1/Vn2), ∈2ᐱ(Ln1/Wn2), ∈2ᐱ(Ln1/Yn2), ∈2ᐱ(Ln1/Zn2), ∈2ᐱ(Ln1n2), ∈2ᐱ(Ln1n1)),2ᐱ(Ln1cn/ᐱn2cn), ∈2ᐱ(Ln1cn/ᗑn2cn), ∈2ᐱ(Ln1cn/∘⧊°n2cn), ∈2ᐱ(Ln1cn/∘∇°n2cn)

2ᐱ(Mn1/An2), ∈2ᐱ(Mn1/Bn2), ∈2ᐱ(Mn1/Dn2), ∈2ᐱ(Mn1/En2), ∈2ᐱ(Mn1/Fn2), ∈2ᐱ(Mn1/Gn2), ∈2ᐱ(Mn1/Hn2), ∈2ᐱ(Mn1/In2), ∈2ᐱ(Mn1/Jn2), ∈2ᐱ(Mn1/Kn2), ∈2ᐱ(Mn1/Ln2), 2ᐱ(Mn1/Mn2), ∈2ᐱ(Mn1/Nn2), ∈2ᐱ(Mn1/On2), ∈2ᐱ(Mn1/Pn2), ∈2ᐱ(Mn1/Qn2), ∈2ᐱ(Mn1/Rn2), ∈2ᐱ(Mn1/Sn2), ∈2ᐱ(Mn1/Tn2),∈2ᐱ(Mn1/Un2),  ∈2ᐱ(Mn1/Vn2), ∈2ᐱ(Mn1/Wn2), ∈2ᐱ(Mn1/Yn2), ∈2ᐱ(Mn1/Zn2), ∈2ᐱ(Mn1n2), ∈2ᐱ(Mn1n2),2ᐱ(Mn1cn/ᐱn2cn), ∈2ᐱ(Mn1cn/ᗑn2cn), ∈2ᐱ(Mn1cn/∘⧊°n2cn), ∈2ᐱ(Mn1cn/∘∇°n2cn)

2ᐱ(Nn1/An2), ∈2ᐱ(Nn1/Bn2), ∈2ᐱ(Nn1/Dn2), ∈2ᐱ(Nn1/En2), ∈2ᐱ(Nn1/Fn2), ∈2ᐱ(Nn1/Gn2), ∈2ᐱ(Nn1/Hn2), ∈2ᐱ(Nn1/In2), ∈2ᐱ(Nn1/Jn2), ∈2ᐱ(Nn1/Kn2), ∈2ᐱ(Nn1/Ln2), ∈2ᐱ(Nn1/Mn2), 2ᐱ(Nn1/Nn2), ∈2ᐱ(Nn1/On2), ∈2ᐱ(Nn1/Pn2), ∈2ᐱ(Nn1/Qn2), ∈2ᐱ(Nn1/Rn2), ∈2ᐱ(Nn1/Sn2), ∈2ᐱ(Nn1/Tn2),∈2ᐱ(Nn1/Un2),  ∈2ᐱ(Nn1/Vn2), ∈2ᐱ(Nn1/Wn2), ∈2ᐱ(Nn1/Yn2), ∈2ᐱ(Nn1/Zn2), ∈2ᐱ(Nn1n2), ∈2ᐱ(Nn1n2),2ᐱ(Nn1cn/ᐱn2cn), ∈2ᐱ(Nn1cn/ᗑn2cn), ∈2ᐱ(Nn1cn/∘⧊°n2cn), ∈2ᐱ(Nn1cn/∘∇°n2cn)

2ᐱ(On1/An2), ∈2ᐱ(On1/Bn2), ∈2ᐱ(On1/Dn2), ∈2ᐱ(On1/En2), ∈2ᐱ(On1/Fn2), ∈2ᐱ(On1/Gn2), ∈2ᐱ(On1/Hn2), ∈2ᐱ(On1/In2), ∈2ᐱ(On1/Jn2), ∈2ᐱ(On1/Kn2), ∈2ᐱ(On1/Ln2), ∈2ᐱ(On1/Mn2), ∈2ᐱ(On1/Nn2), 2ᐱ(On1/On2), ∈2ᐱ(On1/Pn2), ∈2ᐱ(On1/Qn2), ∈2ᐱ(On1/Rn2), ∈2ᐱ(On1/Sn2), ∈2ᐱ(On1/Tn2),∈2ᐱ(On1/Un2),  ∈2ᐱ(On1/Vn2), ∈2ᐱ(On1/Wn2), ∈2ᐱ(On1/Yn2), ∈2ᐱ(On1/Zn2), ∈2ᐱ(On1n2), ∈2ᐱ(On1n2),2ᐱ(On1cn/ᐱn2cn), ∈2ᐱ(On1cn/ᗑn2cn), ∈2ᐱ(On1cn/∘⧊°n2cn), ∈2ᐱ(On1cn/∘∇°n2cn)

2ᐱ(Pn1/An2), ∈2ᐱ(Pn1/Bn2), ∈2ᐱ(Pn1/Dn2), ∈2ᐱ(Pn1/En2), ∈2ᐱ(Pn1/Fn2), ∈2ᐱ(Pn1/Gn2), ∈2ᐱ(Pn1/Hn2), ∈2ᐱ(Pn1/In2), ∈2ᐱ(Pn1/Jn2), ∈2ᐱ(Pn1/Kn2), ∈2ᐱ(Pn1/Ln2), ∈2ᐱ(Pn1/Mn2), ∈2ᐱ(Pn1/Nn2), ∈2ᐱ(Pn1/On2), 2ᐱ(Pn1/Pn2), ∈2ᐱ(Pn1/Qn2), ∈2ᐱ(Pn1/Rn2), ∈2ᐱ(Pn1/Sn2), ∈2ᐱ(Pn1/Tn2),∈2ᐱ(Pn1/Un2),  ∈2ᐱ(Pn1/Vn2), ∈2ᐱ(Pn1/Wn2), ∈2ᐱ(Pn1/Yn2), ∈2ᐱ(Pn1/Zn2), ∈2ᐱ(Pn1n2), ∈2ᐱ(Pn1n2),2ᐱ(Pn1cn/ᐱn2cn), ∈2ᐱ(Pn1cn/ᗑn2cn), ∈2ᐱ(Pn1cn/∘⧊°n2cn), ∈2ᐱ(Pn1cn/∘∇°n2cn)

2ᐱ(Qn1/An2), ∈2ᐱ(Qn1/Bn2), ∈2ᐱ(Qn1/Dn2), ∈2ᐱ(Qn1/En2), ∈2ᐱ(Qn1/Fn2), ∈2ᐱ(Qn1/Gn2), ∈2ᐱ(Qn1/Hn2), ∈2ᐱ(Qn1/In2), ∈2ᐱ(Qn1/Jn2), ∈2ᐱ(Qn1/Kn2), ∈2ᐱ(Qn1/Ln2), ∈2ᐱ(Qn1/Mn2), ∈2ᐱ(Qn1/Nn2), ∈2ᐱ(Qn1/On2), ∈2ᐱ(Qn1/Pn2), 2ᐱ(Qn1/Qn2), ∈2ᐱ(Qn1/Rn2), ∈2ᐱ(Qn1/Sn2), ∈2ᐱ(Qn1/Tn2),∈2ᐱ(Qn1/Un2),  ∈2ᐱ(Qn1/Vn2), ∈2ᐱ(Qn1/Wn2), ∈2ᐱ(Qn1/Yn2), ∈2ᐱ(Qn1/Zn2), ∈2ᐱ(Qn1n2), ∈2ᐱ(Qn1n2),2ᐱ(Qn1cn/ᐱn2cn), ∈2ᐱ(Qn1cn/ᗑn2cn), ∈2ᐱ(Qn1cn/∘⧊°n2cn), ∈2ᐱ(Qn1cn/∘∇°n2cn)

2ᐱ(Rn1/An2), ∈2ᐱ(Rn1/Bn2), ∈2ᐱ(Rn1/Dn2), ∈2ᐱ(Rn1/En2), ∈2ᐱ(Rn1/Fn2), ∈2ᐱ(Rn1/Gn2), ∈2ᐱ(Rn1/Hn2), ∈2ᐱ(Rn1/In2), ∈2ᐱ(Rn1/Jn2), ∈2ᐱ(Rn1/Kn2), ∈2ᐱ(Rn1/Ln2), ∈2ᐱ(Rn1/Mn2), ∈2ᐱ(Rn1/Nn2), ∈2ᐱ(Rn1/On2), ∈2ᐱ(Rn1/Pn2), ∈2ᐱ(Rn1/Qn2), 2ᐱ(Rn1/Rn2), ∈2ᐱ(Rn1/Sn2), ∈2ᐱ(Rn1/Tn2),∈2ᐱ(Rn1/Un2),  ∈2ᐱ(Rn1/Vn2), ∈2ᐱ(Rn1/Wn2), ∈2ᐱ(Rn1/Yn2), ∈2ᐱ(Rn1/Zn2), ∈2ᐱ(Rn1n2), ∈2ᐱ(Rn1n2),2ᐱ(Rn1cn/ᐱn2cn), ∈2ᐱ(Rn1cn/ᗑn2cn), ∈2ᐱ(Rn1cn/∘⧊°n2cn), ∈2ᐱ(Rn1cn/∘∇°n2cn)

2ᐱ(Sn1/An2), ∈2ᐱ(Sn1/Bn2), ∈2ᐱ(Sn1/Dn2), ∈2ᐱ(Sn1/En2), ∈2ᐱ(Sn1/Fn2), ∈2ᐱ(Sn1/Gn2), ∈2ᐱ(Sn1/Hn2), ∈2ᐱ(Sn1/In2), ∈2ᐱ(Sn1/Jn2), ∈2ᐱ(Sn1/Kn2), ∈2ᐱ(Sn1/Ln2), ∈2ᐱ(Sn1/Mn2), ∈2ᐱ(Sn1/Nn2), ∈2ᐱ(Sn1/On2), ∈2ᐱ(Sn1/Pn2), ∈2ᐱ(Sn1/Qn2), ∈2ᐱ(Sn1/Rn2), 2ᐱ(Sn1/Sn2), ∈2ᐱ(Sn1/Tn2),∈2ᐱ(Sn1/Un2),  ∈2ᐱ(Sn1/Vn2), ∈2ᐱ(Sn1/Wn2), ∈2ᐱ(Sn1/Yn2), ∈2ᐱ(Sn1/Zn2), ∈2ᐱ(Sn1n2), ∈2ᐱ(Sn1n2),2ᐱ(Sn1cn/ᐱn2cn), ∈2ᐱ(Sn1cn/ᗑn2cn), ∈2ᐱ(Sn1cn/∘⧊°n2cn), ∈2ᐱ(Sn1cn/∘∇°n2cn)

2ᐱ(Tn1/An2), ∈2ᐱ(Tn1/Bn2), ∈2ᐱ(Tn1/Dn2), ∈2ᐱ(Tn1/En2), ∈2ᐱ(Tn1/Fn2), ∈2ᐱ(Tn1/Gn2), ∈2ᐱ(Tn1/Hn2), ∈2ᐱ(Tn1/In2), ∈2ᐱ(Tn1/Jn2), ∈2ᐱ(Tn1/Kn2), ∈2ᐱ(Tn1/Ln2), ∈2ᐱ(Tn1/Mn2), ∈2ᐱ(Tn1/Nn2), ∈2ᐱ(Tn1/On2), ∈2ᐱ(Tn1/Pn2), ∈2ᐱ(Tn1/Qn2), ∈2ᐱ(Tn1/Rn2), ∈2ᐱ(Tn1/Sn2), 2ᐱ(Tn1/Tn2),∈2ᐱ(Tn1/Un2),  ∈2ᐱ(Tn1/Vn2), ∈2ᐱ(Tn1/Wn2), ∈2ᐱ(Tn1/Yn2), ∈2ᐱ(Tn1/Zn2), ∈2ᐱ(Tn1n2), ∈2ᐱ(Tn1n2),2ᐱ(Tn1cn/ᐱn2cn), ∈2ᐱ(Tn1cn/ᗑn2cn), ∈2ᐱ(Tn1cn/∘⧊°n2cn), ∈2ᐱ(Tn1cn/∘∇°n2cn)

2ᐱ(Un1/An2), ∈2ᐱ(Un1/Bn2), ∈2ᐱ(Un1/Dn2), ∈2ᐱ(Un1/En2), ∈2ᐱ(Un1/Fn2), ∈2ᐱ(Un1/Gn2), ∈2ᐱ(Un1/Hn2), ∈2ᐱ(Un1/In2), ∈2ᐱ(Un1/Jn2), ∈2ᐱ(Un1/Kn2), ∈2ᐱ(Un1/Ln2), ∈2ᐱ(Un1/Mn2), ∈2ᐱ(Un1/Nn2), ∈2ᐱ(Un1/On2), ∈2ᐱ(Un1/Pn2), ∈2ᐱ(Un1/Qn2), ∈n2ᐱ(Un1/Rn2), ∈2ᐱ(Un1/Sn2), ∈2ᐱ(Un1/Tn2), 2ᐱ(Un1/Un2),  ∈2ᐱ(Un1/Vn2), ∈2ᐱ(Un1/Wn2), ∈2ᐱ(Un1/Yn2), ∈2ᐱ(Un1/Zn2), ∈2ᐱ(Un1n2), ∈2ᐱ(Un1n2),2ᐱ(Un1cn/ᐱn2cn), ∈2ᐱ(Un1cn/ᗑn2cn), ∈2ᐱ(Un1cn/∘⧊°n2cn), ∈2ᐱ(Un1cn/∘∇°n2cn)

2ᐱ(Vn1/An2), ∈2ᐱ(Vn1/Bn2), ∈2ᐱ(Vn1/Dn2), ∈2ᐱ(Vn1/En2), ∈2ᐱ(Vn1/Fn2), ∈2ᐱ(Vn1/Gn2), ∈2ᐱ(Vn1/Hn2), ∈2ᐱ(Vn1/In2), ∈2ᐱ(Vn1/Jn2), ∈2ᐱ(Vn1/Kn2), ∈2ᐱ(Vn1/Ln2), ∈2ᐱ(Vn1/Mn2), ∈2ᐱ(Vn1/Nn2), ∈2ᐱ(Vn1/On2), ∈2ᐱ(Vn1/Pn2), ∈2ᐱ(Vn1/Qn2), ∈2ᐱ(Vn1/Rn2), ∈2ᐱ(Vn1/Sn2), ∈2ᐱ(Vn1/Tn2),∈2ᐱ(Vn1/Un2),  2ᐱ(Vn1/Vn2), ∈2ᐱ(Vn1/Wn2), ∈2ᐱ(Vn1/Yn2), ∈2ᐱ(Vn1/Zn2), ∈2ᐱ(Vn1n2), ∈2ᐱ(Vn1n2),2ᐱ(Vn1cn/ᐱn2cn), ∈2ᐱ(Vn1cn/ᗑn2cn), ∈2ᐱ(Vn1cn/∘⧊°n2cn), ∈2ᐱ(Vn1cn/∘∇°n2cn)

2ᐱ(Wn1/An2), ∈2ᐱ(Wn1/Bn2), ∈2ᐱ(Wn1/Dn2), ∈2ᐱ(Wn1/En2), ∈2ᐱ(Wn1/Fn2), ∈2ᐱ(Wn1/Gn2), ∈2ᐱ(Wn1/Hn2), ∈2ᐱ(Wn1/In2), ∈2ᐱ(Wn1/Jn2), ∈2ᐱ(Wn1/Kn2), ∈2ᐱ(Wn1/Ln2), ∈2ᐱ(Wn1/Mn2), ∈2ᐱ(Wn1/Nn2), ∈2ᐱ(Wn1/On2), ∈2ᐱ(Wn1/Pn2), ∈2ᐱ(Wn1/Qn2), ∈2ᐱ(Wn1/Rn2), ∈2ᐱ(Wn1/Sn2), ∈2ᐱ(Wn1/Tn2),∈2ᐱ(Wn1/Un2),  ∈2ᐱ(Wn1/Vn2), 2ᐱ(Wn1/Wn2), ∈2ᐱ(Wn1/Yn2), ∈2ᐱ(Wn1/Zn2), ∈2ᐱ(Wn1n2), ∈2ᐱ(Wn1n2),2ᐱ(Wn1cn/ᐱn2cn), ∈2ᐱ(Wn1cn/ᗑn2cn), ∈2ᐱ(Wn1cn/∘⧊°n2cn), ∈2ᐱ(Wn1cn/∘∇°n2cn)

2ᐱ(Yn1/An2), ∈2ᐱ(Yn1/Bn2), ∈2ᐱ(Yn1/Dn2), ∈2ᐱ(Yn1/En2), ∈2ᐱ(Yn1/Fn2), ∈2ᐱ(Yn1/Gn2), ∈2ᐱ(Yn1/Hn2), ∈2ᐱ(Yn1/In2), ∈2ᐱ(Yn1/Jn2), ∈2ᐱ(Yn1/Kn2), ∈2ᐱ(Yn1/Ln2), ∈2ᐱ(Yn1/Mn2), ∈2ᐱ(Yn1/Nn2), ∈2ᐱ(Yn1/On2), ∈2ᐱ(Yn1/Pn2), ∈2ᐱ(Yn1/Qn2), ∈2ᐱ(Yn1/Rn2), ∈2ᐱ(Yn1/Sn2), ∈2ᐱ(Yn1/Tn2),∈2ᐱ(Yn1/Un2),  ∈2ᐱ(Yn1/Vn2), ∈2ᐱ(Yn1/Wn2), 2ᐱ(Yn1/Yn2), ∈2ᐱ(Yn1/Zn2), ∈2ᐱ(Yn1n2), ∈2ᐱ(Yn1n2),2ᐱ(Yn1cn/ᐱn2cn), ∈2ᐱ(Yn1cn/ᗑn2cn), ∈2ᐱ(Yn1cn/∘⧊°n2cn), ∈2ᐱ(Yn1cn/∘∇°n2cn)

2ᐱ(Zn1/An2), ∈2ᐱ(Zn1/Bn2), ∈2ᐱ(Zn1/Dn2), ∈2ᐱ(Zn1/En2), ∈2ᐱ(Zn1/Fn2), ∈2ᐱ(Zn1/Gn2), ∈2ᐱ(Zn1/Hn2), ∈2ᐱ(Zn1/In2), ∈2ᐱ(Zn1/Jn2), ∈2ᐱ(Zn1/Kn2), ∈2ᐱ(Zn1/Ln2), ∈2ᐱ(Zn1/Mn2), ∈2ᐱ(Zn1/Nn2), ∈2ᐱ(Zn1/On2), ∈2ᐱ(Zn1/Pn2), ∈2ᐱ(Zn1/Qn2), ∈2ᐱ(Zn1/Rn2), ∈2ᐱ(Zn1/Sn2), ∈2ᐱ(Zn1/Tn2),∈2ᐱ(Zn1/Un2),  ∈2ᐱ(Zn1/Vn2), ∈2ᐱ(Zn1/Wn2), ∈2ᐱ(Zn1/Yn2), 2ᐱ(Zn1/Zn2), ∈2ᐱ(Zn1n2), ∈2ᐱ(Zn1n2),2ᐱ(Zn1cn/ᐱn2cn), ∈2ᐱ(Zn1cn/ᗑn2cn), ∈2ᐱ(Zn1cn/∘⧊°n2cn), ∈2ᐱ(Zn1cn/∘∇°n2cn)

2ᐱ(φn1/An2), ∈2ᐱ(φn1/Bn2), ∈2ᐱ(φn1/Dn2), ∈2ᐱ(φn1/En2), ∈2ᐱ(φn1/Fn2), ∈2ᐱ(φn1/Gn2), ∈2ᐱ(φn1/Hn2), ∈2ᐱ(φn1/In2), ∈2ᐱ(φn1/Jn2), ∈2ᐱ(φn1/Kn2), ∈2ᐱ(φn1/Ln2), ∈2ᐱ(φn1/Mn2), ∈2ᐱ(φn1/Nn2), ∈2ᐱ(φn1/On2), ∈2ᐱ(φn1/Pn2), ∈2ᐱ(φn1/Qn2), ∈2ᐱ(φn1/Rn2), ∈2ᐱ(φn1/Sn2), ∈2ᐱ(φn1/Tn2),∈2ᐱ(φn1/Un2),  ∈2ᐱ(φn1/Vn2), ∈2ᐱ(φn1/Wn2), ∈2ᐱ(φn1/Yn2), ∈2ᐱ(φn1/Zn2), 2ᐱ(φn1n2), ∈2ᐱ(φn1n2),2ᐱ(φn1cn/ᐱn2cn), ∈2ᐱ(φn1cn/ᗑn2cn), ∈2ᐱ(φn1cn/∘⧊°n2cn), ∈2ᐱ(φn1cn/∘∇°n2cn)

2ᐱ(Θn1/An2), ∈2ᐱ(Θn1/Bn2), ∈2ᐱ(Θn1/Dn2), ∈2ᐱ(Θn1/En2), ∈2ᐱ(Θn1/Fn2), ∈2ᐱ(Θn1/Gn2), ∈2ᐱ(Θn1/Hn2), ∈2ᐱ(Θn1/In2), ∈2ᐱ(Θn1/Jn2), ∈2ᐱ(Θn1/Kn2), ∈2ᐱ(Θn1/Ln2), ∈2ᐱ(Θn1/Mn2), ∈2ᐱ(Θn1/Nn2), ∈2ᐱ(Θn1/On2), ∈2ᐱ(Θn1/Pn2), ∈2ᐱ(Θn1/Qn2), ∈2ᐱ(Θn1/Rn2), ∈2ᐱ(Θn1/Sn2), ∈2ᐱ(Θn1/Tn2),∈2ᐱ(Θn1/Un2),  ∈2ᐱ(Θn1/Vn2), ∈2ᐱ(Θn1/Wn2), ∈2ᐱ(Θn1/Yn2), ∈2ᐱ(Θn1/Zn2), ∈2ᐱ(Θn1n2), 2ᐱ(Θn1n2), ∈2ᐱ(Θn1cn/ᐱn2cn), ∈2ᐱ(Θn1cn/ᗑn2cn), ∈2ᐱ(Θn1cn/∘⧊°n2cn), ∈2ᐱ(Θn1cn/∘∇°n2cn)


3=(n1cn/n1cn)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

Function path 3ncn=(nncn/nncn) is nncn a number in a set of variables with a variant potential change in decimal stem cycle count of cn divided by nncn a number similar in a set of variables with a variant change in decimal stem cycle count of cn , such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant. 


3ncn is not applicable to whole number variables with no decimal stem repeating numerals of set variables nᐱ(Yn/Yn), nᐱ(Yn/Pn), nᐱ(Pn/Pn), and ∈nᐱ(Pn/Yn) aside from noting that a number of a set in whole numbers divided by a same number from its set and will always equal 1 unless the variable 0 zero from Y base is applied as 0/0=0. While any variable no matter the length of decimal divided with zero equals zero and and variable divided with one equals the decimal ratio the number of stem cycles in the factors is important to note in all factoring. 


If it is needed in a system of calculations noted for example 3(Yn/Yn) or 3(Pn/Pn) then it should be noted and if that variable factor is incorrect while a variable very close in value with decimal then that variable may help to allocate the change or loss of a system in quantum field fractals that are polarized to one set or more of numerator and denominator ratio.

Examples of micron numerical variable change with constant stem cycle repeating decimal chains in path 3.

3ncn=(nnc1/nnc2)

3ncn=(nnc2/nnc1)

3ncn=(nnc1/nnc3)

3ncn=(nnc3/nnc1)

3ncn=(nnc2/nnc3)

3ncn=(nnc3/nnc2)


Example 

3ncn=(nncn/nncn) is applicable to set variable below with nᐱ(Pn/Pn), ∈nᐱ(Pn/Yn), ∈nᐱ(Yn/Yn) and ∈nᐱ(Yn/Pn) excluded having no decimal variants to a cn of Y & P variables as they are whole numbers.

[ nncnᐱ(An/An) / nncnᐱ(An/An) ]=Nncn then requires definition of both the variables of nᐱ(An/An) defined and cn of all factors of nᐱ(An/An) since path 1=(nn2cn/nn1cn) and path 2=(nn1cn/nn2cn) then path 3ncn=(nncn/nncn) of nᐱ(An/An) while A represents path 1/Q)cn variables a path 2=(nn1cn/nn2cn) is a function applicable to A variables once defined from path set 1/Q)cn that Q path variable must be defined of 1⅄Q or 2⅄Q from P bases of P to satisfy the specific definition of nᐱ(An/An

if An=1/Q)cn and 1=(An2cn/An1cn)=12An1 while 2=(An1cn/An2cn)=22An1 then nᐱ(An/An)={12An1 : 22An1 : 32An1} potential variable sets while the variant Nncn of Q and A variables then also have potential change to final quotient and must be defined to cn. 


Path 3ncn=(nncn/nncn) function is then applicable to sets and the variables of the sets below

nᐱ(An/An), ∈nᐱ(An/Bn), ∈nᐱ(An/Dn), ∈nᐱ(An/En), ∈nᐱ(An/Fn), ∈nᐱ(An/Gn), ∈nᐱ(An/Hn), ∈nᐱ(An/In), ∈nᐱ(An/Jn), ∈nᐱ(An/Kn), ∈nᐱ(An/Ln), ∈nᐱ(An/Mn), ∈nᐱ(An/Nn), ∈nᐱ(An/On), ∈nᐱ(An/Pn), ∈nᐱ(An/Qn), ∈nᐱ(An/Rn), ∈nᐱ(An/Sn), ∈nᐱ(An/Tn),∈nᐱ(An/Un),  ∈nᐱ(An/Vn), ∈nᐱ(An/Wn), ∈nᐱ(An/Yn), ∈nᐱ(An/Zn), ∈nᐱ(Ann), ∈nᐱ(Ann), nᐱ(Ancn/ᐱncn), ∈nᐱ(Ancn/ᗑncn), ∈nᐱ(Ancn/∘⧊°ncn), ∈nᐱ(Ancn/∘∇°ncn)

nᐱ(Bn/An), nᐱ(Bn/Bn), ∈nᐱ(Bn/Dn), ∈nᐱ(Bn/En), ∈nᐱ(Bn/Fn), ∈nᐱ(Bn/Gn), ∈nᐱ(Bn/Hn), ∈nᐱ(Bn/In), ∈nᐱ(Bn/Jn), ∈nᐱ(Bn/Kn), ∈nᐱ(Bn/Ln), ∈nᐱ(Bn/Mn), ∈nᐱ(Bn/Nn), ∈nᐱ(Bn/On), ∈nᐱ(Bn/Pn), ∈nᐱ(Bn/Qn), ∈nᐱ(Bn/Rn), ∈nᐱ(Bn/Sn), ∈nᐱ(Bn/Tn),∈nᐱ(Bn/Un),  ∈nᐱ(Bn/Vn), ∈nᐱ(Bn/Wn), ∈nᐱ(Bn/Yn), ∈nᐱ(Bn/Zn), ∈nᐱ(Bnn), ∈nᐱ(Bnn),nᐱ(Bncn/ᐱncn), ∈nᐱ(Bncnxᗑncn), ∈nᐱ(Bncn/∘⧊°ncn), ∈nᐱ(Bncn/∘∇°ncn)

nᐱ(Dn/An), ∈nᐱ(Dn/Bn), nᐱ(Dn/Dn), ∈nᐱ(Dn/En), ∈nᐱ(Dn/Fn), ∈nᐱ(Dn/Gn), ∈nᐱ(Dn/Hn), ∈nᐱ(Dn/In), ∈nᐱ(Dn/Jn), ∈nᐱ(Dn/Kn), ∈nᐱ(Dn/Ln), ∈nᐱ(Dn/Mn), ∈nᐱ(Dn/Nn), ∈nᐱ(Dn/On), ∈nᐱ(Dn/Pn), ∈nᐱ(Dn/Qn), ∈nᐱ(Dn/Rn), ∈nᐱ(Dn/Sn), ∈nᐱ(Dn/Tn),∈nᐱ(Dn/Un),  ∈nᐱ(Dn/Vn), ∈nᐱ(Dn/Wn), ∈nᐱ(Dn/Yn), ∈nᐱ(Dn/Zn), ∈nᐱ(Dnn), ∈nᐱ(Dnn), nᐱ(Dncn/ᐱncn), ∈nᐱ(Dncn/ᗑncn), ∈nᐱ(Dncn/∘⧊°ncn), ∈nᐱ(Dncn/∘∇°ncn)

nᐱ(En/An), ∈nᐱ(En/Bn), ∈nᐱ(En/Dn), nᐱ(En/En), ∈nᐱ(En/Fn), ∈nᐱ(En/Gn), ∈nᐱ(En/Hn), ∈nᐱ(En/In), ∈nᐱ(En/Jn), ∈nᐱ(En/Kn), ∈nᐱ(En/Ln), ∈nᐱ(En/Mn), ∈nᐱ(En/Nn), ∈nᐱ(En/On), ∈nᐱ(En/Pn), ∈nᐱ(En/Qn), ∈nᐱ(En/Rn), ∈nᐱ(En/Sn), ∈nᐱ(En/Tn),∈nᐱ(En/Un),  ∈nᐱ(En/Vn), ∈nᐱ(En/Wn), ∈nᐱ(En/Yn), ∈nᐱ(En/Zn), ∈nᐱ(Enn), ∈nᐱ(Enn),nᐱ(Encn/ᐱncn), ∈nᐱ(Encn/ᗑncn), ∈nᐱ(Encn/∘⧊°ncn), ∈nᐱ(Encn/∘∇°ncn)

nᐱ(Fn/An), ∈nᐱ(Fn/Bn), ∈nᐱ(Fn/Dn), ∈nᐱ(Fn/En), nᐱ(Fn/Fn), ∈nᐱ(Fn/Gn), ∈nᐱ(Fn/Hn), ∈nᐱ(Fn/In), ∈nᐱ(Fn/Jn), ∈nᐱ(Fn/Kn), ∈nᐱ(Fn/Ln), ∈nᐱ(Fn/Mn), ∈nᐱ(Fn/Nn), ∈nᐱ(Fn/On), ∈nᐱ(Fn/Pn), ∈nᐱ(Fn/Qn), ∈nᐱ(Fn/Rn), ∈nᐱ(Fn/Sn), ∈nᐱ(Fn/Tn),∈nᐱ(Fn/Un),  ∈nᐱ(Fn/Vn), ∈nᐱ(Fn/Wn), ∈nᐱ(Fn/Yn), ∈nᐱ(Fn/Zn), ∈nᐱ(Fnn), ∈nᐱ(Fnn),nᐱ(Fncn/ᐱncn), ∈nᐱ(Fncn/ᗑncn), ∈nᐱ(Fncn/∘⧊°ncn), ∈nᐱ(Fncn/∘∇°ncn)

nᐱ(Gn/An), ∈nᐱ(Gn/Bn), ∈nᐱ(Gn/Dn), ∈nᐱ(Gn/En), ∈nᐱ(Gn/Fn), nᐱ(Gn/Gn), ∈nᐱ(Gn/Hn), ∈nᐱ(Gn/In), ∈nᐱ(Gn/Jn), ∈nᐱ(Gn/Kn), ∈nᐱ(Gn/Ln), ∈nᐱ(Gn/Mn), ∈nᐱ(Gn/Nn), ∈nᐱ(Gn/On), ∈nᐱ(Gn/Pn), ∈nᐱ(Gn/Qn), ∈nᐱ(Gn/Rn), ∈nᐱ(Gn/Sn), ∈nᐱ(Gn/Tn),∈nᐱ(Gn/Un),  ∈nᐱ(Gn/Vn), ∈nᐱ(Gn/Wn), ∈nᐱ(Gn/Yn), ∈nᐱ(Gn/Zn), ∈nᐱ(Gnn), ∈nᐱ(Gnn),nᐱ(Gncn/ᐱncn), ∈nᐱ(Gncn/ᗑncn), ∈nᐱ(Gncn/∘⧊°ncn), ∈nᐱ(Gncn/∘∇°ncn)

nᐱ(Hn/An), ∈nᐱ(Hn/Bn), ∈nᐱ(Hn/Dn), ∈nᐱ(Hn/En), ∈nᐱ(Hn/Fn), ∈nᐱ(Hn/Gn), nᐱ(Hn/Hn), ∈nᐱ(Hn/In), ∈nᐱ(Hn/Jn), ∈nᐱ(Hn/Kn), ∈nᐱ(Hn/Ln), ∈nᐱ(Hn/Mn), ∈nᐱ(Hn/Nn), ∈nᐱ(Hn/On), ∈nᐱ(Hn/Pn), ∈nᐱ(Hn/Qn), ∈nᐱ(Hn/Rn), ∈nᐱ(Hn/Sn), ∈nᐱ(Hn/Tn),∈nᐱ(Hn/Un),  ∈nᐱ(Hn/Vn), ∈nᐱ(Hn/Wn), ∈nᐱ(Hn/Yn), ∈nᐱ(Hn/Zn), ∈nᐱ(Hnn), ∈nᐱ(Hnn),nᐱ(Hncn/ᐱncn), ∈n⅄Xᐱ(Hncn/ᗑncn), ∈nᐱ(Hncn/∘⧊°ncn), ∈nᐱ(Hncn/∘∇°ncn)

nᐱ(In/An), ∈nᐱ(In/Bn), ∈nᐱ(In/Dn), ∈nᐱ(In/En), ∈nᐱ(In/Fn), ∈nᐱ(In/Gn), ∈nᐱ(In/Hn), nᐱ(In/In), ∈nᐱ(In/Jn), ∈nᐱ(In/Kn), ∈nᐱ(In/Ln), ∈nᐱ(In/Mn), ∈nᐱ(In/Nn), ∈nᐱ(In/On), ∈nᐱ(In/Pn), ∈nᐱ(In/Qn), ∈nᐱ(In/Rn), ∈nᐱ(In/Sn), ∈nᐱ(In/Tn),∈nᐱ(In/Un),  ∈nᐱ(In/Vn), ∈nᐱ(In/Wn), ∈nᐱ(In/Yn), ∈nᐱ(In/Zn), ∈nᐱ(Inn), ∈nᐱ(Inn),nᐱ(Incn/ᐱncn), ∈nᐱ(Incn/ᗑncn), ∈nᐱ(Incn/∘⧊°ncn), ∈nᐱ(Incn/∘∇°ncn)

nᐱ(Jn/An), ∈nᐱ(Jn/Bn), ∈nᐱ(Jn/Dn), ∈nᐱ(Jn/En), ∈nᐱ(Jn/Fn), ∈nᐱ(Jn/Gn), ∈nᐱ(Jn/Hn), ∈nᐱ(Jn/In), nᐱ(Jn/Jn), ∈nᐱ(Jn/Kn), ∈nᐱ(Jn/Ln), ∈nᐱ(Jn/Mn), ∈nᐱ(Jn/Nn), ∈nᐱ(Jn/On), ∈nᐱ(Jn/Pn), ∈nᐱ(Jn/Qn), ∈nᐱ(Jn/Rn), ∈nᐱ(Jn/Sn), ∈nᐱ(Jn/Tn),∈nᐱ(Jn/Un),  ∈nᐱ(Jn/Vn), ∈nᐱ(Jn/Wn), ∈nᐱ(Jn/Yn), ∈nᐱ(Jn/Zn), ∈nᐱ(Jnn), ∈nᐱ(Jnn),nᐱ(Jncn/ᐱncn), ∈nᐱ(Jncn/ᗑncn), ∈nᐱ(Jncn/∘⧊°ncn), ∈nᐱ(Jncn/∘∇°ncn)

nᐱ(Kn/An), ∈nᐱ(Kn/Bn), ∈nᐱ(Kn/Dn), ∈nᐱ(Kn/En), ∈nᐱ(Kn/Fn), ∈nᐱ(Kn/Gn), ∈nᐱ(Kn/Hn), ∈nᐱ(Kn/In), ∈nᐱ(Kn/Jn), nᐱ(Kn/Kn), ∈nᐱ(Kn/Ln), ∈nᐱ(Kn/Mn), ∈nᐱ(Kn/Nn), ∈nᐱ(Kn/On), ∈nᐱ(Kn/Pn), ∈nᐱ(Kn/Qn), ∈nᐱ(Kn/Rn), ∈nᐱ(Kn/Sn), ∈nᐱ(Kn/Tn),∈nᐱ(Kn/Un),  ∈nᐱ(Kn/Vn), ∈nᐱ(Kn/Wn), ∈nᐱ(Kn/Yn), ∈nᐱ(Kn/Zn), ∈nᐱ(Knn), ∈nᐱ(Knn),nᐱ(Kncn/ᐱncn), ∈nᐱ(Kncn/ᗑncn), ∈nᐱ(Kncn/∘⧊°ncn), ∈nᐱ(Kncn/∘∇°ncn)

nᐱ(Ln/An), ∈nᐱ(Ln/Bn), ∈nᐱ(Ln/Dn), ∈nᐱ(Ln/En), ∈nᐱ(Ln/Fn), ∈nᐱ(Ln/Gn), ∈nᐱ(Ln/Hn), ∈nᐱ(Ln/In), ∈nᐱ(Ln/Jn), ∈nᐱ(Ln/Kn), nᐱ(Ln/Ln), ∈nᐱ(Ln/Mn), ∈nᐱ(Ln/Nn), ∈nᐱ(Ln/On), ∈nᐱ(Ln/Pn), ∈nᐱ(Ln/Qn), ∈nᐱ(Ln/Rn), ∈nᐱ(Ln/Sn), ∈nᐱ(Ln/Tn),∈nᐱ(Ln/Un),  ∈nᐱ(Ln/Vn), ∈nᐱ(Ln/Wn), ∈nᐱ(Ln/Yn), ∈nᐱ(Ln/Zn), ∈nᐱ(Lnn), ∈nᐱ(Lnn)),nᐱ(Lncn/ᐱncn), ∈nᐱ(Lncn/ᗑncn), ∈nᐱ(Lncn/∘⧊°ncn), ∈nᐱ(Lncn/∘∇°ncn)

nᐱ(Mn/An), ∈nᐱ(Mn/Bn), ∈nᐱ(Mn/Dn), ∈nᐱ(Mn/En), ∈nᐱ(Mn/Fn), ∈nᐱ(Mn/Gn), ∈nᐱ(Mn/Hn), ∈nᐱ(Mn/In), ∈nᐱ(Mn/Jn), ∈nᐱ(Mn/Kn), ∈nᐱ(Mn/Ln), nᐱ(Mn/Mn), ∈nᐱ(Mn/Nn), ∈nᐱ(Mn/On), ∈nᐱ(Mn/Pn), ∈nᐱ(Mn/Qn), ∈nᐱ(Mn/Rn), ∈nᐱ(Mn/Sn), ∈nᐱ(Mn/Tn),∈nᐱ(Mn/Un),  ∈nᐱ(Mn/Vn), ∈nᐱ(Mn/Wn), ∈nᐱ(Mn/Yn), ∈nᐱ(Mn/Zn), ∈nᐱ(Mnn), ∈nᐱ(Mnn),nᐱ(Mncn/ᐱncn), ∈nᐱ(Mncn/ᗑncn), ∈nᐱ(Mncn/∘⧊°ncn), ∈nᐱ(Mncn/∘∇°ncn)

nᐱ(Nn/An), ∈nᐱ(Nn/Bn), ∈nᐱ(Nn/Dn), ∈nᐱ(Nn/En), ∈nᐱ(Nn/Fn), ∈nᐱ(Nn/Gn), ∈nᐱ(Nn/Hn), ∈nᐱ(Nn/In), ∈nᐱ(Nn/Jn), ∈nᐱ(Nn/Kn), ∈nᐱ(Nn/Ln), ∈nᐱ(Nn/Mn), nᐱ(Nn/Nn), ∈nᐱ(Nn/On), ∈nᐱ(Nn/Pn), ∈nᐱ(Nn/Qn), ∈nᐱ(Nn/Rn), ∈nᐱ(Nn/Sn), ∈nᐱ(Nn/Tn),∈nᐱ(Nn/Un),  ∈nᐱ(Nn/Vn), ∈nᐱ(Nn/Wn), ∈nᐱ(Nn/Yn), ∈nᐱ(Nn/Zn), ∈nᐱ(Nnn), ∈nᐱ(Nnn),nᐱ(Nncn/ᐱncn), ∈nᐱ(Nncn/ᗑncn), ∈nᐱ(Nncn/∘⧊°ncn), ∈nᐱ(Nncn/∘∇°ncn)

nᐱ(On/An), ∈nᐱ(On/Bn), ∈nᐱ(On/Dn), ∈nᐱ(On/En), ∈nᐱ(On/Fn), ∈nᐱ(On/Gn), ∈nᐱ(On/Hn), ∈nᐱ(On/In), ∈nᐱ(On/Jn), ∈nᐱ(On/Kn), ∈nᐱ(On/Ln), ∈nᐱ(On/Mn), ∈nᐱ(On/Nn), nᐱ(On/On), ∈nᐱ(On/Pn), ∈nᐱ(On/Qn), ∈nᐱ(On/Rn), ∈nᐱ(On/Sn), ∈nᐱ(On/Tn),∈nᐱ(On/Un),  ∈nᐱ(On/Vn), ∈nᐱ(On/Wn), ∈nᐱ(On/Yn), ∈nᐱ(On/Zn), ∈nᐱ(Onn), ∈nᐱ(Onn),nᐱ(Oncn/ᐱncn), ∈nᐱ(Oncn/ᗑncn), ∈nᐱ(Oncn/∘⧊°ncn), ∈nᐱ(Oncn/∘∇°ncn)

nᐱ(Pn/An), ∈nᐱ(Pn/Bn), ∈nᐱ(Pn/Dn), ∈nᐱ(Pn/En), ∈nᐱ(Pn/Fn), ∈nᐱ(Pn/Gn), ∈nᐱ(Pn/Hn), ∈nᐱ(Pn/In), ∈nᐱ(Pn/Jn), ∈nᐱ(Pn/Kn), ∈nᐱ(Pn/Ln), ∈nᐱ(Pn/Mn), ∈nᐱ(Pn/Nn), ∈nᐱ(Pn/On), ∈nᐱ(Pn/Qn), ∈nᐱ(Pn/Rn), ∈nᐱ(Pn/Sn), ∈nᐱ(Pn/Tn),∈nᐱ(Pn/Un),  ∈nᐱ(Pn/Vn), ∈nᐱ(Pn/Wn), ∈nᐱ(Pn/Zn), ∈nᐱ(Pnn), ∈nᐱ(Pnn),nᐱ(Pncn/ᐱncn), ∈nᐱ(Pncn/ᗑncn), ∈nᐱ(Pncn/∘⧊°ncn), ∈nᐱ(Pncn/∘∇°ncn)

while path 3ncn is not applicable to whole number variables with no decimal stem repeating numerals of set variables nᐱ(Pn/Pn) and ∈nᐱ(Pn/Yn)

nᐱ(Qn/An), ∈nᐱ(Qn/Bn), ∈nᐱ(Qn/Dn), ∈nᐱ(Qn/En), ∈nᐱ(Qn/Fn), ∈nᐱ(Qn/Gn), ∈nᐱ(Qn/Hn), ∈nᐱ(Qn/In), ∈nᐱ(Qn/Jn), ∈nᐱ(Qn/Kn), ∈nᐱ(Qn/Ln), ∈nᐱ(Qn/Mn), ∈nᐱ(Qn/Nn), ∈nᐱ(Qn/On), ∈nᐱ(Qn/Pn), nᐱ(Qn/Qn), ∈nᐱ(Qn/Rn), ∈nᐱ(Qn/Sn), ∈nᐱ(Qn/Tn),∈nᐱ(Qn/Un),  ∈nᐱ(Qn/Vn), ∈nᐱ(Qn/Wn), ∈nᐱ(Qn/Yn), ∈nᐱ(Qn/Zn), ∈nᐱ(Qnn), ∈nᐱ(Qnn),nᐱ(Qncn/ᐱncn), ∈nᐱ(Qncn/ᗑncn), ∈nᐱ(Qncn/∘⧊°ncn), ∈nᐱ(Qncn/∘∇°ncn)

nᐱ(Rn/An), ∈nᐱ(Rn/Bn), ∈nᐱ(Rn/Dn), ∈nᐱ(Rn/En), ∈nᐱ(Rn/Fn), ∈nᐱ(Rn/Gn), ∈nᐱ(Rn/Hn), ∈nᐱ(Rn/In), ∈nᐱ(Rn/Jn), ∈nᐱ(Rn/Kn), ∈nᐱ(Rn/Ln), ∈nᐱ(Rn/Mn), ∈nᐱ(Rn/Nn), ∈nᐱ(Rn/On), ∈nᐱ(Rn/Pn), ∈nᐱ(Rn/Qn), nᐱ(Rn/Rn), ∈nᐱ(Rn/Sn), ∈nᐱ(Rn/Tn),∈nᐱ(Rn/Un),  ∈nᐱ(Rn/Vn), ∈nᐱ(Rn/Wn), ∈nᐱ(Rn/Yn), ∈nᐱ(Rn/Zn), ∈nᐱ(Rnn), ∈nᐱ(Rnn),nᐱ(Rncn/ᐱncn), ∈nᐱ(Rncn/ᗑncn), ∈nᐱ(Rncn/∘⧊°ncn), ∈nᐱ(Rncn/∘∇°ncn)

nᐱ(Sn/An), ∈nᐱ(Sn/Bn), ∈nᐱ(Sn/Dn), ∈nᐱ(Sn/En), ∈nᐱ(Sn/Fn), ∈nᐱ(Sn/Gn), ∈nᐱ(Sn/Hn), ∈nᐱ(Sn/In), ∈nᐱ(Sn/Jn), ∈nᐱ(Sn/Kn), ∈nᐱ(Sn/Ln), ∈nᐱ(Sn/Mn), ∈nᐱ(Sn/Nn), ∈nᐱ(Sn/On), ∈nᐱ(Sn/Pn), ∈nᐱ(Sn/Qn), ∈nᐱ(Sn/Rn), nᐱ(Sn/Sn), ∈nᐱ(Sn/Tn),∈nᐱ(Sn/Un),  ∈nᐱ(Sn/Vn), ∈nᐱ(Sn/Wn), ∈nᐱ(Sn/Yn), ∈nᐱ(Sn/Zn), ∈nᐱ(Snn), ∈nᐱ(Snn),nᐱ(Sncn/ᐱncn), ∈nᐱ(Sncn/ᗑncn), ∈nᐱ(Sncn/∘⧊°ncn), ∈nᐱ(Sncn/∘∇°ncn)

nᐱ(Tn/An), ∈nᐱ(Tn/Bn), ∈nᐱ(Tn/Dn), ∈nᐱ(Tn/En), ∈nᐱ(Tn/Fn), ∈nᐱ(Tn/Gn), ∈nᐱ(Tn/Hn), ∈nᐱ(Tn/In), ∈nᐱ(Tn/Jn), ∈nᐱ(Tn/Kn), ∈nᐱ(Tn/Ln), ∈nᐱ(Tn/Mn), ∈nᐱ(Tn/Nn), ∈nᐱ(Tn/On), ∈nᐱ(Tn/Pn), ∈nᐱ(Tn/Qn), ∈nᐱ(Tn/Rn), ∈nᐱ(Tn/Sn), nᐱ(Tn/Tn),∈nᐱ(Tn/Un),  ∈nᐱ(Tn/Vn), ∈nᐱ(Tn/Wn), ∈nᐱ(Tn/Yn), ∈nᐱ(Tn/Zn), ∈nᐱ(Tnn), ∈nᐱ(Tnn),nᐱ(Tncn/ᐱncn), ∈nᐱ(Tncn/ᗑncn), ∈nᐱ(Tncn/∘⧊°ncn), ∈nᐱ(Tncn/∘∇°ncn)

nᐱ(Un/An), ∈nᐱ(Un/Bn), ∈nᐱ(Un/Dn), ∈nᐱ(Un/En), ∈nᐱ(Un/Fn), ∈nᐱ(Un/Gn), ∈nᐱ(Un/Hn), ∈nᐱ(Un/In), ∈nᐱ(Un/Jn), ∈nᐱ(Un/Kn), ∈nᐱ(Un/Ln), ∈nᐱ(Un/Mn), ∈nᐱ(Un/Nn), ∈nᐱ(Un/On), ∈nᐱ(Un/Pn), ∈nᐱ(Un/Qn), ∈nᐱ(Un/Rn), ∈nᐱ(Un/Sn), ∈nᐱ(Un/Tn), nᐱ(Un/Un),  ∈nᐱ(Un/Vn), ∈nᐱ(Un/Wn), ∈nᐱ(Un/Yn), ∈nᐱ(Un/Zn), ∈nᐱ(Unn), ∈nᐱ(Unn),nᐱ(Uncn/ᐱncn), ∈nᐱ(Uncn/ᗑncn), ∈nᐱ(Uncn/∘⧊°ncn), ∈nᐱ(Uncn/∘∇°ncn)

nᐱ(Vn/An), ∈nᐱ(Vn/Bn), ∈nᐱ(Vn/Dn), ∈nᐱ(Vn/En), ∈nᐱ(Vn/Fn), ∈nᐱ(Vn/Gn), ∈nᐱ(Vn/Hn), ∈nᐱ(Vn/In), ∈nᐱ(Vn/Jn), ∈nᐱ(Vn/Kn), ∈nᐱ(Vn/Ln), ∈nᐱ(Vn/Mn), ∈nᐱ(Vn/Nn), ∈nᐱ(Vn/On), ∈nᐱ(Vn/Pn), ∈nᐱ(Vn/Qn), ∈nᐱ(Vn/Rn), ∈nᐱ(Vn/Sn), ∈nᐱ(Vn/Tn),∈nᐱ(Vn/Un),  nᐱ(Vn/Vn), ∈nᐱ(Vn/Wn), ∈nᐱ(Vn/Yn), ∈nᐱ(Vn/Zn), ∈nᐱ(Vnn), ∈nᐱ(Vnn),nᐱ(Vncn/ᐱncn), ∈nᐱ(Vncn/ᗑncn), ∈nᐱ(Vncn/∘⧊°ncn), ∈nᐱ(Vncn/∘∇°ncn)

nᐱ(Wn/An), ∈nᐱ(Wn/Bn), ∈nᐱ(Wn/Dn), ∈nᐱ(Wn/En), ∈nᐱ(Wn/Fn), ∈nᐱ(Wn/Gn), ∈nᐱ(Wn/Hn), ∈nᐱ(Wn/In), ∈nᐱ(Wn/Jn), ∈nᐱ(Wn/Kn), ∈nᐱ(Wn/Ln), ∈nᐱ(Wn/Mn), ∈nᐱ(Wn/Nn), ∈nᐱ(Wn/On), ∈nᐱ(Wn/Pn), ∈nᐱ(Wn/Qn), ∈nᐱ(Wn/Rn), ∈nᐱ(Wn/Sn), ∈nᐱ(Wn/Tn),∈nᐱ(Wn/Un),  ∈nᐱ(Wn/Vn), nᐱ(Wn/Wn), ∈nᐱ(Wn/Yn), ∈nᐱ(Wn/Zn), ∈nᐱ(Wnn), ∈nᐱ(Wnn),nᐱ(Wncn/ᐱncn), ∈nᐱ(Wncn/ᗑncn), ∈nᐱ(Wncn/∘⧊°ncn), ∈nᐱ(Wncn/∘∇°ncn)

nᐱ(Yn/An), ∈nᐱ(Yn/Bn), ∈nᐱ(Yn/Dn), ∈nᐱ(Yn/En), ∈nᐱ(Yn/Fn), ∈nᐱ(Yn/Gn), ∈nᐱ(Yn/Hn), ∈nᐱ(Yn/In), ∈nᐱ(Yn/Jn), ∈nᐱ(Yn/Kn), ∈nᐱ(Yn/Ln), ∈nᐱ(Yn/Mn), ∈nᐱ(Yn/Nn), ∈nᐱ(Yn/On), ∈nᐱ(Yn/Qn), ∈nᐱ(Yn/Rn), ∈nᐱ(Yn/Sn), ∈nᐱ(Yn/Tn),∈nᐱ(Yn/Un),  ∈nᐱ(Yn/Vn), ∈nᐱ(Yn/Wn), ∈nᐱ(Yn/Zn), ∈nᐱ(Ynn), ∈nᐱ(Ynn),nᐱ(Yncn/ᐱncn), ∈nᐱ(Yncn/ᗑncn), ∈nᐱ(Yncn/∘⧊°ncn), ∈nᐱ(Yncn/∘∇°ncn)

while path 3ncn is not applicable to whole number variables with no decimal stem repeating numerals of set variables nᐱ(Yn/Yn) and nᐱ(Yn/Pn)

nᐱ(Zn/An), ∈nᐱ(Zn/Bn), ∈nᐱ(Zn/Dn), ∈nᐱ(Zn/En), ∈nᐱ(Zn/Fn), ∈nᐱ(Zn/Gn), ∈nᐱ(Zn/Hn), ∈nᐱ(Zn/In), ∈nᐱ(Zn/Jn), ∈nᐱ(Zn/Kn), ∈nᐱ(Zn/Ln), ∈nᐱ(Zn/Mn), ∈nᐱ(Zn/Nn), ∈nᐱ(Zn/On), ∈nᐱ(Zn/Pn), ∈nᐱ(Zn/Qn), ∈nᐱ(Zn/Rn), ∈nᐱ(Zn/Sn), ∈nᐱ(Zn/Tn),∈nᐱ(Zn/Un),  ∈nᐱ(Zn/Vn), ∈nᐱ(Zn/Wn), ∈nᐱ(Zn/Yn), nᐱ(Zn/Zn), ∈nᐱ(Znn), ∈nᐱ(Znn),nᐱ(Zncn/ᐱncn), ∈nᐱ(Zncn/ᗑncn), ∈nᐱ(Zncn/∘⧊°ncn), ∈nᐱ(Zncn/∘∇°ncn)

nᐱ(φn/An), ∈nᐱ(φn/Bn), ∈nᐱ(φn/Dn), ∈nᐱ(φn/En), ∈nᐱ(φn/Fn), ∈nᐱ(φn/Gn), ∈nᐱ(φn/Hn), ∈nᐱ(φn/In), ∈nᐱ(φn/Jn), ∈nᐱ(φn/Kn), ∈nᐱ(φn/Ln), ∈nᐱ(φn/Mn), ∈nᐱ(φn/Nn), ∈nᐱ(φn/On), ∈nᐱ(φn/Pn), ∈nᐱ(φn/Qn), ∈nᐱ(φn/Rn), ∈nᐱ(φn/Sn), ∈nᐱ(φn/Tn),∈nᐱ(φn/Un),  ∈nᐱ(φn/Vn), ∈nᐱ(φn/Wn), ∈nᐱ(φn/Yn), ∈nᐱ(φn/Zn), nᐱ(φnn), ∈nᐱ(φnn),nᐱ(φncn/ᐱncn), ∈nᐱ(φncn/ᗑncn), ∈nᐱ(φncn/∘⧊°ncn), ∈nᐱ(φncn/∘∇°ncn)

nᐱ(Θn/An), ∈nᐱ(Θn/Bn), ∈nᐱ(Θn/Dn), ∈nᐱ(Θn/En), ∈nᐱ(Θn/Fn), ∈nᐱ(Θn/Gn), ∈nᐱ(Θn/Hn), ∈nᐱ(Θn/In), ∈nᐱ(Θn/Jn), ∈nᐱ(Θn/Kn), ∈nᐱ(Θn/Ln), ∈nᐱ(Θn/Mn), ∈nᐱ(Θn/Nn), ∈nᐱ(Θn/On), ∈nᐱ(Θn/Pn), ∈nᐱ(Θn/Qn), ∈nᐱ(Θn/Rn), ∈nᐱ(Θn/Sn), ∈nᐱ(Θn/Tn),∈nᐱ(Θn/Un),  ∈nᐱ(Θn/Vn), ∈nᐱ(Θn/Wn), ∈nᐱ(Θn/Yn), ∈nᐱ(Θn/Zn), ∈nᐱ(Θnn), nᐱ(Θnn), ∈nᐱ(Θncn/ᐱncn), ∈nᐱ(Θncn/ᗑncn), ∈nᐱ(Θncn/∘⧊°ncn), ∈nᐱ(Θncn/∘∇°ncn)


Example 1φn21 having 10 decimals that repeat 1.6^1803399852

32φ of (1φ21c1/1φ21c2)=(1.6^1803399852/1.6^18033998521803399852)

and 

32φ of (1φ21c1/1φ21c1.5)=(1.6^1803399852/1.6^180339985218033)


1X⅄=(n2xn1)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

⅄X=(nncnxnncn) that a function path is factored to the definition of the function path rather than pemdas order of operations.

Variables are factorable to a measured units that then be later can applied in functions of proper order of operations that is parenthesis, exponents, multiplication, division, addition, and then subtraction. 

Function path ⅄X=(nncnxnncn) is nncn multiplied by nncn such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant.

⅄XA examples

⅄XA multiplication complex function of Ancn variables

if A=∈1/Q)cn and path ⅄ of Q is a variant in the definition of A then 

A=1n2/Qn1)=[(Yn3/Yn2)/(P/P) while Q requires path definition of 1⅄Q or 2⅄Q from P two sets of A complete the formula of Q variable.

A=1n2/1Qn1)=[(Yn3/Yn2)/(Pn2/Pn1)=(1/1)/(3/2)=(1/1.5)=0.^6

and

A=1n2/2Qn1c1)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^6)=1.^6


Applied function of ⅄X=(nncnxnncn) with A variables is then

⅄Xᐱ of A1n2 x 1Qn1)=[(Yn3/Yn2) x (Pn2/Pn1)=(1x1.5)=1.5

and

⅄Xᐱ of A1n2 x 2Qn1c1)=[(Yn3/Yn2) x (Pn1/Pn2)=(1x0.^6)=0.6


Any change in cn stem decimal cycle count variable will change the multiple of the exponent squared value in the example and ultimately the final product value also.

For example ⅄Xᐱ of A1n2 x 2Qn1c2)=[(Yn3/Yn2) x (Pn1/Pn2)=(1x0.^66)=0.66


if A=∈1/Q) and ⅄X=(nncnxnncn) then n x 1Qn) ≠ n x 2Qn) ≠ (Ancn x Ancn)


Alternately rather than multiplying variables of A base φn x 1Qn and multiplying variables of A base φn x 2Qn factored variables of are Ancn multiplied in the function n⅄Xᐱ(AncnxAncn) and ∈n⅄Xᐱ represents notation of a complex function.

Then ⅄X=(nncnxnncn) function path applied to variables A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° with completed set A=∈1/Q)cn that are An1cn to Ancn

nᐱ(AncnxAncn), ∈nᐱ(AncnxBncn), ∈nᐱ(AncnxDncn), ∈nᐱ(AncnxEncn), ∈nᐱ(AncnxFncn), ∈nᐱ(AncnxGncn), ∈nᐱ(AncnxHncn), ∈nᐱ(AncnxIncn), ∈nᐱ(AncnxJncn), ∈nᐱ(AncnxKncn), ∈nᐱ(AncnxLncn), ∈nᐱ(AncnxMncn), ∈nᐱ(AncnxNncn), ∈nᐱ(AncnxOncn), ∈nᐱ(AncnxPn), ∈nᐱ(AncnxQncn), ∈nᐱ(AncnxRncn), ∈nᐱ(AncnxSncn), ∈nᐱ(AncnxTncn),∈nᐱ(AncnxUncn),  ∈nᐱ(AncnxVncn), ∈nᐱ(AncnxWncn), ∈nᐱ(AncnxYn), ∈nᐱ(AncnxZncn), ∈nᐱ(Ancnncn), ∈nᐱ(Ancnncn), ∈nᐱ(Ancnxᐱncn), ∈nᐱ(Ancnxᗑncn), ∈nᐱ(Ancnx∘⧊°ncn), ∈nᐱ(Ancnx∘∇°ncn)


nᐱ(AncnxAncn) example given variants of 1Qn1 and 2Qn1c1 ofAn1

if An1 of 1n2/1Qn1)=[(Yn3/Yn2)/(Pn2/Pn1)=(1/1)/(3/2)=(1/1.5)=0.^6

and

An1 of 1n2/2Qn1c1)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^6)=1.^6

while

An2 of 1n3/1Qn2)=[(Yn4/Yn3)/(Pn3/Pn2)=(3/2)/(5/3)=(1.5/1.^6)=0.9375

 and

An2 of 1n3/2Qn2)=[(Yn4/Yn3)/(Pn2/Pn3)=(3/2)/(3/5)=(1.5/0.6)=2.5


then

n⅄XA has an array of base sets to nᐱ(AncnxAncn) {0.^6, 0.9375, 1.^6, 2.5} for {1Qn1, 1Qn2, 2Qn1c1, 2Qn2} of An1 and An2


(1Qn1) variant of A is ⅄XAn1 [An1 of 1n2/1Qn1)] x [An2 of 1n3/1Qn2)]=(0.^6x0.9375)=0.5625

(2Qn1c1) variant of A is ⅄XAn1 [An1 of 1n2/2Qn1c1)] x [An2 of 1n3/2Qn2c1)]=(1.^6x2.5)=4


alternately a path multiplying variables of A with varying Q paths n⅄ is nᐱ(Ancn of 2Qn xAncn of 1Qn)

(1Qn1cn and 2Qn1cn) variant of A is ⅄XAn1 [An1 of 1n2/1Qn1)] x [An1 of 1n2/2Qn1)]=(0.^6x1.^6)=0.96


So multiplying variables 

n2 x 1Qn1) from ⅄Xᐱ of A1n2 x 1Qn1)=(1x1.5)=1.5 

and multiplying variables 

n2 x 2Qn1c1) from ⅄Xᐱ of A1n2 x 2Qn1c1)=(1x0.^6)=0.6 

and multiplying variables

n2 x 2Qn1c1) from ⅄Xᐱ of A1n2 x 2Qn1c2)=(1x0.^66)=0.66 

for 2Qn1c2 of 2Qn1cnc stem decimal variant of variable in ⅄Xᐱ of A1n2 x 2Qn1cn)


While multiplying variables 

An1 and An2 of 1n/1Qn)=(0.^6x0.9375)=0.5625

and multiplying variables

An1 and An2 of 1n/2Qn)=(1.^6x2.5)=4


While multiplying variables

An1 of 1n/1Qn) and An1 of 1n/2Qn)=(0.^6x1.^6)=0.96

and multiplying variables

An1 of 1n/1Qn) and An2 of 1n/2Qn)=(0.^6x2.5)=1.5

and multiplying variables

An1 of 1n/2Qn) and An2 of 1n/1Qn)=(1.^6x0.9375)=1.5


While multiplying variables An1c2 with change in cn of Ancn variables

An1c2 and An2 of 1n/1Qn)=(0.^66x0.9375)=0.61875

and multiplying variables

An1c2 and An2 of 1n/2Qn)=(1.^66x2.5)=4.15


and multiplying variables of An1cn change 

An1c2 of 1n/1Qn) and An1 of 1n/2Qn)=(0.^66x1.^6)=1.056

and multiplying variables of An1cn change 

An1 of 1n/1Qn) and An1c2 of 1n/2Qn)=(0.^6x1.^66)=0.996

and multiplying variables of An1cn change 

An1c2 of 1n/1Qn) and An1c2 of 1n/2Qn)=(0.^66x1.^66)=1.0956


if Qn2c2 is factored through

An2 of 1n3/1Qn2c2)=[(Yn4/Yn3)/(Pn3/Pn2)=(3/2)/(5/3)=(1.5/1.^66)=2.49

rather than 

An2 of 1n3/1Qn2)=[(Yn4/Yn3)/(Pn3/Pn2)=(3/2)/(5/3)=(1.5/1.^6)=0.9375

then a change in 1Qncn  applied to functions

An1 and An2 of 1n/1Qn)=(0.^6x0.9375)=0.5625 1Qnc1 to 1Qnc2 (0.^6x2.49)=1.494

An1 of 1n/2Qn) and An2 of 1n/1Qn)=(1.^6x0.9375)=1.5 1Qnc1 to 1Qnc2 (1.^6x2.49)=3.984

An1c2 and An2 of 1n/1Qn)=(0.^66x0.9375)=0.61875 1Qnc1 to 1Qnc2 (0.^66x2.49)=1.6434


And change in both 1Qnc1 to 1Qnc2 with variant An2 of 1n/1Qn)

An1c2 of 1n/2Qn) and An2 of 1n/1Qn)=(1.^66x2.49)=4.1334


It is not that these order of operations are incorrect by any means given the path and extent of the defined variables decimal stem cycles have potential change and limit to the variable definition at cn of the variants. 

The values are precise scale variables to the function of ƒ⅄XAn1cn of altered multiplication paths with variants Ancn and altered within the paths sub-units nQncn. These are multiplication products from ratios divided by ratios from variables of consecutive bases in y fibonacci and p prime variables. ƒ⅄Xᐱ represents complex path multiplication function of complex ratios.

Isolating a variable to a defined ratio numeral and then factoring with PEMDAS is one factoring path while other paths are not arranged to PEMDAS order of operations.


So then if variables of (A) are applicable to multiplication function ⅄X=(nncnxnncn) for new variables from set equations

n⅄X(AncnxAncn), n⅄X(AncnxBncn), n⅄X(AncnxDncn), n⅄X(AncnxEncn), n⅄X(AncnxFncn), n⅄X(AncnxGncn), n⅄X(AncnxHncn), n⅄X(AncnxIncn), n⅄X(AncnxJncn), n⅄X(AncnxKncn), n⅄X(AncnxLncn), n⅄X(AncnxMncn), n⅄X(AncnxNncn), n⅄X(AncnxOncn), n⅄X(AncnxPn), n⅄X(AncnxQncn), n⅄X(AncnxRncn), n⅄X(AncnxSncn), n⅄X(AncnxTncn), n⅄X(AncnxUncn),  n⅄X(AncnxVncn), n⅄X(AncnxWncn), n⅄X(AncnxYn), n⅄X(AncnxZncn), n⅄X(Ancnncn), n⅄X(Ancnncn), n⅄X(Ancnxᐱncn), n⅄X(Ancnxᗑncn), n⅄X(Ancnx∘⧊°ncn), n⅄X(Ancnx∘∇°ncn)


And ⅄X=(nncnxnncn) function is also applicable to example [Nncn of (AncnxNncn) x Nncn of (AncnxNncn)]=Nncn


Function ⅄X=(nncnxnncn) is applicable with variables from varying equation set variables such as

n⅄Xᐱ(AnxAn), ∈n⅄Xᐱ(AnxBn), ∈n⅄Xᐱ(AnxDn), ∈n⅄Xᐱ(AnxEn), ∈n⅄Xᐱ(AnxFn), ∈n⅄Xᐱ(AnxGn), ∈n⅄Xᐱ(AnxHn), ∈n⅄Xᐱ(AnxIn), ∈n⅄Xᐱ(AnxJn), ∈n⅄Xᐱ(AnxKn), ∈n⅄Xᐱ(AnxLn), ∈n⅄Xᐱ(AnxMn), ∈n⅄Xᐱ(AnxNn), ∈n⅄Xᐱ(AnxOn), ∈n⅄Xᐱ(AnxPn), ∈n⅄Xᐱ(AnxQn), ∈n⅄Xᐱ(AnxRn), ∈n⅄Xᐱ(AnxSn), ∈n⅄Xᐱ(AnxTn),∈n⅄Xᐱ(AnxUn),  ∈n⅄Xᐱ(AnxVn), ∈n⅄Xᐱ(AnxWn), ∈n⅄Xᐱ(AnxYn), ∈n⅄Xᐱ(AnxZn), ∈n⅄Xᐱ(Ann), ∈n⅄Xᐱ(Ann),n⅄Xᐱ(Ancnxᐱncn), ∈n⅄Xᐱ(Ancnxᗑncn), ∈n⅄Xᐱ(Ancnx∘⧊°ncn), ∈n⅄Xᐱ(Ancnx∘∇°ncn)


n⅄Xᐱ(BnxAn), n⅄Xᐱ(BnxBn), ∈n⅄Xᐱ(BnxDn), ∈n⅄Xᐱ(BnxEn), ∈n⅄Xᐱ(BnxFn), ∈n⅄Xᐱ(BnxGn), ∈n⅄Xᐱ(BnxHn), ∈n⅄Xᐱ(BnxIn), ∈n⅄Xᐱ(BnxJn), ∈n⅄Xᐱ(BnxKn), ∈n⅄Xᐱ(BnxLn), ∈n⅄Xᐱ(BnxMn), ∈n⅄Xᐱ(BnxNn), ∈n⅄Xᐱ(BnxOn), ∈n⅄Xᐱ(BnxPn), ∈n⅄Xᐱ(BnxQn), ∈n⅄Xᐱ(BnxRn), ∈n⅄Xᐱ(BnxSn), ∈n⅄Xᐱ(BnxTn),∈n⅄Xᐱ(BnxUn),  ∈n⅄Xᐱ(BnxVn), ∈n⅄Xᐱ(BnxWn), ∈n⅄Xᐱ(BnxYn), ∈n⅄Xᐱ(BnxZn), ∈n⅄Xᐱ(Bnn), ∈n⅄Xᐱ(Bnn),n⅄Xᐱ(Bncnxᐱncn), ∈n⅄Xᐱ(Bncnxᗑncn), ∈n⅄Xᐱ(Bncnx∘⧊°ncn), ∈n⅄Xᐱ(Bncnx∘∇°ncn)


n⅄Xᐱ(DnxAn), ∈n⅄Xᐱ(DnxBn), n⅄Xᐱ(DnxDn), ∈n⅄Xᐱ(DnxEn), ∈n⅄Xᐱ(DnxFn), ∈n⅄Xᐱ(DnxGn), ∈n⅄Xᐱ(DnxHn), ∈n⅄Xᐱ(DnxIn), ∈n⅄Xᐱ(DnxJn), ∈n⅄Xᐱ(DnxKn), ∈n⅄Xᐱ(DnxLn), ∈n⅄Xᐱ(DnxMn), ∈n⅄Xᐱ(DnxNn), ∈n⅄Xᐱ(DnxOn), ∈n⅄Xᐱ(DnxPn), ∈n⅄Xᐱ(DnxQn), ∈n⅄Xᐱ(DnxRn), ∈n⅄Xᐱ(DnxSn), ∈n⅄Xᐱ(DnxTn),∈n⅄Xᐱ(DnxUn),  ∈n⅄Xᐱ(DnxVn), ∈n⅄Xᐱ(DnxWn), ∈n⅄Xᐱ(DnxYn), ∈n⅄Xᐱ(DnxZn), ∈n⅄Xᐱ(Dnn), ∈n⅄Xᐱ(Dnn),n⅄Xᐱ(Dncnxᐱncn), ∈n⅄Xᐱ(Dncnxᗑncn), ∈n⅄Xᐱ(Dncnx∘⧊°ncn), ∈n⅄Xᐱ(Dncnx∘∇°ncn)


n⅄Xᐱ(EnxAn), ∈n⅄Xᐱ(EnxBn), ∈n⅄Xᐱ(EnxDn), n⅄Xᐱ(EnxEn), ∈n⅄Xᐱ(EnxFn), ∈n⅄Xᐱ(EnxGn), ∈n⅄Xᐱ(EnxHn), ∈n⅄Xᐱ(EnxIn), ∈n⅄Xᐱ(EnxJn), ∈n⅄Xᐱ(EnxKn), ∈n⅄Xᐱ(EnxLn), ∈n⅄Xᐱ(EnxMn), ∈n⅄Xᐱ(EnxNn), ∈n⅄Xᐱ(EnxOn), ∈n⅄Xᐱ(EnxPn), ∈n⅄Xᐱ(EnxQn), ∈n⅄Xᐱ(EnxRn), ∈n⅄Xᐱ(EnxSn), ∈n⅄Xᐱ(EnxTn),∈n⅄Xᐱ(EnxUn),  ∈n⅄Xᐱ(EnxVn), ∈n⅄Xᐱ(EnxWn), ∈n⅄Xᐱ(EnxYn), ∈n⅄Xᐱ(EnxZn), ∈n⅄Xᐱ(Enn), ∈n⅄Xᐱ(Enn),n⅄Xᐱ(Encnxᐱncn), ∈n⅄Xᐱ(Encnxᗑncn), ∈n⅄Xᐱ(Encnx∘⧊°ncn), ∈n⅄Xᐱ(Encnx∘∇°ncn)


n⅄Xᐱ(FnxAn), ∈n⅄Xᐱ(FnxBn), ∈n⅄Xᐱ(FnxDn), ∈n⅄Xᐱ(FnxEn), n⅄Xᐱ(FnxFn), ∈n⅄Xᐱ(FnxGn), ∈n⅄Xᐱ(FnxHn), ∈n⅄Xᐱ(FnxIn), ∈n⅄Xᐱ(FnxJn), ∈n⅄Xᐱ(FnxKn), ∈n⅄Xᐱ(FnxLn), ∈n⅄Xᐱ(FnxMn), ∈n⅄Xᐱ(FnxNn), ∈n⅄Xᐱ(FnxOn), ∈n⅄Xᐱ(FnxPn), ∈n⅄Xᐱ(FnxQn), ∈n⅄Xᐱ(FnxRn), ∈n⅄Xᐱ(FnxSn), ∈n⅄Xᐱ(FnxTn),∈n⅄Xᐱ(FnxUn),  ∈n⅄Xᐱ(FnxVn), ∈n⅄Xᐱ(FnxWn), ∈n⅄Xᐱ(FnxYn), ∈n⅄Xᐱ(FnxZn), ∈n⅄Xᐱ(Fnn), ∈n⅄Xᐱ(Fnn),n⅄Xᐱ(Fncnxᐱncn), ∈n⅄Xᐱ(Fncnxᗑncn), ∈n⅄Xᐱ(Fncnx∘⧊°ncn), ∈n⅄Xᐱ(Fncnx∘∇°ncn)


n⅄Xᐱ(GnxAn), ∈n⅄Xᐱ(GnxBn), ∈n⅄Xᐱ(GnxDn), ∈n⅄Xᐱ(GnxEn), ∈n⅄Xᐱ(GnxFn), n⅄Xᐱ(GnxGn), ∈n⅄Xᐱ(GnxHn), ∈n⅄Xᐱ(GnxIn), ∈n⅄Xᐱ(GnxJn), ∈n⅄Xᐱ(GnxKn), ∈n⅄Xᐱ(GnxLn), ∈n⅄Xᐱ(GnxMn), ∈n⅄Xᐱ(GnxNn), ∈n⅄Xᐱ(GnxOn), ∈n⅄Xᐱ(GnxPn), ∈n⅄Xᐱ(GnxQn), ∈n⅄Xᐱ(GnxRn), ∈n⅄Xᐱ(GnxSn), ∈n⅄Xᐱ(GnxTn),∈n⅄Xᐱ(GnxUn),  ∈n⅄Xᐱ(GnxVn), ∈n⅄Xᐱ(GnxWn), ∈n⅄Xᐱ(GnxYn), ∈n⅄Xᐱ(GnxZn), ∈n⅄Xᐱ(Gnn), ∈n⅄Xᐱ(Gnn),n⅄Xᐱ(Gncnxᐱncn), ∈n⅄Xᐱ(Gncnxᗑncn), ∈n⅄Xᐱ(Gncnx∘⧊°ncn), ∈n⅄Xᐱ(Gncnx∘∇°ncn)


n⅄Xᐱ(HnxAn), ∈n⅄Xᐱ(HnxBn), ∈n⅄Xᐱ(HnxDn), ∈n⅄Xᐱ(HnxEn), ∈n⅄Xᐱ(HnxFn), ∈n⅄Xᐱ(HnxGn), n⅄Xᐱ(HnxHn), ∈n⅄Xᐱ(HnxIn), ∈n⅄Xᐱ(HnxJn), ∈n⅄Xᐱ(HnxKn), ∈n⅄Xᐱ(HnxLn), ∈n⅄Xᐱ(HnxMn), ∈n⅄Xᐱ(HnxNn), ∈n⅄Xᐱ(HnxOn), ∈n⅄Xᐱ(HnxPn), ∈n⅄Xᐱ(HnxQn), ∈n⅄Xᐱ(HnxRn), ∈n⅄Xᐱ(HnxSn), ∈n⅄Xᐱ(HnxTn),∈n⅄Xᐱ(HnxUn),  ∈n⅄Xᐱ(HnxVn), ∈n⅄Xᐱ(HnxWn), ∈n⅄Xᐱ(HnxYn), ∈n⅄Xᐱ(HnxZn), ∈n⅄Xᐱ(Hnn), ∈n⅄Xᐱ(Hnn),n⅄Xᐱ(Hncnxᐱncn), ∈n⅄Xᐱ(Hncnxᗑncn), ∈n⅄Xᐱ(Hncnx∘⧊°ncn), ∈n⅄Xᐱ(Hncnx∘∇°ncn)


n⅄Xᐱ(InxAn), ∈n⅄Xᐱ(InxBn), ∈n⅄Xᐱ(InxDn), ∈n⅄Xᐱ(InxEn), ∈n⅄Xᐱ(InxFn), ∈n⅄Xᐱ(InxGn), ∈n⅄Xᐱ(InxHn), n⅄Xᐱ(InxIn), ∈n⅄Xᐱ(InxJn), ∈n⅄Xᐱ(InxKn), ∈n⅄Xᐱ(InxLn), ∈n⅄Xᐱ(InxMn), ∈n⅄Xᐱ(InxNn), ∈n⅄Xᐱ(InxOn), ∈n⅄Xᐱ(InxPn), ∈n⅄Xᐱ(InxQn), ∈n⅄Xᐱ(InxRn), ∈n⅄Xᐱ(InxSn), ∈n⅄Xᐱ(InxTn),∈n⅄Xᐱ(InxUn),  ∈n⅄Xᐱ(InxVn), ∈n⅄Xᐱ(InxWn), ∈n⅄Xᐱ(InxYn), ∈n⅄Xᐱ(InxZn), ∈n⅄Xᐱ(Inn), ∈n⅄Xᐱ(Inn),n⅄Xᐱ(Incnxᐱncn), ∈n⅄Xᐱ(Incnxᗑncn), ∈n⅄Xᐱ(Incnx∘⧊°ncn), ∈n⅄Xᐱ(Incnx∘∇°ncn)


n⅄Xᐱ(JnxAn), ∈n⅄Xᐱ(JnxBn), ∈n⅄Xᐱ(JnxDn), ∈n⅄Xᐱ(JnxEn), ∈n⅄Xᐱ(JnxFn), ∈n⅄Xᐱ(JnxGn), ∈n⅄Xᐱ(JnxHn), ∈n⅄Xᐱ(JnxIn), n⅄Xᐱ(JnxJn), ∈n⅄Xᐱ(JnxKn), ∈n⅄Xᐱ(JnxLn), ∈n⅄Xᐱ(JnxMn), ∈n⅄Xᐱ(JnxNn), ∈n⅄Xᐱ(JnxOn), ∈n⅄Xᐱ(JnxPn), ∈n⅄Xᐱ(JnxQn), ∈n⅄Xᐱ(JnxRn), ∈n⅄Xᐱ(JnxSn), ∈n⅄Xᐱ(JnxTn),∈n⅄Xᐱ(JnxUn),  ∈n⅄Xᐱ(JnxVn), ∈n⅄Xᐱ(JnxWn), ∈n⅄Xᐱ(JnxYn), ∈n⅄Xᐱ(JnxZn), ∈n⅄Xᐱ(Jnn), ∈n⅄Xᐱ(Jnn),n⅄Xᐱ(Jncnxᐱncn), ∈n⅄Xᐱ(Jncnxᗑncn), ∈n⅄Xᐱ(Jncnx∘⧊°ncn), ∈n⅄Xᐱ(Jncnx∘∇°ncn)


n⅄Xᐱ(KnxAn), ∈n⅄Xᐱ(KnxBn), ∈n⅄Xᐱ(KnxDn), ∈n⅄Xᐱ(KnxEn), ∈n⅄Xᐱ(KnxFn), ∈n⅄Xᐱ(KnxGn), ∈n⅄Xᐱ(KnxHn), ∈n⅄Xᐱ(KnxIn), ∈n⅄Xᐱ(KnxJn), n⅄Xᐱ(KnxKn), ∈n⅄Xᐱ(KnxLn), ∈n⅄Xᐱ(KnxMn), ∈n⅄Xᐱ(KnxNn), ∈n⅄Xᐱ(KnxOn), ∈n⅄Xᐱ(KnxPn), ∈n⅄Xᐱ(KnxQn), ∈n⅄Xᐱ(KnxRn), ∈n⅄Xᐱ(KnxSn), ∈n⅄Xᐱ(KnxTn),∈n⅄Xᐱ(KnxUn),  ∈n⅄Xᐱ(KnxVn), ∈n⅄Xᐱ(KnxWn), ∈n⅄Xᐱ(KnxYn), ∈n⅄Xᐱ(KnxZn), ∈n⅄Xᐱ(Knn), ∈n⅄Xᐱ(Knn),n⅄Xᐱ(Kncnxᐱncn), ∈n⅄Xᐱ(Kncnxᗑncn), ∈n⅄Xᐱ(Kncnx∘⧊°ncn), ∈n⅄Xᐱ(Kncnx∘∇°ncn)


n⅄Xᐱ(LnxAn), ∈n⅄Xᐱ(LnxBn), ∈n⅄Xᐱ(LnxDn), ∈n⅄Xᐱ(LnxEn), ∈n⅄Xᐱ(LnxFn), ∈n⅄Xᐱ(LnxGn), ∈n⅄Xᐱ(LnxHn), ∈n⅄Xᐱ(LnxIn), ∈n⅄Xᐱ(LnxJn), ∈n⅄Xᐱ(LnxKn), n⅄Xᐱ(LnxLn), ∈n⅄Xᐱ(LnxMn), ∈n⅄Xᐱ(LnxNn), ∈n⅄Xᐱ(LnxOn), ∈n⅄Xᐱ(LnxPn), ∈n⅄Xᐱ(LnxQn), ∈n⅄Xᐱ(LnxRn), ∈n⅄Xᐱ(LnxSn), ∈n⅄Xᐱ(LnxTn),∈n⅄Xᐱ(LnxUn),  ∈n⅄Xᐱ(LnxVn), ∈n⅄Xᐱ(LnxWn), ∈n⅄Xᐱ(LnxYn), ∈n⅄Xᐱ(LnxZn), ∈n⅄Xᐱ(Lnn), ∈n⅄Xᐱ(Lnn),n⅄Xᐱ(Lncnxᐱncn), ∈n⅄Xᐱ(Lncnxᗑncn), ∈n⅄Xᐱ(Lncnx∘⧊°ncn), ∈n⅄Xᐱ(Lncnx∘∇°ncn)


n⅄Xᐱ(MnxAn), ∈n⅄Xᐱ(MnxBn), ∈n⅄Xᐱ(MnxDn), ∈n⅄Xᐱ(MnxEn), ∈n⅄Xᐱ(MnxFn), ∈n⅄Xᐱ(MnxGn), ∈n⅄Xᐱ(MnxHn), ∈n⅄Xᐱ(MnxIn), ∈n⅄Xᐱ(MnxJn), ∈n⅄Xᐱ(MnxKn), ∈n⅄Xᐱ(MnxLn), n⅄Xᐱ(MnxMn), ∈n⅄Xᐱ(MnxNn), ∈n⅄Xᐱ(MnxOn), ∈n⅄Xᐱ(MnxPn), ∈n⅄Xᐱ(MnxQn), ∈n⅄Xᐱ(MnxRn), ∈n⅄Xᐱ(MnxSn), ∈n⅄Xᐱ(MnxTn),∈n⅄Xᐱ(MnxUn),  ∈n⅄Xᐱ(MnxVn), ∈n⅄Xᐱ(MnxWn), ∈n⅄Xᐱ(MnxYn), ∈n⅄Xᐱ(MnxZn), ∈n⅄Xᐱ(Mnn), ∈n⅄Xᐱ(Mnn),n⅄Xᐱ(Mncnxᐱncn), ∈n⅄Xᐱ(Mncnxᗑncn), ∈n⅄Xᐱ(Mncnx∘⧊°ncn), ∈n⅄Xᐱ(Mncnx∘∇°ncn)


n⅄Xᐱ(NnxAn), ∈n⅄Xᐱ(NnxBn), ∈n⅄Xᐱ(NnxDn), ∈n⅄Xᐱ(NnxEn), ∈n⅄Xᐱ(NnxFn), ∈n⅄Xᐱ(NnxGn), ∈n⅄Xᐱ(NnxHn), ∈n⅄Xᐱ(NnxIn), ∈n⅄Xᐱ(NnxJn), ∈n⅄Xᐱ(NnxKn), ∈n⅄Xᐱ(NnxLn), ∈n⅄Xᐱ(NnxMn), n⅄Xᐱ(NnxNn), ∈n⅄Xᐱ(NnxOn), ∈n⅄Xᐱ(NnxPn), ∈n⅄Xᐱ(NnxQn), ∈n⅄Xᐱ(NnxRn), ∈n⅄Xᐱ(NnxSn), ∈n⅄Xᐱ(NnxTn),∈n⅄Xᐱ(NnxUn),  ∈n⅄Xᐱ(NnxVn), ∈n⅄Xᐱ(NnxWn), ∈n⅄Xᐱ(NnxYn), ∈n⅄Xᐱ(NnxZn), ∈n⅄Xᐱ(Nnn), ∈n⅄Xᐱ(Nnn),n⅄Xᐱ(Nncnxᐱncn), ∈n⅄Xᐱ(Nncnxᗑncn), ∈n⅄Xᐱ(Nncnx∘⧊°ncn), ∈n⅄Xᐱ(Nncnx∘∇°ncn)


n⅄Xᐱ(OnxAn), ∈n⅄Xᐱ(OnxBn), ∈n⅄Xᐱ(OnxDn), ∈n⅄Xᐱ(OnxEn), ∈n⅄Xᐱ(OnxFn), ∈n⅄Xᐱ(OnxGn), ∈n⅄Xᐱ(OnxHn), ∈n⅄Xᐱ(OnxIn), ∈n⅄Xᐱ(OnxJn), ∈n⅄Xᐱ(OnxKn), ∈n⅄Xᐱ(OnxLn), ∈n⅄Xᐱ(OnxMn), ∈n⅄Xᐱ(OnxNn), n⅄Xᐱ(OnxOn), ∈n⅄Xᐱ(OnxPn), ∈n⅄Xᐱ(OnxQn), ∈n⅄Xᐱ(OnxRn), ∈n⅄Xᐱ(OnxSn), ∈n⅄Xᐱ(OnxTn),∈n⅄Xᐱ(OnxUn),  ∈n⅄Xᐱ(OnxVn), ∈n⅄Xᐱ(OnxWn), ∈n⅄Xᐱ(OnxYn), ∈n⅄Xᐱ(OnxZn), ∈n⅄Xᐱ(Onn), ∈n⅄Xᐱ(Onn),n⅄Xᐱ(Oncnxᐱncn), ∈n⅄Xᐱ(Oncnxᗑncn), ∈n⅄Xᐱ(Oncnx∘⧊°ncn), ∈n⅄Xᐱ(Oncnx∘∇°ncn)


n⅄Xᐱ(PnxAn), ∈n⅄Xᐱ(PnxBn), ∈n⅄Xᐱ(PnxDn), ∈n⅄Xᐱ(PnxEn), ∈n⅄Xᐱ(PnxFn), ∈n⅄Xᐱ(PnxGn), ∈n⅄Xᐱ(PnxHn), ∈n⅄Xᐱ(PnxIn), ∈n⅄Xᐱ(PnxJn), ∈n⅄Xᐱ(PnxKn), ∈n⅄Xᐱ(PnxLn), ∈n⅄Xᐱ(PnxMn), ∈n⅄Xᐱ(PnxNn), ∈n⅄Xᐱ(PnxOn), n⅄Xᐱ(PnxPn), ∈n⅄Xᐱ(PnxQn), ∈n⅄Xᐱ(PnxRn), ∈n⅄Xᐱ(PnxSn), ∈n⅄Xᐱ(PnxTn),∈n⅄Xᐱ(PnxUn),  ∈n⅄Xᐱ(PnxVn), ∈n⅄Xᐱ(PnxWn), ∈n⅄Xᐱ(PnxYn), ∈n⅄Xᐱ(PnxZn), ∈n⅄Xᐱ(Pnn), ∈n⅄Xᐱ(Pnn),n⅄Xᐱ(Pncnxᐱncn), ∈n⅄Xᐱ(Pncnxᗑncn), ∈n⅄Xᐱ(Pncnx∘⧊°ncn), ∈n⅄Xᐱ(Pncnx∘∇°ncn)


n⅄Xᐱ(QnxAn), ∈n⅄Xᐱ(QnxBn), ∈n⅄Xᐱ(QnxDn), ∈n⅄Xᐱ(QnxEn), ∈n⅄Xᐱ(QnxFn), ∈n⅄Xᐱ(QnxGn), ∈n⅄Xᐱ(QnxHn), ∈n⅄Xᐱ(QnxIn), ∈n⅄Xᐱ(QnxJn), ∈n⅄Xᐱ(QnxKn), ∈n⅄Xᐱ(QnxLn), ∈n⅄Xᐱ(QnxMn), ∈n⅄Xᐱ(QnxNn), ∈n⅄Xᐱ(QnxOn), ∈n⅄Xᐱ(QnxPn), n⅄Xᐱ(QnxQn), ∈n⅄Xᐱ(QnxRn), ∈n⅄Xᐱ(QnxSn), ∈n⅄Xᐱ(QnxTn),∈n⅄Xᐱ(QnxUn),  ∈n⅄Xᐱ(QnxVn), ∈n⅄Xᐱ(QnxWn), ∈n⅄Xᐱ(QnxYn), ∈n⅄Xᐱ(QnxZn), ∈n⅄Xᐱ(Qnn), ∈n⅄Xᐱ(Qnn),n⅄Xᐱ(Qncnxᐱncn), ∈n⅄Xᐱ(Qncnxᗑncn), ∈n⅄Xᐱ(Qncnx∘⧊°ncn), ∈n⅄Xᐱ(Qncnx∘∇°ncn)


n⅄Xᐱ(RnxAn), ∈n⅄Xᐱ(RnxBn), ∈n⅄Xᐱ(RnxDn), ∈n⅄Xᐱ(RnxEn), ∈n⅄Xᐱ(RnxFn), ∈n⅄Xᐱ(RnxGn), ∈n⅄Xᐱ(RnxHn), ∈n⅄Xᐱ(RnxIn), ∈n⅄Xᐱ(RnxJn), ∈n⅄Xᐱ(RnxKn), ∈n⅄Xᐱ(RnxLn), ∈n⅄Xᐱ(RnxMn), ∈n⅄Xᐱ(RnxNn), ∈n⅄Xᐱ(RnxOn), ∈n⅄Xᐱ(RnxPn), ∈n⅄Xᐱ(RnxQn), n⅄Xᐱ(RnxRn), ∈n⅄Xᐱ(RnxSn), ∈n⅄Xᐱ(RnxTn),∈n⅄Xᐱ(RnxUn),  ∈n⅄Xᐱ(RnxVn), ∈n⅄Xᐱ(RnxWn), ∈n⅄Xᐱ(RnxYn), ∈n⅄Xᐱ(RnxZn), ∈n⅄Xᐱ(Rnn), ∈n⅄Xᐱ(Rnn),n⅄Xᐱ(Rncnxᐱncn), ∈n⅄Xᐱ(Rncnxᗑncn), ∈n⅄Xᐱ(Rncnx∘⧊°ncn), ∈n⅄Xᐱ(Rncnx∘∇°ncn)


n⅄Xᐱ(SnxAn), ∈n⅄Xᐱ(SnxBn), ∈n⅄Xᐱ(SnxDn), ∈n⅄Xᐱ(SnxEn), ∈n⅄Xᐱ(SnxFn), ∈n⅄Xᐱ(SnxGn), ∈n⅄Xᐱ(SnxHn), ∈n⅄Xᐱ(SnxIn), ∈n⅄Xᐱ(SnxJn), ∈n⅄Xᐱ(SnxKn), ∈n⅄Xᐱ(SnxLn), ∈n⅄Xᐱ(SnxMn), ∈n⅄Xᐱ(SnxNn), ∈n⅄Xᐱ(SnxOn), ∈n⅄Xᐱ(SnxPn), ∈n⅄Xᐱ(SnxQn), ∈n⅄Xᐱ(SnxRn), n⅄Xᐱ(SnxSn), ∈n⅄Xᐱ(SnxTn),∈n⅄Xᐱ(SnxUn),  ∈n⅄Xᐱ(SnxVn), ∈n⅄Xᐱ(SnxWn), ∈n⅄Xᐱ(SnxYn), ∈n⅄Xᐱ(SnxZn), ∈n⅄Xᐱ(Snn), ∈n⅄Xᐱ(Snn),n⅄Xᐱ(Sncnxᐱncn), ∈n⅄Xᐱ(Sncnxᗑncn), ∈n⅄Xᐱ(Sncnx∘⧊°ncn), ∈n⅄Xᐱ(Sncnx∘∇°ncn)


n⅄Xᐱ(TnxAn), ∈n⅄Xᐱ(TnxBn), ∈n⅄Xᐱ(TnxDn), ∈n⅄Xᐱ(TnxEn), ∈n⅄Xᐱ(TnxFn), ∈n⅄Xᐱ(TnxGn), ∈n⅄Xᐱ(TnxHn), ∈n⅄Xᐱ(TnxIn), ∈n⅄Xᐱ(TnxJn), ∈n⅄Xᐱ(TnxKn), ∈n⅄Xᐱ(TnxLn), ∈n⅄Xᐱ(TnxMn), ∈n⅄Xᐱ(TnxNn), ∈n⅄Xᐱ(TnxOn), ∈n⅄Xᐱ(TnxPn), ∈n⅄Xᐱ(TnxQn), ∈n⅄Xᐱ(TnxRn), ∈n⅄Xᐱ(TnxSn), n⅄Xᐱ(TnxTn),∈n⅄Xᐱ(TnxUn),  ∈n⅄Xᐱ(TnxVn), ∈n⅄Xᐱ(TnxWn), ∈n⅄Xᐱ(TnxYn), ∈n⅄Xᐱ(TnxZn), ∈n⅄Xᐱ(Tnn), ∈n⅄Xᐱ(Tnn),n⅄Xᐱ(Tncnxᐱncn), ∈n⅄Xᐱ(Tncnxᗑncn), ∈n⅄Xᐱ(Tncnx∘⧊°ncn), ∈n⅄Xᐱ(Tncnx∘∇°ncn)


n⅄Xᐱ(UnxAn), ∈n⅄Xᐱ(UnxBn), ∈n⅄Xᐱ(UnxDn), ∈n⅄Xᐱ(UnxEn), ∈n⅄Xᐱ(UnxFn), ∈n⅄Xᐱ(UnxGn), ∈n⅄Xᐱ(UnxHn), ∈n⅄Xᐱ(UnxIn), ∈n⅄Xᐱ(UnxJn), ∈n⅄Xᐱ(UnxKn), ∈n⅄Xᐱ(UnxLn), ∈n⅄Xᐱ(UnxMn), ∈n⅄Xᐱ(UnxNn), ∈n⅄Xᐱ(UnxOn), ∈n⅄Xᐱ(UnxPn), ∈n⅄Xᐱ(UnxQn), ∈n⅄Xᐱ(UnxRn), ∈n⅄Xᐱ(UnxSn), ∈n⅄Xᐱ(UnxTn), n⅄Xᐱ(UnxUn),  ∈n⅄Xᐱ(UnxVn), ∈n⅄Xᐱ(UnxWn), ∈n⅄Xᐱ(UnxYn), ∈n⅄Xᐱ(UnxZn), ∈n⅄Xᐱ(Unn), ∈n⅄Xᐱ(Unn),n⅄Xᐱ(Uncnxᐱncn), ∈n⅄Xᐱ(Uncnxᗑncn), ∈n⅄Xᐱ(Uncnx∘⧊°ncn), ∈n⅄Xᐱ(Uncnx∘∇°ncn)


n⅄Xᐱ(VnxAn), ∈n⅄Xᐱ(VnxBn), ∈n⅄Xᐱ(VnxDn), ∈n⅄Xᐱ(VnxEn), ∈n⅄Xᐱ(VnxFn), ∈n⅄Xᐱ(VnxGn), ∈n⅄Xᐱ(VnxHn), ∈n⅄Xᐱ(VnxIn), ∈n⅄Xᐱ(VnxJn), ∈n⅄Xᐱ(VnxKn), ∈n⅄Xᐱ(VnxLn), ∈n⅄Xᐱ(VnxMn), ∈n⅄Xᐱ(VnxNn), ∈n⅄Xᐱ(VnxOn), ∈n⅄Xᐱ(VnxPn), ∈n⅄Xᐱ(VnxQn), ∈n⅄Xᐱ(VnxRn), ∈n⅄Xᐱ(VnxSn), ∈n⅄Xᐱ(VnxTn),∈n⅄Xᐱ(VnxUn),  n⅄Xᐱ(VnxVn), ∈n⅄Xᐱ(VnxWn), ∈n⅄Xᐱ(VnxYn), ∈n⅄Xᐱ(VnxZn), ∈n⅄Xᐱ(Vnn), ∈n⅄Xᐱ(Vnn),n⅄Xᐱ(Vncnxᐱncn), ∈n⅄Xᐱ(Vncnxᗑncn), ∈n⅄Xᐱ(Vncnx∘⧊°ncn), ∈n⅄Xᐱ(Vncnx∘∇°ncn)


n⅄Xᐱ(WnxAn), ∈n⅄Xᐱ(WnxBn), ∈n⅄Xᐱ(WnxDn), ∈n⅄Xᐱ(WnxEn), ∈n⅄Xᐱ(WnxFn), ∈n⅄Xᐱ(WnxGn), ∈n⅄Xᐱ(WnxHn), ∈n⅄Xᐱ(WnxIn), ∈n⅄Xᐱ(WnxJn), ∈n⅄Xᐱ(WnxKn), ∈n⅄Xᐱ(WnxLn), ∈n⅄Xᐱ(WnxMn), ∈n⅄Xᐱ(WnxNn), ∈n⅄Xᐱ(WnxOn), ∈n⅄Xᐱ(WnxPn), ∈n⅄Xᐱ(WnxQn), ∈n⅄Xᐱ(WnxRn), ∈n⅄Xᐱ(WnxSn), ∈n⅄Xᐱ(WnxTn),∈n⅄Xᐱ(WnxUn),  ∈n⅄Xᐱ(WnxVn), n⅄Xᐱ(WnxWn), ∈n⅄Xᐱ(WnxYn), ∈n⅄Xᐱ(WnxZn), ∈n⅄Xᐱ(Wnn), ∈n⅄Xᐱ(Wnn),n⅄Xᐱ(Wncnxᐱncn), ∈n⅄Xᐱ(Wncnxᗑncn), ∈n⅄Xᐱ(Wncnx∘⧊°ncn), ∈n⅄Xᐱ(Wncnx∘∇°ncn)


n⅄Xᐱ(YnxAn), ∈n⅄Xᐱ(YnxBn), ∈n⅄Xᐱ(YnxDn), ∈n⅄Xᐱ(YnxEn), ∈n⅄Xᐱ(YnxFn), ∈n⅄Xᐱ(YnxGn), ∈n⅄Xᐱ(YnxHn), ∈n⅄Xᐱ(YnxIn), ∈n⅄Xᐱ(YnxJn), ∈n⅄Xᐱ(YnxKn), ∈n⅄Xᐱ(YnxLn), ∈n⅄Xᐱ(YnxMn), ∈n⅄Xᐱ(YnxNn), ∈n⅄Xᐱ(YnxOn), ∈n⅄Xᐱ(YnxPn), ∈n⅄Xᐱ(YnxQn), ∈n⅄Xᐱ(YnxRn), ∈n⅄Xᐱ(YnxSn), ∈n⅄Xᐱ(YnxTn),∈n⅄Xᐱ(YnxUn),  ∈n⅄Xᐱ(YnxVn), ∈n⅄Xᐱ(YnxWn), n⅄Xᐱ(YnxYn), ∈n⅄Xᐱ(YnxZn), ∈n⅄Xᐱ(Ynn), ∈n⅄Xᐱ(Ynn),n⅄Xᐱ(Yncnxᐱncn), ∈n⅄Xᐱ(Yncnxᗑncn), ∈n⅄Xᐱ(Yncnx∘⧊°ncn), ∈n⅄Xᐱ(Yncnx∘∇°ncn)


n⅄Xᐱ(ZnxAn), ∈n⅄Xᐱ(ZnxBn), ∈n⅄Xᐱ(ZnxDn), ∈n⅄Xᐱ(ZnxEn), ∈n⅄Xᐱ(ZnxFn), ∈n⅄Xᐱ(ZnxGn), ∈n⅄Xᐱ(ZnxHn), ∈n⅄Xᐱ(ZnxIn), ∈n⅄Xᐱ(ZnxJn), ∈n⅄Xᐱ(ZnxKn), ∈n⅄Xᐱ(ZnxLn), ∈n⅄Xᐱ(ZnxMn), ∈n⅄Xᐱ(ZnxNn), ∈n⅄Xᐱ(ZnxOn), ∈n⅄Xᐱ(ZnxPn), ∈n⅄Xᐱ(ZnxQn), ∈n⅄Xᐱ(ZnxRn), ∈n⅄Xᐱ(ZnxSn), ∈n⅄Xᐱ(ZnxTn),∈n⅄Xᐱ(ZnxUn),  ∈n⅄Xᐱ(ZnxVn), ∈n⅄Xᐱ(ZnxWn), ∈n⅄Xᐱ(ZnxYn), n⅄Xᐱ(ZnxZn), ∈n⅄Xᐱ(Znn), ∈n⅄Xᐱ(Znn),n⅄Xᐱ(Zncnxᐱncn), ∈n⅄Xᐱ(Zncnxᗑncn), ∈n⅄Xᐱ(Zncnx∘⧊°ncn), ∈n⅄Xᐱ(Zncnx∘∇°ncn)


n⅄Xᐱ(φnxAn), ∈n⅄Xᐱ(φnxBn), ∈n⅄Xᐱ(φnxDn), ∈n⅄Xᐱ(φnxEn), ∈n⅄Xᐱ(φnxFn), ∈n⅄Xᐱ(φnxGn), ∈n⅄Xᐱ(φnxHn), ∈n⅄Xᐱ(φnxIn), ∈n⅄Xᐱ(φnxJn), ∈n⅄Xᐱ(φnxKn), ∈n⅄Xᐱ(φnxLn), ∈n⅄Xᐱ(φnxMn), ∈n⅄Xᐱ(φnxNn), ∈n⅄Xᐱ(φnxOn), ∈n⅄Xᐱ(φnxPn), ∈n⅄Xᐱ(φnxQn), ∈n⅄Xᐱ(φnxRn), ∈n⅄Xᐱ(φnxSn), ∈n⅄Xᐱ(φnxTn),∈n⅄Xᐱ(φnxUn),  ∈n⅄Xᐱ(φnxVn), ∈n⅄Xᐱ(φnxWn), ∈n⅄Xᐱ(φnxYn), ∈n⅄Xᐱ(φnxZn), n⅄Xᐱ(φnn), ∈n⅄Xᐱ(φnn),n⅄Xᐱ(φncnxᐱncn), ∈n⅄Xᐱ(φncnxᗑncn), ∈n⅄Xᐱ(φncnx∘⧊°ncn), ∈n⅄Xᐱ(φncnx∘∇°ncn)


n⅄Xᐱ(ΘnxAn), ∈n⅄Xᐱ(ΘnxBn), ∈n⅄Xᐱ(ΘnxDn), ∈n⅄Xᐱ(ΘnxEn), ∈n⅄Xᐱ(ΘnxFn), ∈n⅄Xᐱ(ΘnxGn), ∈n⅄Xᐱ(ΘnxHn), ∈n⅄Xᐱ(ΘnxIn), ∈n⅄Xᐱ(ΘnxJn), ∈n⅄Xᐱ(ΘnxKn), ∈n⅄Xᐱ(ΘnxLn), ∈n⅄Xᐱ(ΘnxMn), ∈n⅄Xᐱ(ΘnxNn), ∈n⅄Xᐱ(ΘnxOn), ∈n⅄Xᐱ(ΘnxPn), ∈n⅄Xᐱ(ΘnxQn), ∈n⅄Xᐱ(ΘnxRn), ∈n⅄Xᐱ(ΘnxSn), ∈n⅄Xᐱ(ΘnxTn),∈n⅄Xᐱ(ΘnxUn),  ∈n⅄Xᐱ(ΘnxVn), ∈n⅄Xᐱ(ΘnxWn), ∈n⅄Xᐱ(ΘnxYn), ∈n⅄Xᐱ(ΘnxZn), ∈n⅄Xᐱ(Θnn), n⅄Xᐱ(Θnn), ∈n⅄Xᐱ(Θncnxᐱncn), ∈n⅄Xᐱ(Θncnxᗑncn), ∈n⅄Xᐱ(Θncnx∘⧊°ncn), ∈n⅄Xᐱ(Θncnx∘∇°ncn)


+⅄=(n2+n1)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

+⅄=(nncn+nncn) that a function path is factored to the definition of the function path rather than pemdas order of operations.

Variables are factorable to a measured units that then be later can applied in functions of proper order of operations that is parenthesis, exponents, multiplication, division, addition, and then subtraction. 

Function path +⅄=(nncn+nncn) is nncn a number or variable with a repeating or not repeating decimal stem cycle variant added with nncn another a number or variable with a repeating or not repeating decimal stem cycle variant.

⅄+⅄A examples

+⅄A multiplication complex function of Ancn variables

if A=∈1/Q)cn and path ⅄ of Q is a variant in the definition of A then 

A=1n2/Qn1)=[(Yn3/Yn2)/(P/P) while Q requires path definition of 1⅄Q or 2⅄Q from P two sets of A complete the formula of Q variable.

A=1n2/1Qn1)=[(Yn3/Yn2)/(Pn2/Pn1)=(1/1)/(3/2)=(1/1.5)=0.^6

and

A=1n2/2Qn1c1)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^6)=1.^6


Applied function of +⅄=(nncn+nncn) with A variables is then

+⅄ᐱ of A1n2 + 1Qn1)=[(Yn3/Yn2) + (Pn2/Pn1)=(1+1.5)=2.5

and

+⅄ᐱ of A1n2 + 2Qn1c1)=[(Yn3/Yn2) + (Pn1/Pn2)=(1+0.^6)=1.6


Any change in cn stem decimal cycle count variable will change the added in the example and ultimately the final sum value also.

For example +⅄ᐱ of A1n2 + 2Qn1c2)=[(Yn3/Yn2) + (Pn1/Pn2)=(1+0.^66)=1.66


if A=∈1/Q) and +⅄=(nncn+nncn) then n + 1Qn) ≠ n + 2Qn) ≠ (Ancn + Ancn)


Alternately rather than adding variables of A base φn + 1Qn and adding variables of A base φn + 2Qn factored variables of are Ancn added in the function n+⅄ᐱ(Ancn+Ancn) and ∈n+⅄ᐱ represents notation of a complex function.

Then +⅄=(nncn+nncn) function path applied to variables A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° with completed set A=∈1/Q)cn that are An1cn to Ancn

n+⅄ᐱ(Ancn+Ancn), ∈n+⅄ᐱ(Ancn+Bncn), ∈n+⅄ᐱ(Ancn+Dncn), ∈n+⅄ᐱ(Ancn+Encn), ∈n+⅄ᐱ(Ancn+Fncn), ∈n+⅄ᐱ(Ancn+Gncn), ∈n+⅄ᐱ(Ancn+Hncn), ∈n+⅄ᐱ(Ancn+Incn), ∈n+⅄ᐱ(Ancn+Jncn), ∈n+⅄ᐱ(Ancn+Kncn), ∈n+⅄ᐱ(Ancn+Lncn), ∈n+⅄ᐱ(Ancn+Mncn), ∈n+⅄ᐱ(Ancn+Nncn), ∈n+⅄ᐱ(Ancn+Oncn), ∈n+⅄ᐱ(Ancn+Pn), ∈n+⅄ᐱ(Ancn+Qncn), ∈n+⅄ᐱ(Ancn+Rncn), ∈n+⅄ᐱ(Ancn+Sncn), ∈n+⅄ᐱ(Ancn+Tncn), ∈n+⅄ᐱ(Ancn+Uncn),  ∈n+⅄ᐱ(Ancn+Vncn), ∈n+⅄ᐱ(Ancn+Wncn), ∈n+⅄ᐱ(Ancn+Yn), ∈n+⅄ᐱ(Ancn+Zncn), ∈n+⅄ᐱ(Ancnncn), ∈n+⅄ᐱ(Ancnncn), ∈n+⅄ᐱ(Ancn+ᐱncn), ∈n+⅄ᐱ(Ancn+ᗑncn), ∈n+⅄ᐱ(Ancn+∘⧊°ncn), ∈n+⅄ᐱ(Ancn+∘∇°ncn)


n+⅄ᐱ(Ancn+Ancn) example given variants of 1Qn1 and 2Qn1c1 ofAn1

if An1 of 1n2/1Qn1)=[(Yn3/Yn2)/(Pn2/Pn1)=(1/1)/(3/2)=(1/1.5)=0.^6

and

An1 of 1n2/2Qn1c1)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^6)=1.^6

while

An2 of 1n3/1Qn2)=[(Yn4/Yn3)/(Pn3/Pn2)=(3/2)/(5/3)=(1.5/1.^6)=0.9375

 and

An2 of 1n3/2Qn2)=[(Yn4/Yn3)/(Pn2/Pn3)=(3/2)/(3/5)=(1.5/0.6)=2.5


then

n+⅄A has an array of base sets to n+⅄ᐱ(Ancn+Ancn


(1Qn1) variant of A is +⅄An1 [An1 of 1n2/1Qn1)] + [An2 of 1n3/1Qn2)]=(0.^6+0.9375)=1.5375

(2Qn1c1) variant of A is +⅄An1 [An1 of 1n2/2Qn1c1)] + [An2 of 1n3/2Qn2c1)]=(1.^6+2.5)=4.1


alternately a path adding variables of A with varying Q paths n⅄ is nᐱ(Ancn of 2Qn xAncn of 1Qn)

(1Qn1cn and 2Qn1cn) variant of A is +⅄An1 [An1 of 1n2/1Qn1)] + [An1 of 1n2/2Qn1)]=(0.^6+1.^6)=2.2


So adding variables 

n2 x 1Qn1) from +⅄ᐱ of A1n2 + 1Qn1)=(1+1.5)=2.5 

and adding variables 

n2 x 2Qn1c1) from +⅄ᐱ of A1n2 + 2Qn1c1)=(1+0.^6)=1.6 

and adding variables

n2 x 2Qn1c1) from +⅄ᐱ of A1n2 + 2Qn1c2)=(1+0.^66)=1.66 

for 2Qn1c2 of 2Qn1cnc stem decimal variant of variable in +⅄ᐱ of A1n2 + 2Qn1cn)


While adding variables 

An1 and An2 of 1n/1Qn)=(0.^6+0.9375)=1.5375

and adding variables

An1 and An2 of 1n/2Qn)=(1.^6+2.5)=4.1


While adding variables

An1 of 1n/1Qn) and An1 of 1n/2Qn)=(0.^6+1.^6)=2.2

and adding variables

An1 of 1n/1Qn) and An2 of 1n/2Qn)=(0.^6+2.5)=3.1

and adding variables

An1 of 1n/2Qn) and An2 of 1n/1Qn)=(1.^6+0.9375)=2.5375


While adding variables An1c2 with change in cn of Ancn variables

An1c2 and An2 of 1n/1Qn)=(0.^66+0.9375)=1.5975

and adding variables

An1c2 and An2 of 1n/2Qn)=(1.^66+2.5)=4.16


and adding variables of An1cn change 

An1c2 of 1n/1Qn) and An1 of 1n/2Qn)=(0.^66+1.^6)=2.26

and adding variables of An1cn change 

An1 of 1n/1Qn) and An1c2 of 1n/2Qn)=(0.^6+1.^66)=2.26

and adding variables of An1cn change 

An1c2 of 1n/1Qn) and An1c2 of 1n/2Qn)=(0.^66+1.^66)=2.32


if Qn2c2 is factored through

An2 of 1n3/1Qn2c2)=[(Yn4/Yn3)/(Pn3/Pn2)=(3/2)/(5/3)=(1.5/1.^66)=2.49

rather than 

An2 of 1n3/1Qn2)=[(Yn4/Yn3)/(Pn3/Pn2)=(3/2)/(5/3)=(1.5/1.^6)=0.9375

then a change in 1Qncn  applied to functions

An1 and An2 of 1n/1Qn)=(0.^6+0.9375)=1.5375 1Qnc1 to 1Qnc2 (0.^6+2.49)=3.09

An1 of 1n/2Qn) and An2 of 1n/1Qn)=(1.^6+0.9375)=2.5375 1Qnc1 to 1Qnc2 (1.^6+2.49)=4.09

An1c2 and An2 of 1n/1Qn)=(0.^66+0.9375)=1.5975 1Qnc1 to 1Qnc2 (0.^66+2.49)=3.15


And change in both 1Qnc1 to 1Qnc2 with variant An2 of 1n/1Qn)

An1c2 of 1n/2Qn) and An2 of 1n/1Qn)=(1.^66+2.49)=4.15


It is not that these order of operations are incorrect by any means given the path and extent of the defined variables decimal stem cycles have potential change and limit to the variable definition at cn of the variants. 

The values are precise scale variables to the function of ƒ+⅄An1cn of altered addition paths with variants Ancn and altered within the paths sub-units nQncn. These are addition sums from ratios divided by ratios from variables of consecutive bases in y fibonacci and p prime variables. ƒ+⅄ᐱ represents complex path multiplication function of complex ratios.

Isolating a variable to a defined ratio numeral and then factoring with PEMDAS is one factoring path while other paths are not arranged to PEMDAS order of operations.


So then if variables of (A) are applicable to multiplication function +⅄=(nncn+nncn) for new variables from set equations

n+⅄ᐱ(Ancn+Ancn), ∈n+⅄ᐱ(Ancn+Bncn), ∈n+⅄ᐱ(Ancn+Dncn), ∈n+⅄ᐱ(Ancn+Encn), ∈n+⅄ᐱ(Ancn+Fncn), ∈n+⅄ᐱ(Ancn+Gncn), ∈n+⅄ᐱ(Ancn+Hncn), ∈n+⅄ᐱ(Ancn+Incn), ∈n+⅄ᐱ(Ancn+Jncn), ∈n+⅄ᐱ(Ancn+Kncn), ∈n+⅄ᐱ(Ancn+Lncn), ∈n+⅄ᐱ(Ancn+Mncn), ∈n+⅄ᐱ(Ancn+Nncn), ∈n+⅄ᐱ(Ancn+Oncn), ∈n+⅄ᐱ(Ancn+Pn), ∈n+⅄ᐱ(Ancn+Qncn), ∈n+⅄ᐱ(Ancn+Rncn), ∈n+⅄ᐱ(Ancn+Sncn), ∈n+⅄ᐱ(Ancn+Tncn), ∈n+⅄ᐱ(Ancn+Uncn),  ∈n+⅄ᐱ(Ancn+Vncn), ∈n+⅄ᐱ(Ancn+Wncn), ∈n+⅄ᐱ(Ancn+Yn), ∈n+⅄ᐱ(Ancn+Zncn), ∈n+⅄ᐱ(Ancnncn), ∈n+⅄ᐱ(Ancnncn), ∈n+⅄ᐱ(Ancn+ᐱncn), ∈n+⅄ᐱ(Ancn+ᗑncn), ∈n+⅄ᐱ(Ancn+∘⧊°ncn), ∈n+⅄ᐱ(Ancn+∘∇°ncn)


And +⅄=(nncn+nncn) function is also applicable to example [Nncn of (Ancn+Nncn) + Nncn of (Ancn+Nncn)]=Nncn


Function +⅄=(nncn+nncn) is applicable with variables from varying equation set variables such as

n+⅄ᐱ(An+An), ∈n+⅄ᐱ(An+Bn), ∈n+⅄ᐱ(An+Dn), ∈n+⅄ᐱ(An+En), ∈n+⅄ᐱ(An+Fn), ∈n+⅄ᐱ(An+Gn), ∈n+⅄ᐱ(An+Hn), ∈n+⅄ᐱ(An+In), ∈n+⅄ᐱ(An+Jn), ∈n+⅄ᐱ(An+Kn), ∈n+⅄ᐱ(An+Ln), ∈n+⅄ᐱ(An+Mn), ∈n+⅄ᐱ(An+Nn), ∈n+⅄ᐱ(An+On), ∈n+⅄ᐱ(An+Pn), ∈n+⅄ᐱ(An+Qn), ∈n+⅄ᐱ(An+Rn), ∈n+⅄ᐱ(An+Sn), ∈n+⅄ᐱ(An+Tn),∈n+⅄ᐱ(An+Un),  ∈n+⅄ᐱ(An+Vn), ∈n+⅄ᐱ(An+Wn), ∈n+⅄ᐱ(An+Yn), ∈n+⅄ᐱ(An+Zn), ∈n+⅄ᐱ(Ann), ∈n+⅄ᐱ(Ann),n+⅄ᐱ(Ancn+ᐱncn), ∈n+⅄ᐱ(Ancn+ᗑncn), ∈n+⅄ᐱ(Ancn+∘⧊°ncn), ∈n+⅄ᐱ(Ancn+∘∇°ncn)


n+⅄ᐱ(Bn+An), n+⅄ᐱ(Bn+Bn), ∈n+⅄ᐱ(Bn+Dn), ∈n+⅄ᐱ(Bn+En), ∈n+⅄ᐱ(Bn+Fn), ∈n+⅄ᐱ(Bn+Gn), ∈n+⅄ᐱ(Bn+Hn), ∈n+⅄ᐱ(Bn+In), ∈n+⅄ᐱ(Bn+Jn), ∈n+⅄ᐱ(Bn+Kn), ∈n+⅄ᐱ(Bn+Ln), ∈n+⅄ᐱ(Bn+Mn), ∈n+⅄ᐱ(Bn+Nn), ∈n+⅄ᐱ(Bn+On), ∈n+⅄ᐱ(Bn+Pn), ∈n+⅄ᐱ(Bn+Qn), ∈n+⅄ᐱ(Bn+Rn), ∈n+⅄ᐱ(Bn+Sn), ∈n+⅄ᐱ(Bn+Tn),∈n+⅄ᐱ(Bn+Un),  ∈n+⅄ᐱ(Bn+Vn), ∈n+⅄ᐱ(Bn+Wn), ∈n+⅄ᐱ(Bn+Yn), ∈n+⅄ᐱ(Bn+Zn), ∈n+⅄ᐱ(Bnn), ∈n+⅄ᐱ(Bnn),n+⅄ᐱ(Bncn+ᐱncn), ∈n+⅄ᐱ(Bncn+ᗑncn), ∈n+⅄ᐱ(Bncn+∘⧊°ncn), ∈n+⅄ᐱ(Bncn+∘∇°ncn)


n+⅄ᐱ(Dn+An), ∈n+⅄ᐱ(Dn+Bn), n+⅄ᐱ(Dn+Dn), ∈n+⅄ᐱ(Dn+En), ∈n+⅄ᐱ(Dn+Fn), ∈n+⅄ᐱ(Dn+Gn), ∈n+⅄ᐱ(Dn+Hn), ∈n+⅄ᐱ(Dn+In), ∈n+⅄ᐱ(Dn+Jn), ∈n+⅄ᐱ(Dn+Kn), ∈n+⅄ᐱ(Dn+Ln), ∈n+⅄ᐱ(Dn+Mn), ∈n+⅄ᐱ(Dn+Nn), ∈n+⅄ᐱ(Dn+On), ∈n+⅄ᐱ(Dn+Pn), ∈n+⅄ᐱ(Dn+Qn), ∈n+⅄ᐱ(Dn+Rn), ∈n+⅄ᐱ(Dn+Sn), ∈n+⅄ᐱ(Dn+Tn),∈n+⅄ᐱ(Dn+Un),  ∈n+⅄ᐱ(Dn+Vn), ∈n+⅄ᐱ(Dn+Wn), ∈n+⅄ᐱ(Dn+Yn), ∈n+⅄ᐱ(Dn+Zn), ∈n+⅄ᐱ(Dnn), ∈n+⅄ᐱ(Dnn),n+⅄ᐱ(Dncn+ᐱncn), ∈n+⅄ᐱ(Dncn+ᗑncn), ∈n+⅄ᐱ(Dncn+∘⧊°ncn), ∈n+⅄ᐱ(Dncn+∘∇°ncn)


n+⅄ᐱ(En+An), ∈n+⅄ᐱ(En+Bn), ∈n+⅄ᐱ(En+Dn), n+⅄ᐱ(En+En), ∈n+⅄ᐱ(En+Fn), ∈n+⅄ᐱ(En+Gn), ∈n+⅄ᐱ(En+Hn), ∈n+⅄ᐱ(En+In), ∈n+⅄ᐱ(En+Jn), ∈n+⅄ᐱ(En+Kn), ∈n+⅄ᐱ(En+Ln), ∈n+⅄ᐱ(En+Mn), ∈n+⅄ᐱ(En+Nn), ∈n+⅄ᐱ(En+On), ∈n+⅄ᐱ(En+Pn), ∈n+⅄ᐱ(En+⅄Qn), ∈n+⅄ᐱ(En+Rn), ∈n+⅄ᐱ(En+Sn), ∈n+⅄ᐱ(En+Tn),∈n+⅄ᐱ(En+Un),  ∈n+⅄ᐱ(En+Vn), ∈n+⅄ᐱ(En+Wn), ∈n+⅄ᐱ(En+Yn), ∈n+⅄ᐱ(En+Zn), ∈n+⅄ᐱ(Enn), ∈n+⅄ᐱ(Enn),n+⅄ᐱ(Encn+ᐱncn), ∈n+⅄ᐱ(Encn+ᗑncn), ∈n+⅄ᐱ(Encn+∘⧊°ncn), ∈n+⅄ᐱ(Encn+∘∇°ncn)


n+⅄ᐱ(Fn+An), ∈n+⅄ᐱ(Fnx+Bn), ∈n+⅄ᐱ(Fn+Dn), ∈n+⅄ᐱ(Fn+En), n+⅄ᐱ(Fn+Fn), ∈n+⅄ᐱ(Fn+Gn), ∈n+⅄ᐱ(Fn+Hn), ∈n+⅄ᐱ(Fn+In), ∈n+⅄ᐱ(Fn+Jn), ∈n+⅄ᐱ(Fn+Kn), ∈n+⅄ᐱ(Fn+Ln), ∈n+⅄ᐱ(Fn+Mn), ∈n+⅄ᐱ(Fn+Nn), ∈n+⅄ᐱ(Fn+On), ∈n+⅄ᐱ(Fn+Pn), ∈n+⅄ᐱ(Fn+Qn), ∈n+⅄ᐱ(Fn+Rn), ∈n+⅄ᐱ(Fn+Sn), ∈n+⅄ᐱ(Fn+Tn),∈n+⅄ᐱ(Fn+Un),  ∈n+⅄ᐱ(Fn+Vn), ∈n+⅄ᐱ(Fn+Wn), ∈n+⅄ᐱ(Fn+Yn), ∈n+⅄ᐱ(Fn+Zn), ∈n+⅄ᐱ(Fnn), ∈n+⅄ᐱ(Fnn),n+⅄ᐱ(Fncn+ᐱncn), ∈n+⅄ᐱ(Fncn+ᗑncn), ∈n+⅄ᐱ(Fncn+∘⧊°ncn), ∈n+⅄ᐱ(Fncn+∘∇°ncn)


n+⅄ᐱ(Gn+An), ∈n+⅄ᐱ(Gn+Bn), ∈n+⅄ᐱ(Gn+Dn), ∈n+⅄ᐱ(Gn+En), ∈n+⅄ᐱ(Gn+Fn), n+⅄ᐱ(Gn+Gn), ∈n+⅄ᐱ(Gn+Hn), ∈n+⅄ᐱ(Gn+In), ∈n+⅄ᐱ(Gn+Jn), ∈n+⅄ᐱ(Gn+Kn), ∈n+⅄ᐱ(Gn+Ln), ∈n+⅄ᐱ(Gn+Mn), ∈n+⅄ᐱ(Gn+Nn), ∈n+⅄ᐱ(Gn+On), ∈n+⅄ᐱ(Gn+Pn), ∈n+⅄ᐱ(Gn+Qn), ∈n+⅄ᐱ(Gn+Rn), ∈n+⅄ᐱ(Gn+Sn), ∈n+⅄ᐱ(Gn+Tn),∈n+⅄ᐱ(Gn+Un),  ∈n+⅄ᐱ(Gn+Vn), ∈n+⅄ᐱ(Gn+Wn), ∈n+⅄ᐱ(Gn+Yn), ∈n+⅄ᐱ(Gn+Zn), ∈n+⅄ᐱ(Gnn), ∈n+⅄ᐱ(Gnn),n+⅄ᐱ(Gncn+ᐱncn), ∈n+⅄ᐱ(Gncn+ᗑncn), ∈n+⅄ᐱ(Gncn+∘⧊°ncn), ∈n+⅄ᐱ(Gncn+∘∇°ncn)


n+⅄ᐱ(Hn+An), ∈n+⅄ᐱ(Hn+Bn), ∈n+⅄ᐱ(Hn+Dn), ∈n+⅄ᐱ(Hn+En), ∈n+⅄ᐱ(Hn+Fn), ∈n+⅄ᐱ(Hn+Gn), n+⅄ᐱ(Hn+Hn), ∈n+⅄ᐱ(Hn+In), ∈n+⅄ᐱ(Hn+Jn), ∈n+⅄ᐱ(Hn+Kn), ∈n+⅄ᐱ(Hn+Ln), ∈n+⅄ᐱ(Hn+Mn), ∈n+⅄ᐱ(Hn+Nn), ∈n+⅄ᐱ(Hn+On), ∈n+⅄ᐱ(Hn+Pn), ∈n+⅄ᐱ(Hn+Qn), ∈n+⅄ᐱ(Hn+Rn), ∈n+⅄ᐱ(Hn+Sn), ∈n+⅄ᐱ(Hn+Tn),∈n+⅄ᐱ(Hn+Un),  ∈n+⅄ᐱ(Hn+Vn), ∈n+⅄ᐱ(Hn+Wn), ∈n+⅄ᐱ(Hn+Yn), ∈n+⅄ᐱ(Hn+Zn), ∈n+⅄ᐱ(Hnn), ∈n+⅄ᐱ(Hnn),n+⅄ᐱ(Hncn+ᐱncn), ∈n+⅄ᐱ(Hncn+ᗑncn), ∈n+⅄ᐱ(Hncn+∘⧊°ncn), ∈n+⅄ᐱ(Hncn+∘∇°ncn)


n+⅄ᐱ(In+An), ∈n+⅄ᐱ(In+Bn), ∈n+⅄ᐱ(In+Dn), ∈n+⅄ᐱ(In+En), ∈n+⅄ᐱ(In+Fn), ∈n+⅄ᐱ(In+Gn), ∈n+⅄ᐱ(In+Hn), n+⅄ᐱ(In+In), ∈n+⅄ᐱ(In+Jn), ∈n+⅄ᐱ(In+Kn), ∈n+⅄ᐱ(In+Ln), ∈n+⅄ᐱ(In+Mn), ∈n+⅄ᐱ(In+Nn), ∈n+⅄ᐱ(In+On), ∈n+⅄ᐱ(In+Pn), ∈n+⅄ᐱ(In+Qn), ∈n+⅄ᐱ(In+Rn), ∈n+⅄ᐱ(In+Sn), ∈n+⅄ᐱ(In+Tn),∈n+⅄ᐱ(In+Un),  ∈n+⅄ᐱ(In+Vn), ∈n+⅄ᐱ(In+Wn), ∈n+⅄ᐱ(In+Yn), ∈n+⅄ᐱ(In+Zn), ∈n+⅄ᐱ(Inn), ∈n+⅄ᐱ(Inn),n+⅄ᐱ(Incn+ᐱncn), ∈n+⅄ᐱ(Incn+ᗑncn), ∈n+⅄ᐱ(Incn+∘⧊°ncn), ∈n+⅄ᐱ(Incn+∘∇°ncn)


n+⅄ᐱ(Jn+An), ∈n+⅄ᐱ(Jn+Bn), ∈n+⅄ᐱ(Jn+Dn), ∈n+⅄ᐱ(Jn+En), ∈n+⅄ᐱ(Jn+Fn), ∈n+⅄ᐱ(Jn+Gn), ∈n+⅄ᐱ(Jn+Hn), ∈n+⅄ᐱ(Jn+In), n+⅄ᐱ(Jn+Jn), ∈n+⅄ᐱ(Jn+Kn), ∈n+⅄ᐱ(Jn+Ln), ∈n+⅄ᐱ(Jn+Mn), ∈n+⅄ᐱ(Jn+Nn), ∈n+⅄ᐱ(Jn+On), ∈n+⅄ᐱ(Jn+Pn), ∈n+⅄ᐱ(Jn+Qn), ∈n+⅄ᐱ(Jn+Rn), ∈n+⅄ᐱ(Jn+Sn), ∈n+⅄ᐱ(Jn+Tn),∈n+⅄ᐱ(Jn+Un),  ∈n+⅄ᐱ(Jn+Vn), ∈n+⅄ᐱ(Jn+Wn), ∈n+⅄ᐱ(Jn+Yn), ∈n+⅄ᐱ(Jn+Zn), ∈n+⅄ᐱ(Jnn), ∈n+⅄ᐱ(Jnn),n+⅄ᐱ(Jncn+ᐱncn), ∈n+⅄ᐱ(Jncn+ᗑncn), ∈n+⅄ᐱ(Jncn+∘⧊°ncn), ∈n+⅄ᐱ(Jncn+∘∇°ncn)


n+⅄ᐱ(Kn+An), ∈n+⅄ᐱ(Kn+Bn), ∈n+⅄ᐱ(Kn+Dn), ∈n+⅄ᐱ(Kn+En), ∈n+⅄ᐱ(Kn+Fn), ∈n+⅄ᐱ(Kn+Gn), ∈n+⅄ᐱ(Kn+Hn), ∈n+⅄ᐱ(Kn+In), ∈n+⅄ᐱ(Kn+Jn), n+⅄ᐱ(Kn+Kn), ∈n+⅄ᐱ(Kn+Ln), ∈n+⅄ᐱ(Kn+Mn), ∈n+⅄ᐱ(Kn+Nn), ∈n+⅄ᐱ(Kn+On), ∈n+⅄ᐱ(Kn+Pn), ∈n+⅄ᐱ(Kn+Qn), ∈n+⅄ᐱ(Kn+Rn), ∈n+⅄ᐱ(Kn+Sn), ∈n+⅄ᐱ(Kn+Tn),∈n+⅄ᐱ(Kn+Un),  ∈n+⅄ᐱ(Kn+Vn), ∈n+⅄ᐱ(Kn+Wn), ∈n+⅄ᐱ(Kn+Yn), ∈n+⅄ᐱ(Kn+Zn), ∈n+⅄ᐱ(Knn), ∈n+⅄ᐱ(Knn),n+⅄ᐱ(Kncn+ᐱncn), ∈n+⅄ᐱ(Kncn+ᗑncn), ∈n+⅄ᐱ(Kncn+∘⧊°ncn), ∈n+⅄ᐱ(Kncn+∘∇°ncn)


n+⅄ᐱ(Ln+An), ∈n+⅄ᐱ(Ln+Bn), ∈n+⅄ᐱ(Ln+Dn), ∈n+⅄ᐱ(Ln+En), ∈n+⅄ᐱ(Ln+Fn), ∈n+⅄ᐱ(Ln+Gn), ∈n+⅄ᐱ(Ln+Hn), ∈n+⅄ᐱ(Ln+In), ∈n+⅄ᐱ(Ln+Jn), ∈n+⅄ᐱ(Ln+Kn), n+⅄ᐱ(Ln+Ln), ∈n+⅄ᐱ(Ln+Mn), ∈n+⅄ᐱ(Ln+Nn), ∈n+⅄ᐱ(Ln+On), ∈n+⅄ᐱ(Ln+Pn), ∈n+⅄ᐱ(Ln+Qn), ∈n+⅄ᐱ(Ln+Rn), ∈n+⅄ᐱ(Ln+Sn), ∈n+⅄ᐱ(Ln+Tn),∈n+⅄ᐱ(Ln+Un),  ∈n+⅄ᐱ(Ln+Vn), ∈n+⅄ᐱ(Ln+Wn), ∈n+⅄ᐱ(Ln+Yn), ∈n+⅄ᐱ(Ln+Zn), ∈n+⅄ᐱ(Lnn), ∈n+⅄ᐱ(Lnn),n+⅄ᐱ(Lncn+ᐱncn), ∈n+⅄ᐱ(Lncn+ᗑncn), ∈n+⅄ᐱ(Lncn+∘⧊°ncn), ∈n+⅄ᐱ(Lncn+∘∇°ncn)


n+⅄ᐱ(Mn+An), ∈n+⅄ᐱ(Mn+Bn), ∈n+⅄ᐱ(Mn+Dn), ∈n+⅄ᐱ(Mn+En), ∈n+⅄ᐱ(Mn+Fn), ∈n+⅄ᐱ(Mn+Gn), ∈n+⅄ᐱ(Mn+Hn), ∈n+⅄ᐱ(Mn+In), ∈n+⅄ᐱ(Mn+Jn), ∈n+⅄ᐱ(Mn+Kn), ∈n+⅄ᐱ(Mn+Ln), n+⅄ᐱ(Mn+Mn), ∈n+⅄ᐱ(Mn+Nn), ∈n+⅄ᐱ(Mn+On), ∈n+⅄ᐱ(Mn+Pn), ∈n+⅄ᐱ(Mn+Qn), ∈n+⅄ᐱ(Mn+Rn), ∈n+⅄ᐱ(Mn+Sn), ∈n+⅄ᐱ(Mn+Tn),∈n+⅄ᐱ(Mn+Un),  ∈n+⅄ᐱ(Mn+Vn), ∈n+⅄ᐱ(Mn+Wn), ∈n+⅄ᐱ(Mn+Yn), ∈n+⅄ᐱ(Mn+Zn), ∈n+⅄ᐱ(Mnn), ∈n+⅄ᐱ(Mnn),n+⅄ᐱ(Mncn+ᐱncn), ∈n+⅄ᐱ(Mncn+ᗑncn), ∈n+⅄ᐱ(Mncn+∘⧊°ncn), ∈n+⅄ᐱ(Mncn+∘∇°ncn)


n+⅄ᐱ(Nn+An), ∈n+⅄ᐱ(Nn+Bn), ∈n+⅄ᐱ(Nn+Dn), ∈n+⅄ᐱ(Nn+En), ∈n+⅄ᐱ(Nn+Fn), ∈n+⅄ᐱ(Nn+Gn), ∈n+⅄ᐱ(Nn+Hn), ∈n+⅄ᐱ(Nn+In), ∈n+⅄ᐱ(Nn+Jn), ∈n+⅄ᐱ(Nn+Kn), ∈n+⅄ᐱ(Nn+Ln), ∈n+⅄ᐱ(Nn+Mn), n+⅄ᐱ(Nn+Nn), ∈n+⅄ᐱ(Nn+On), ∈n+⅄ᐱ(Nn+Pn), ∈n+⅄ᐱ(Nn+Qn), ∈n+⅄ᐱ(Nn+Rn), ∈n+⅄ᐱ(Nn+Sn), ∈n+⅄ᐱ(Nn+Tn),∈n+⅄ᐱ(Nn+Un),  ∈n+⅄ᐱ(Nn+Vn), ∈n+⅄ᐱ(Nn+Wn), ∈n+⅄ᐱ(Nn+Yn), ∈n+⅄ᐱ(Nn+Zn), ∈n+⅄ᐱ(Nnn), ∈n+⅄ᐱ(Nnn),n+⅄ᐱ(Nncn+ᐱncn), ∈n+⅄ᐱ(Nncn+ᗑncn), ∈n+⅄ᐱ(Nncn+∘⧊°ncn), ∈n+⅄ᐱ(Nncn+∘∇°ncn)


n+⅄ᐱ(On+An), ∈n+⅄ᐱ(On+Bn), ∈n+⅄ᐱ(On+Dn), ∈n+⅄ᐱ(On+En), ∈n+⅄ᐱ(On+Fn), ∈n+⅄ᐱ(On+Gn), ∈n+⅄ᐱ(On+Hn), ∈n+⅄ᐱ(On+In), ∈n+⅄ᐱ(On+Jn), ∈n+⅄ᐱ(On+Kn), ∈n+⅄ᐱ(On+Ln), ∈n+⅄ᐱ(On+Mn), ∈n+⅄ᐱ(On+Nn), n+⅄ᐱ(On+On), ∈n+⅄ᐱ(On+Pn), ∈n+⅄ᐱ(On+Qn), ∈n+⅄ᐱ(On+Rn), ∈n+⅄ᐱ(On+Sn), ∈n+⅄ᐱ(On+Tn),∈n+⅄ᐱ(On+Un),  ∈n+⅄ᐱ(On+Vn), ∈n+⅄ᐱ(On+Wn), ∈n+⅄ᐱ(On+Yn), ∈n+⅄ᐱ(On+Zn), ∈n+⅄ᐱ(Onn), ∈n+⅄ᐱ(Onn),n+⅄ᐱ(Oncn+ᐱncn), ∈n+⅄ᐱ(Oncn+ᗑncn), ∈n+⅄ᐱ(Oncn+∘⧊°ncn), ∈n+⅄ᐱ(Oncn+∘∇°ncn)


n+⅄ᐱ(Pn+An), ∈n+⅄ᐱ(Pn+Bn), ∈n+⅄ᐱ(Pn+Dn), ∈n+⅄ᐱ(Pn+En), ∈n+⅄ᐱ(Pn+Fn), ∈n+⅄ᐱ(Pn+Gn), ∈n+⅄ᐱ(Pn+Hn), ∈n+⅄ᐱ(Pn+In), ∈n+⅄ᐱ(Pn+Jn), ∈n+⅄ᐱ(Pn+Kn), ∈n+⅄ᐱ(Pn+Ln), ∈n+⅄ᐱ(Pn+Mn), ∈n+⅄ᐱ(Pn+Nn), ∈n+⅄ᐱ(Pn+On), n+⅄ᐱ(Pn+Pn), ∈n+⅄ᐱ(Pn+Qn), ∈n+⅄ᐱ(Pn+Rn), ∈n+⅄ᐱ(Pn+Sn), ∈n+⅄ᐱ(Pn+Tn),∈n+⅄ᐱ(Pn+Un),  ∈n+⅄ᐱ(Pn+Vn), ∈n+⅄ᐱ(Pn+Wn), ∈n+⅄ᐱ(Pn+Yn), ∈n+⅄ᐱ(Pn+Zn), ∈n+⅄ᐱ(Pnn), ∈n+⅄ᐱ(Pnn),n+⅄ᐱ(Pncn+ᐱncn), ∈n+⅄ᐱ(Pncn+ᗑncn), ∈n+⅄ᐱ(Pncn+∘⧊°ncn), ∈n+⅄ᐱ(Pncn+∘∇°ncn)


n+⅄ᐱ(Qn+An), ∈n+⅄ᐱ(Qn+Bn), ∈n+⅄ᐱ(Qn+Dn), ∈n+⅄ᐱ(Qn+En), ∈n+⅄ᐱ(Qn+Fn), ∈n+⅄ᐱ(Qn+Gn), ∈n+⅄ᐱ(Qn+Hn), ∈n+⅄ᐱ(Qn+In), ∈n+⅄ᐱ(Qn+Jn), ∈n+⅄ᐱ(Qn+Kn), ∈n+⅄ᐱ(Qn+Ln), ∈n+⅄ᐱ(Qn+Mn), ∈n+⅄ᐱ(Qn+Nn), ∈n+⅄ᐱ(Qn+On), ∈n+⅄ᐱ(Qn+Pn), n+⅄ᐱ(Qn+Qn), ∈n+⅄ᐱ(Qn+Rn), ∈n+⅄ᐱ(Qn+Sn), ∈n+⅄ᐱ(Qn+Tn),∈n+⅄ᐱ(Qn+Un),  ∈n+⅄ᐱ(Qn+Vn), ∈n+⅄ᐱ(Qn+Wn), ∈n+⅄ᐱ(Qn+Yn), ∈n+⅄ᐱ(Qn+Zn), ∈n+⅄ᐱ(Qnn), ∈n+⅄ᐱ(Qnn),n+⅄ᐱ(Qncn+ᐱncn), ∈n+⅄ᐱ(Qncn+ᗑncn), ∈n+⅄ᐱ(Qncn+∘⧊°ncn), ∈n+⅄ᐱ(Qncn+∘∇°ncn)


n+⅄ᐱ(Rn+An), ∈n+⅄ᐱ(Rn+Bn), ∈n+⅄ᐱ(Rn+Dn), ∈n+⅄ᐱ(Rn+En), ∈n+⅄ᐱ(Rn+Fn), ∈n+⅄ᐱ(Rn+Gn), ∈n+⅄ᐱ(Rn+Hn), ∈n+⅄ᐱ(Rn+In), ∈n+⅄ᐱ(Rn+Jn), ∈n+⅄ᐱ(Rn+Kn), ∈n+⅄ᐱ(Rn+Ln), ∈n+⅄ᐱ(Rn+Mn), ∈n+⅄ᐱ(Rn+Nn), ∈n+⅄ᐱ(Rn+On), ∈n+⅄ᐱ(Rn+Pn), ∈n+⅄ᐱ(Rn+Qn), n+⅄ᐱ(Rn+Rn), ∈n+⅄ᐱ(Rn+Sn), ∈n+⅄ᐱ(Rn+Tn),∈n+⅄ᐱ(Rn+Un),  ∈n+⅄ᐱ(Rn+Vn), ∈n+⅄ᐱ(Rn+Wn), ∈n+⅄ᐱ(Rn+Yn), ∈n+⅄ᐱ(Rn+Zn), ∈n+⅄ᐱ(Rnn), ∈n+⅄ᐱ(Rnn),n+⅄ᐱ(Rncn+ᐱncn), ∈n+⅄ᐱ(Rncn+ᗑncn), ∈n+⅄ᐱ(Rncn+∘⧊°ncn), ∈n+⅄ᐱ(Rncn+∘∇°ncn)


n+⅄ᐱ(Sn+An), ∈n+⅄ᐱ(Sn+Bn), ∈n+⅄ᐱ(Sn+Dn), ∈n+⅄ᐱ(Sn+En), ∈n+⅄ᐱ(Sn+Fn), ∈n+⅄ᐱ(Sn+Gn), ∈n+⅄ᐱ(Sn+Hn), ∈n+⅄ᐱ(Sn+In), ∈n+⅄ᐱ(Sn+Jn), ∈n+⅄ᐱ(Sn+Kn), ∈n+⅄ᐱ(Sn+Ln), ∈n+⅄ᐱ(Sn+Mn), ∈n+⅄ᐱ(Sn+Nn), ∈n+⅄ᐱ(Sn+On), ∈n+⅄ᐱ(Sn+Pn), ∈n+⅄ᐱ(Sn+Qn), ∈n+⅄ᐱ(Sn+Rn), n+⅄ᐱ(Sn+Sn), ∈n+⅄ᐱ(Sn+Tn),∈n+⅄ᐱ(Sn+Un),  ∈n+⅄ᐱ(Sn+Vn), ∈n+⅄ᐱ(Sn+Wn), ∈n+⅄ᐱ(Sn+Yn), ∈n+⅄ᐱ(Sn+Zn), ∈n+⅄ᐱ(Snn), ∈n+⅄ᐱ(Snn),n+⅄ᐱ(Sncn+ᐱncn), ∈n+⅄ᐱ(Sncn+ᗑncn), ∈n+⅄ᐱ(Sncn+∘⧊°ncn), ∈n+⅄ᐱ(Sncn+∘∇°ncn)


n+⅄ᐱ(Tn+An), ∈n+⅄ᐱ(Tn+Bn), ∈n+⅄ᐱ(Tn+Dn), ∈n+⅄ᐱ(Tn+En), ∈n+⅄ᐱ(Tn+Fn), ∈n+⅄ᐱ(Tn+Gn), ∈n+⅄ᐱ(Tn+Hn), ∈n+⅄ᐱ(Tn+In), ∈n+⅄ᐱ(Tn+Jn), ∈n+⅄ᐱ(Tn+Kn), ∈n+⅄ᐱ(Tn+Ln), ∈n+⅄ᐱ(Tn+Mn), ∈n+⅄ᐱ(Tn+Nn), ∈n+⅄ᐱ(Tn+On), ∈n+⅄ᐱ(Tn+Pn), ∈n+⅄ᐱ(Tn+Qn), ∈n+⅄ᐱ(Tn+Rn), ∈n+⅄ᐱ(Tn+Sn), n+⅄ᐱ(Tn+Tn),∈n+⅄ᐱ(Tn+Un),  ∈n+⅄ᐱ(Tn+Vn), ∈n+⅄ᐱ(Tn+Wn), ∈n+⅄ᐱ(Tn+Yn), ∈n+⅄ᐱ(Tn+Zn), ∈n+⅄ᐱ(Tnn), ∈n+⅄ᐱ(Tnn),n+⅄ᐱ(Tncn+ᐱncn), ∈n+⅄ᐱ(Tncn+ᗑncn), ∈n+⅄ᐱ(Tncn+∘⧊°ncn), ∈n+⅄ᐱ(Tncn+∘∇°ncn)


n+⅄ᐱ(Un+An), ∈n+⅄ᐱ(Un+Bn), ∈n+⅄ᐱ(Un+Dn), ∈n+⅄ᐱ(Un+En), ∈n+⅄ᐱ(Un+Fn), ∈n+⅄ᐱ(Un+Gn), ∈n+⅄ᐱ(Un+Hn), ∈n+⅄ᐱ(Un+In), ∈n+⅄ᐱ(Un+Jn), ∈n+⅄ᐱ(Un+Kn), ∈n+⅄ᐱ(Un+Ln), ∈n+⅄ᐱ(Un+Mn), ∈n+⅄ᐱ(Un+Nn), ∈n+⅄ᐱ(Un+On), ∈n+⅄ᐱ(Un+Pn), ∈n+⅄ᐱ(Un+Qn), ∈n+⅄ᐱ(Un+Rn), ∈n+⅄ᐱ(Un+Sn), ∈n+⅄ᐱ(Un+Tn),n+⅄ᐱ(Un+Un),  ∈n+⅄ᐱ(Un+Vn), ∈n+⅄ᐱ(Un+Wn), ∈n+⅄ᐱ(Un+Yn), ∈n+⅄ᐱ(Un+Zn), ∈n+⅄ᐱ(Unn), ∈n+⅄ᐱ(Unn),n+⅄ᐱ(Uncn+ᐱncn), ∈n+⅄ᐱ(Uncn+ᗑncn), ∈n+⅄ᐱ(Uncn+∘⧊°ncn), ∈n+⅄ᐱ(Uncn+∘∇°ncn)


n+⅄ᐱ(Vn+An), ∈n+⅄ᐱ(Vn+Bn), ∈n+⅄ᐱ(Vn+Dn), ∈n+⅄ᐱ(Vn+En), ∈n+⅄ᐱ(Vn+Fn), ∈n+⅄ᐱ(Vn+Gn), ∈n+⅄ᐱ(Vn+Hn), ∈n+⅄ᐱ(Vn+In), ∈n+⅄ᐱ(Vn+Jn), ∈n+⅄ᐱ(Vn+Kn), ∈n+⅄ᐱ(Vn+Ln), ∈n+⅄ᐱ(Vn+Mn), ∈n+⅄ᐱ(Vn+Nn), ∈n+⅄ᐱ(Vn+On), ∈n+⅄ᐱ(Vn+Pn), ∈n+⅄ᐱ(Vn+Qn), ∈n+⅄ᐱ(Vn+Rn), ∈n+⅄ᐱ(Vn+Sn), ∈n+⅄ᐱ(Vn+Tn),∈n+⅄ᐱ(Vn+Un),  n+⅄ᐱ(Vn+Vn), ∈n+⅄ᐱ(Vn+Wn), ∈n+⅄ᐱ(Vn+Yn), ∈n+⅄ᐱ(Vn+Zn), ∈n+⅄ᐱ(Vnn), ∈n+⅄ᐱ(Vnn),n+⅄ᐱ(Vncn+ᐱncn), ∈n+⅄ᐱ(Vncn+ᗑncn), ∈n+⅄ᐱ(Vncn+∘⧊°ncn), ∈n+⅄ᐱ(Vncn+∘∇°ncn)


n+⅄ᐱ(Wn+An), ∈n+⅄ᐱ(Wn+Bn), ∈n+⅄ᐱ(Wn+Dn), ∈n+⅄ᐱ(Wn+En), ∈n+⅄ᐱ(Wn+Fn), ∈n+⅄ᐱ(Wn+Gn), ∈n+⅄ᐱ(Wn+Hn), ∈n+⅄ᐱ(Wn+In), ∈n+⅄ᐱ(Wn+Jn), ∈n+⅄ᐱ(Wn+Kn), ∈n+⅄ᐱ(Wn+Ln), ∈n+⅄ᐱ(Wn+Mn), ∈n+⅄ᐱ(Wn+Nn), ∈n+⅄ᐱ(Wn+On), ∈n+⅄ᐱ(Wn+Pn), ∈n+⅄ᐱ(Wn+Qn), ∈n+⅄ᐱ(Wn+Rn), ∈n+⅄ᐱ(Wn+Sn), ∈n+⅄ᐱ(Wn+Tn),∈n+⅄ᐱ(Wn+Un),  ∈n+⅄ᐱ(Wn+Vn), n+⅄ᐱ(Wn+Wn), ∈n+⅄ᐱ(Wn+Yn), ∈n+⅄ᐱ(Wn+Zn), ∈n+⅄ᐱ(Wnn), ∈n+⅄ᐱ(Wnn),n+⅄ᐱ(Wncn+ᐱncn), ∈n+⅄ᐱ(Wncn+ᗑncn), ∈n+⅄ᐱ(Wncn+∘⧊°ncn), ∈n+⅄ᐱ(Wncn+∘∇°ncn)


n+⅄ᐱ(Yn+An), ∈n+⅄ᐱ(Yn+Bn), ∈n+⅄ᐱ(Yn+Dn), ∈n+⅄ᐱ(Yn+En), ∈n+⅄ᐱ(Yn+Fn), ∈n+⅄ᐱ(Yn+Gn), ∈n+⅄ᐱ(Yn+Hn), ∈n+⅄ᐱ(Yn+In), ∈n+⅄ᐱ(Yn+Jn), ∈n+⅄ᐱ(Yn+Kn), ∈n+⅄ᐱ(Yn+Ln), ∈n+⅄ᐱ(Yn+Mn), ∈n+⅄ᐱ(Yn+Nn), ∈n+⅄ᐱ(Yn+On), ∈n+⅄ᐱ(Yn+Pn), ∈n+⅄ᐱ(Yn+Qn), ∈n+⅄ᐱ(Yn+Rn), ∈n+⅄ᐱ(Yn+Sn), ∈n+⅄ᐱ(Yn+Tn),∈n+⅄ᐱ(Yn+Un),  ∈n+⅄ᐱ(Yn+Vn), ∈n+⅄ᐱ(Yn+Wn), n+⅄ᐱ(Yn+Yn), ∈n+⅄ᐱ(Yn+Zn), ∈n+⅄ᐱ(Ynn), ∈n+⅄ᐱ(Ynn),n+⅄ᐱ(Yncn+ᐱncn), ∈n+⅄ᐱ(Yncn+ᗑncn), ∈n+⅄ᐱ(Yncn+∘⧊°ncn), ∈n+⅄ᐱ(Yncn+∘∇°ncn)


n+⅄ᐱ(Zn+An), ∈n+⅄ᐱ(Zn+Bn), ∈n+⅄ᐱ(Zn+Dn), ∈n+⅄ᐱ(Zn+En), ∈n+⅄ᐱ(Zn+Fn), ∈n+⅄ᐱ(Zn+Gn), ∈n+⅄ᐱ(Zn+Hn), ∈n+⅄ᐱ(Zn+In), ∈n+⅄ᐱ(Zn+Jn), ∈n+⅄ᐱ(Zn+Kn), ∈n+⅄ᐱ(Zn+Ln), ∈n+⅄ᐱ(Zn+Mn), ∈n+⅄ᐱ(Zn+Nn), ∈n+⅄ᐱ(Zn+On), ∈n+⅄ᐱ(Zn+Pn), ∈n+⅄ᐱ(Zn+Qn), ∈n+⅄ᐱ(Zn+Rn), ∈n+⅄ᐱ(Zn+Sn), ∈n+⅄ᐱ(Zn+Tn),∈n+⅄ᐱ(Zn+Un),  ∈n+⅄ᐱ(Zn+Vn), ∈n+⅄ᐱ(Zn+Wn), ∈n+⅄ᐱ(Zn+Yn), n+⅄ᐱ(Zn+Zn), ∈n+⅄ᐱ(Znn), ∈n+⅄ᐱ(Znn),n+⅄ᐱ(Zncn+ᐱncn), ∈n+⅄ᐱ(Zncn+ᗑncn), ∈n+⅄ᐱ(Zncn+∘⧊°ncn), ∈n+⅄ᐱ(Zncn+∘∇°ncn)


n+⅄ᐱ(φn+An), ∈n+⅄ᐱ(φn+Bn), ∈n+⅄ᐱ(φn+Dn), ∈n+⅄ᐱ(φn+En), ∈n+⅄ᐱ(φn+Fn), ∈n+⅄ᐱ(φn+Gn), ∈n+⅄ᐱ(φn+Hn), ∈n+⅄ᐱ(φn+In), ∈n+⅄ᐱ(φn+Jn), ∈n+⅄ᐱ(φn+Kn), ∈n+⅄ᐱ(φn+Ln), ∈n+⅄ᐱ(φn+Mn), ∈n+⅄ᐱ(φn+Nn), ∈n+⅄ᐱ(φn+On), ∈n+⅄ᐱ(φn+Pn), ∈n+⅄ᐱ(φn+Qn), ∈n+⅄ᐱ(φn+Rn), ∈n+⅄ᐱ(φn+Sn), ∈n+⅄ᐱ(φn+Tn),∈n+⅄ᐱ(φn+Un),  ∈n+⅄ᐱ(φn+Vn), ∈n+⅄ᐱ(φn+Wn), ∈n+⅄ᐱ(φn+Yn), ∈n+⅄ᐱ(φn+Zn), n+⅄ᐱ(φnn), ∈n+⅄ᐱ(φnn),n+⅄ᐱ(φncn+ᐱncn), ∈n+⅄ᐱ(φncn+ᗑncn), ∈n+⅄ᐱ(φncn+∘⧊°ncn), ∈n+⅄ᐱ(φncn+∘∇°ncn)


n+⅄ᐱ(Θn+An), ∈n+⅄ᐱ(Θn+Bn), ∈n+⅄ᐱ(Θn+Dn), ∈n+⅄ᐱ(Θn+En), ∈n+⅄ᐱ(Θn+Fn), ∈n+⅄ᐱ(Θn+Gn), ∈n+⅄ᐱ(Θn+Hn), ∈n+⅄ᐱ(Θn+In), ∈n+⅄ᐱ(Θn+Jn), ∈n+⅄ᐱ(Θn+Kn), ∈n+⅄ᐱ(Θn+Ln), ∈n+⅄ᐱ(Θn+Mn), ∈n+⅄ᐱ(Θn+Nn), ∈n+⅄ᐱ(Θn+On), ∈n+⅄ᐱ(Θn+Pn), ∈n+⅄ᐱ(Θn+Qn), ∈n+⅄ᐱ(Θn+Rn), ∈n+⅄ᐱ(Θn+Sn), ∈n+⅄ᐱ(Θn+Tn),∈n+⅄ᐱ(Θn+Un),  ∈n+⅄ᐱ(Θn+Vn), ∈n+⅄ᐱ(Θn+Wn), ∈n+⅄ᐱ(Θn+Yn), ∈n+⅄ᐱ(Θn+Zn), ∈n+⅄ᐱ(Θnn), n+⅄ᐱ(Θnn), ∈n+⅄ᐱ(Θncn+ᐱncn), ∈n+⅄ᐱ(Θncn+ᗑncn), ∈n+⅄ᐱ(Θncn+∘⧊°ncn), ∈n+⅄ᐱ(Θncn+∘∇°ncn)


1-⅄=(n2-n1)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

1-⅄=(n2-n1) that a function path is factored to the definition of the function path rather than pemdas order of operations.

Variables are factorable to a measured units that then be later can applied in functions of proper order of operations that is parenthesis, exponents, multiplication, division, addition, and then subtraction. 

Function path 1-⅄=(n2-n1) is nn2cn later number in a set of consecutive variables minus nn1cn previous number in a set of consecutive variables, such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant.

1-ᐱ(An2-An1), ∈1-⅄ᐱ(An2-Bn1), ∈1-⅄ᐱ(An2-Dn1), ∈1-⅄ᐱ(An2-En1), ∈1-⅄ᐱ(An2-Fn1), ∈1-⅄ᐱ(An2-Gn1), ∈1-⅄ᐱ(An2-Hn1), ∈1-⅄ᐱ(An2-In1), ∈1-⅄ᐱ(An2-Jn1), ∈1-⅄ᐱ(An2-Kn1), ∈1-⅄ᐱ(An2-Ln1), ∈1-⅄ᐱ(An2-Mn1), ∈1-⅄ᐱ(An2-Nn1), ∈1-⅄ᐱ(An2-On1), ∈1-⅄ᐱ(An2-Pn1), ∈1-⅄ᐱ(An2-Qn1), ∈1-⅄ᐱ(An2-Rn1), ∈1-⅄ᐱ(An2-Sn1), ∈1-⅄ᐱ(An2-Tn1), ∈1-⅄ᐱ(An2-Un1),  ∈1-⅄ᐱ(An2-Vn1), ∈1-⅄ᐱ(An2-Wn1), ∈1-⅄ᐱ(An2-Yn1), ∈1-⅄ᐱ(An2-Zn1), ∈1-⅄ᐱ(An2n1), ∈1-⅄ᐱ(An2n1), 2-ᐱ(An2cn-n1cn), ∈1-ᐱ(An2cn-n1cn), ∈1-ᐱ(An2cn-∘⧊°n1cn), ∈1-ᐱ(An2cn-∘∇°n1cn)

1-⅄ᐱ(Bn2-An1), 2-ᐱ(Bn2-Bn1), ∈1-⅄ᐱ(Bn2-Dn1), ∈1-⅄ᐱ(Bn2-En1), ∈1-⅄ᐱ(Bn2-Fn1), ∈1-⅄ᐱ(Bn2-Gn1), ∈1-⅄ᐱ(Bn2-Hn1), ∈1-⅄ᐱ(Bn2-In1), ∈1-⅄ᐱ(Bn2-Jn1), ∈1-⅄ᐱ(Bn2-Kn1), ∈1-⅄ᐱ(Bn2-Ln1), ∈1-⅄ᐱ(Bn2-Mn1), ∈1-⅄ᐱ(Bn2-Nn1), ∈1-⅄ᐱ(Bn2-On1), ∈1-⅄ᐱ(Bn2-Pn1), ∈1-⅄ᐱ(Bn2-Qn1), ∈1-⅄ᐱ(Bn2-Rn1), ∈1-⅄ᐱ(Bn2-Sn1), ∈1-⅄ᐱ(Bn2-Tn1), ∈1-⅄ᐱ(Bn2-Un1), ∈1-⅄ᐱ(Bn2-Vn1), ∈1-⅄ᐱ(Bn2-Wn1), ∈1-⅄ᐱ(Bn2-Yn1), ∈1-⅄ᐱ(Bn2-Zn1), ∈1-⅄ᐱ(Bn2n1), ∈1-⅄ᐱ(Bn2n1),1-ᐱ(Bn2cn-n1cn), ∈1-ᐱ(Bn2cn-n1cn), ∈1-ᐱ(Bn2cn-∘⧊°n1cn), ∈1-ᐱ(Bn2cn-∘∇°n1cn)

1-⅄ᐱ(Dn2-An1), ∈1-⅄ᐱ(Dn2-Bn1), 1-ᐱ(Dn2-Dn1), ∈1-⅄ᐱ(Dn2-En1), ∈1-⅄ᐱ(Dn2-Fn1), ∈1-⅄ᐱ(Dn2-Gn1), ∈1-⅄ᐱ(Dn2-Hn1), ∈1-⅄ᐱ(Dn2-In1), ∈1-⅄ᐱ(Dn2-Jn1), ∈1-⅄ᐱ(Dn2-Kn1), ∈1-⅄ᐱ(Dn2-Ln1), ∈1-⅄ᐱ(Dn2-Mn1), ∈1-⅄ᐱ(Dn2-Nn1), ∈1-⅄ᐱ(Dn2-On1), ∈1-⅄ᐱ(Dn2-Pn1), ∈1-⅄ᐱ(Dn2-Qn1), ∈1-⅄ᐱ(Dn2-Rn1), ∈1-⅄ᐱ(Dn2-Sn1), ∈1-⅄ᐱ(Dn2-Tn1), ∈1-⅄ᐱ(Dn2-Un1),  ∈1-⅄ᐱ(Dn2-Vn1), ∈1-⅄ᐱ(Dn2-Wn1), ∈1-⅄ᐱ(Dn2-Yn1), ∈1-⅄ᐱ(Dn2-Zn1), ∈1-⅄ᐱ(Dn2n1), ∈1-⅄ᐱ(Dn2n1), 1-ᐱ(Dn2cn-n1cn), ∈1-ᐱ(Dn2cn-n1cn), ∈1-ᐱ(Dn2cn-∘⧊°n1cn), ∈1-ᐱ(Dn2cn-∘∇°n1cn)

1-⅄ᐱ(En2-An1), ∈1-⅄ᐱ(En2-Bn1), ∈1-⅄ᐱ(En2-Dn1), 1-ᐱ(En2-En1), ∈1-⅄ᐱ(En2-Fn1), ∈1-⅄ᐱ(En2-Gn1), ∈1-⅄ᐱ(En2-Hn1), ∈1-⅄ᐱ(En2-In1), ∈1-⅄ᐱ(En2-Jn1), ∈1-⅄ᐱ(En2-Kn1), ∈1-⅄ᐱ(En2-Ln1), ∈1-⅄ᐱ(En2-Mn1), ∈1-⅄ᐱ(En2-Nn1), ∈1-⅄ᐱ(En2-On1), ∈1-⅄ᐱ(En2-Pn1), ∈1-⅄ᐱ(En2-Qn1), ∈1-⅄ᐱ(En2-Rn1), ∈1-⅄ᐱ(En2-Sn1), ∈1-⅄ᐱ(En2-Tn1),∈1-⅄ᐱ(En2-Un1), ∈1-⅄ᐱ(En2-Vn1), ∈1-⅄ᐱ(En2-Wn1), ∈1-⅄ᐱ(En2-Yn1), ∈1-⅄ᐱ(En2-Zn1), ∈1-⅄ᐱ(En2n1), ∈1-⅄ᐱ(En2n1),1-ᐱ(En2cn-n1cn), ∈1-ᐱ(En2cn-n1cn), ∈1-ᐱ(En2cn-∘⧊°n1cn), ∈1-ᐱ(En2cn-∘∇°n1cn)

1-⅄ᐱ(Fn2-An1), ∈1-⅄ᐱ(Fn2-Bn1), ∈1-⅄ᐱ(Fn2-Dn1), ∈1-⅄ᐱ(Fn2-En1), 1-ᐱ(Fn2-Fn1), ∈1-⅄ᐱ(Fn2-Gn1), ∈1-⅄ᐱ(Fn2-Hn1), ∈1-⅄ᐱ(Fn2-In1), ∈1-⅄ᐱ(Fn2-Jn1), ∈1-⅄ᐱ(Fn2-Kn1), ∈1-⅄ᐱ(Fn2-Ln1), ∈1-⅄ᐱ(Fn2-Mn1), ∈1-⅄ᐱ(Fn2-Nn1), ∈1-⅄ᐱ(Fn2-On1), ∈1-⅄ᐱ(Fn2-Pn1), ∈1-⅄ᐱ(Fn2-Qn1), ∈1-⅄ᐱ(Fn2-Rn1), ∈1-⅄ᐱ(Fn2-Sn1), ∈1-⅄ᐱ(Fn2-Tn1),∈1-⅄ᐱ(Fn2-Un1),  ∈1-⅄ᐱ(Fn2-Vn1), ∈1-⅄ᐱ(Fn2-Wn1), ∈1-⅄ᐱ(Fn2-Yn1), ∈1-⅄ᐱ(Fn2-Zn1), ∈1-⅄ᐱ(Fn2n1), ∈1-⅄ᐱ(Fn2n1),1-ᐱ(Fn2cn-n1cn), ∈1-ᐱ(Fn2cn-n1cn), ∈1-ᐱ(Fn2cn-∘⧊°n1cn), ∈1-ᐱ(Fn2cn-∘∇°n1cn)

1-⅄ᐱ(Gn2-An1), ∈1-⅄ᐱ(Gn2-Bn1), ∈1-⅄ᐱ(Gn2-Dn1), ∈1-⅄ᐱ(Gn2-En1), ∈1-⅄ᐱ(Gn2-Fn1), 1-ᐱ(Gn2-Gn1), ∈1-⅄ᐱ(Gn2-Hn1), ∈1-⅄ᐱ(Gn2-In1), ∈1-⅄ᐱ(Gn2-Jn1), ∈1-⅄ᐱ(Gn2-Kn1), ∈1-⅄ᐱ(Gn2-Ln1), ∈1-⅄ᐱ(Gn2-Mn1), ∈1-⅄ᐱ(Gn2-Nn1), ∈1-⅄ᐱ(Gn2-On1), ∈1-⅄ᐱ(Gn2-Pn1), ∈1-⅄ᐱ(Gn2-Qn1), ∈1-⅄ᐱ(Gn2-Rn1), ∈1-⅄ᐱ(Gn2-Sn1), ∈1-⅄ᐱ(Gn2-Tn1),∈1-⅄ᐱ(Gn2-Un1),  ∈1-⅄ᐱ(Gn2-Vn1), ∈1-⅄ᐱ(Gn2-Wn1), ∈1-⅄ᐱ(Gn2-Yn1), ∈1-⅄ᐱ(Gn2-Zn1), ∈1-⅄ᐱ(Gn2n1), ∈1-⅄ᐱ(Gn2n1),1-ᐱ(Gn2cn-n1cn), ∈1-ᐱ(Gn2cn-n1cn), ∈1-ᐱ(Gn2cn-∘⧊°n1cn), ∈1-ᐱ(Gn2cn-∘∇°n1cn)

1-⅄ᐱ(Hn2-An1), ∈1-⅄ᐱ(Hn2-Bn1), ∈1-⅄ᐱ(Hn2-Dn1), ∈1-⅄ᐱ(Hn2-En1), ∈1-⅄ᐱ(Hn2-Fn1), ∈1-⅄ᐱ(Hn2-Gn1), 1-ᐱ(Hn2-Hn1), ∈1-⅄ᐱ(Hn2-In1), ∈1-⅄ᐱ(Hn2-Jn1), ∈1-⅄ᐱ(Hn2-Kn1), ∈1-⅄ᐱ(Hn2-Ln1), ∈1-⅄ᐱ(Hn2-Mn1), ∈1-⅄ᐱ(Hn2-Nn1), ∈1-⅄ᐱ(Hn2-On1), ∈1-⅄ᐱ(Hn2-Pn1), ∈1-⅄ᐱ(Hn2-Qn1), ∈1-⅄ᐱ(Hn2-Rn1), ∈1-⅄ᐱ(Hn2-Sn1), ∈1-⅄ᐱ(Hn2-Tn1), ∈1-⅄ᐱ(Hn2-Un1),  ∈1-⅄ᐱ(Hn2-Vn1), ∈1-⅄ᐱ(Hn2-Wn1), ∈1-⅄ᐱ(Hn2-Yn1), ∈1-⅄ᐱ(Hn2-Zn1), ∈1-⅄ᐱ(Hn2n1), ∈1-⅄ᐱ(Hn2n1),1-ᐱ(Hn2cn-n1cn), ∈1-⅄Xᐱ(Hn2cn-n1cn), ∈1-ᐱ(Hn2cn-∘⧊°n1cn), ∈1-ᐱ(Hn2cn-∘∇°n1cn)

1-⅄ᐱ(In2-An1), ∈1-⅄ᐱ(In2-Bn1), ∈1-⅄ᐱ(In2-Dn1), ∈1-⅄ᐱ(In2-En1), ∈1-⅄ᐱ(In2-Fn1), ∈1-⅄ᐱ(In2-Gn1), ∈1-⅄ᐱ(In2-Hn1), 1-ᐱ(In2-In1), ∈1-⅄ᐱ(In2-Jn1), ∈1-⅄ᐱ(In2-Kn1), ∈1-⅄ᐱ(In2-Ln1), ∈1-⅄ᐱ(In2-Mn1), ∈1-⅄ᐱ(In2-Nn1), ∈1-⅄ᐱ(In2-On1), ∈1-⅄ᐱ(In2-Pn1), ∈1-⅄ᐱ(In2-Qn1), ∈1-⅄ᐱ(In2-Rn1), ∈1-⅄ᐱ(In2-Sn1), ∈1-⅄ᐱ(In2-Tn1),∈1-⅄ᐱ(In2-Un1),  ∈1-⅄ᐱ(In2-Vn1), ∈1-⅄ᐱ(In2-Wn1), ∈1-⅄ᐱ(In2-Yn1), ∈1-⅄ᐱ(In2-Zn1), ∈1-⅄ᐱ(In2n1), ∈1-⅄ᐱ(In2n1),1-ᐱ(In2cn-n1cn), ∈1-ᐱ(In2cn-n1cn), ∈1-ᐱ(In2cn-∘⧊°n1cn), ∈1-ᐱ(In2cn-∘∇°n1cn)

1-⅄ᐱ(Jn2-An1), ∈1-⅄ᐱ(Jn2-Bn1), ∈1-⅄ᐱ(Jn2-Dn1), ∈1-⅄ᐱ(Jn2-En1), ∈1-⅄ᐱ(Jn2-Fn1), ∈1-⅄ᐱ(Jn2-Gn1), ∈1-⅄ᐱ(Jn2-Hn1), ∈1-⅄ᐱ(Jn2-In1), 1-ᐱ(Jn2-Jn1), ∈1-⅄ᐱ(Jn2-Kn1), ∈1-⅄ᐱ(Jn2-Ln1), ∈1-⅄ᐱ(Jn2-Mn1), ∈1-⅄ᐱ(Jn2-Nn1), ∈1-⅄ᐱ(Jn2-On1), ∈1-⅄ᐱ(Jn2-Pn1), ∈1-⅄ᐱ(Jn2-Qn1), ∈1-⅄ᐱ(Jn2-Rn1), ∈1-⅄ᐱ(Jn2-Sn1), ∈1-⅄ᐱ(Jn2-Tn1),∈1-⅄ᐱ(Jn2-Un1),  ∈1-⅄ᐱ(Jn2-Vn1), ∈1-⅄ᐱ(Jn2-Wn1), ∈1-⅄ᐱ(Jn2-Yn1), ∈1-⅄ᐱ(Jn2-Zn1), ∈1-⅄ᐱ(Jn2n1), ∈1-⅄ᐱ(Jn2n1),1-ᐱ(Jn2cn-n1cn), ∈1-ᐱ(Jn2cn-n1cn), ∈1-ᐱ(Jn2cn-∘⧊°n1cn), ∈1-ᐱ(Jn2cn-∘∇°n1cn)

1-⅄ᐱ(Kn2-An1), ∈1-⅄ᐱ(Kn2-Bn1), ∈1-⅄ᐱ(Kn2-Dn1), ∈1-⅄ᐱ(Kn2-En1), ∈1-⅄ᐱ(Kn2-Fn1), ∈1-⅄ᐱ(Kn2-Gn1), ∈1-⅄ᐱ(Kn2-Hn1), ∈1-⅄ᐱ(Kn2-In1), ∈1-⅄ᐱ(Kn2-Jn1), 1-ᐱ(Kn2-Kn1), ∈1-⅄ᐱ(Kn2-Ln1), ∈1-⅄ᐱ(Kn2-Mn1), ∈1-⅄ᐱ(Kn2-Nn1), ∈1-⅄ᐱ(Kn2-On1), ∈1-⅄ᐱ(Kn2-Pn1), ∈1-⅄ᐱ(Kn2-Qn1), ∈1-⅄ᐱ(Kn2-Rn1), ∈1-⅄ᐱ(Kn2-Sn1), ∈1-⅄ᐱ(Kn2-Tn1),∈1-⅄ᐱ(Kn2-Un1),  ∈1-⅄ᐱ(Kn2-Vn1), ∈1-⅄ᐱ(Kn2-Wn1), ∈1-⅄ᐱ(Kn2-Yn1), ∈1-⅄ᐱ(Kn2-Zn1), ∈1-⅄ᐱ(Kn2n1), ∈1-⅄ᐱ(Kn2n1),1-ᐱ(Kn2cn-n1cn), ∈1-ᐱ(Kn2cn-n1cn), ∈1-ᐱ(Kn2cn-∘⧊°n1cn), ∈1-ᐱ(Kn2cn-∘∇°n1cn)

1-⅄ᐱ(Ln2-An1), ∈1-⅄ᐱ(Ln2-Bn1), ∈1-⅄ᐱ(Ln2-Dn1), ∈1-⅄ᐱ(Ln2-En1), ∈1-⅄ᐱ(Ln2-Fn1), ∈1-⅄ᐱ(Ln2-Gn1), ∈1-⅄ᐱ(Ln2-Hn1), ∈1-⅄ᐱ(Ln2-In1), ∈1-⅄ᐱ(Ln2-Jn1), ∈1-⅄ᐱ(Ln2-Kn1), 1-ᐱ(Ln2-Ln1), ∈1-⅄ᐱ(Ln2-Mn1), ∈1-⅄ᐱ(Ln2-Nn1), ∈1-⅄ᐱ(Ln2-On1), ∈1-⅄ᐱ(Ln2-Pn1), ∈1-⅄ᐱ(Ln2-Qn1), ∈1-⅄ᐱ(Ln2-Rn1), ∈1-⅄ᐱ(Ln2-Sn1), ∈1-⅄ᐱ(Ln2-Tn1),∈1-⅄ᐱ(Ln2-Un1),  ∈1-⅄ᐱ(Ln2-Vn1), ∈1-⅄ᐱ(Ln2-Wn1), ∈1-⅄ᐱ(Ln2-Yn1), ∈1-⅄ᐱ(Ln1-Zn1), ∈1-⅄ᐱ(Ln2n1), ∈1-⅄ᐱ(Ln2n1)),1-ᐱ(Ln2cn-n1cn), ∈1-ᐱ(Ln2cn-n1cn), ∈1-ᐱ(Ln2cn-∘⧊°n1cn), ∈1-ᐱ(Ln2cn-∘∇°n1cn)

1-⅄ᐱ(Mn2-An1), ∈1-⅄ᐱ(Mn2-Bn1), ∈1-⅄ᐱ(Mn2-Dn1), ∈1-⅄ᐱ(Mn2-En1), ∈1-⅄ᐱ(Mn2-Fn1), ∈1-⅄ᐱ(Mn2-Gn1), ∈1-⅄ᐱ(Mn2-Hn1), ∈1-⅄ᐱ(Mn2-In1), ∈1-⅄ᐱ(Mn2-Jn1), ∈1-⅄ᐱ(Mn2-Kn1), ∈1-⅄ᐱ(Mn2-Ln1), 1-ᐱ(Mn2-Mn1), ∈1-⅄ᐱ(Mn2-Nn1), ∈1-⅄ᐱ(Mn2-On1), ∈1-⅄ᐱ(Mn2-Pn1), ∈1-⅄ᐱ(Mn2-Qn1), ∈1-⅄ᐱ(Mn2-Rn1), ∈1-⅄ᐱ(Mn2-Sn1), ∈1-⅄ᐱ(Mn2-Tn1),∈1-⅄ᐱ(Mn2-Un1),  ∈1-⅄ᐱ(Mn2-Vn1), ∈1-⅄ᐱ(Mn2-Wn1), ∈1-⅄ᐱ(Mn2-Yn1), ∈1-⅄ᐱ(Mn2-Zn1), ∈1-⅄ᐱ(Mn2n1), ∈1-⅄ᐱ(Mn2n1),1-ᐱ(Mn2cn-n1cn), ∈1-ᐱ(Mn2cn-n1cn), ∈1-ᐱ(Mn2cn-∘⧊°n1cn), ∈1-ᐱ(Mn2cn-∘∇°n1cn)

1-⅄ᐱ(Nn2-An1), ∈1-⅄ᐱ(Nn2-Bn1), ∈1-⅄ᐱ(Nn2-Dn1), ∈1-⅄ᐱ(Nn2-En1), ∈1-⅄ᐱ(Nn2-Fn1), ∈1-⅄ᐱ(Nn2-Gn1), ∈1-⅄ᐱ(Nn2-Hn1), ∈1-⅄ᐱ(Nn2-In1), ∈1-⅄ᐱ(Nn2-Jn1), ∈1-⅄ᐱ(Nn2-Kn1), ∈1-⅄ᐱ(Nn2-Ln1), ∈1-⅄ᐱ(Nn2-Mn1), 1-ᐱ(Nn2-Nn1), ∈1-⅄ᐱ(Nn2-On1), ∈1-⅄ᐱ(Nn2-Pn1), ∈1-⅄ᐱ(Nn2-Qn1), ∈1-⅄ᐱ(Nn2-Rn1), ∈1-⅄ᐱ(Nn2-Sn1), ∈1-⅄ᐱ(Nn2-Tn1),∈1-⅄ᐱ(Nn2-Un1),  ∈1-⅄ᐱ(Nn2-Vn1), ∈1-⅄ᐱ(Nn2-Wn1), ∈1-⅄ᐱ(Nn2-Yn1), ∈1-⅄ᐱ(Nn2-Zn1), ∈1-⅄ᐱ(Nn2n1), ∈1-⅄ᐱ(Nn2n1),1-ᐱ(Nn2cn-n1cn), ∈1-ᐱ(Nn2cn-n1cn), ∈1-ᐱ(Nn2cn-∘⧊°n1cn), ∈1-ᐱ(Nn2cn-∘∇°n1cn)

1-⅄ᐱ(On2-An1), ∈1-⅄ᐱ(On2-Bn1), ∈1-⅄ᐱ(On2-Dn1), ∈1-⅄ᐱ(On2-En1), ∈1-⅄ᐱ(On2-Fn1), ∈1-⅄ᐱ(On2-Gn1), ∈1-⅄ᐱ(On2-Hn1), ∈1-⅄ᐱ(On2-In1), ∈1-⅄ᐱ(On2-Jn1), ∈1-⅄ᐱ(On2-Kn1), ∈1-⅄ᐱ(On2-Ln1), ∈1-⅄ᐱ(On2-Mn1), ∈1-⅄ᐱ(On2-Nn1), 1-ᐱ(On2-On1), ∈1-⅄ᐱ(On2-Pn1), ∈1-⅄ᐱ(On2-Qn1), ∈1-⅄ᐱ(On2-Rn1), ∈1-⅄ᐱ(On2-Sn1), ∈1-⅄ᐱ(On2-Tn1),∈1-⅄ᐱ(On2-Un1),  ∈1-⅄ᐱ(On2-Vn1), ∈1-⅄ᐱ(On2-Wn1), ∈1-⅄ᐱ(On2-Yn1), ∈1-⅄ᐱ(On2-Zn1), ∈1-⅄ᐱ(On2n1), ∈1-⅄ᐱ(On2n1),1-ᐱ(On2cn-n1cn), ∈1-ᐱ(On2cn-n1cn), ∈1-ᐱ(On2cn-∘⧊°n1cn), ∈1-ᐱ(On2cn-∘∇°n1cn)

1-⅄ᐱ(Pn2-An1), ∈1-⅄ᐱ(Pn2-Bn1), ∈1-⅄ᐱ(Pn2-Dn1), ∈1-⅄ᐱ(Pn2-En1), ∈1-⅄ᐱ(Pn2-Fn1), ∈1-⅄ᐱ(Pn2-Gn1), ∈1-⅄ᐱ(Pn2-Hn1), ∈1-⅄ᐱ(Pn2-In1), ∈1-⅄ᐱ(Pn2-Jn1), ∈1-⅄ᐱ(Pn2-Kn1), ∈1-⅄ᐱ(Pn2-Ln1), ∈1-⅄ᐱ(Pn2-Mn1), ∈1-⅄ᐱ(Pn2-Nn1), ∈1-⅄ᐱ(Pn2-On1), 1-ᐱ(Pn2-Pn1), ∈1-⅄ᐱ(Pn2-Qn1), ∈1-⅄ᐱ(Pn2-Rn1), ∈1-⅄ᐱ(Pn2-Sn1), ∈1-⅄ᐱ(Pn2-Tn1),∈1-⅄ᐱ(Pn2-Un1),  ∈1-⅄ᐱ(Pn2-Vn1), ∈1-⅄ᐱ(Pn2-Wn1), ∈1-⅄ᐱ(Pn2-Yn1), ∈1-⅄ᐱ(Pn2-Zn1), ∈1-⅄ᐱ(Pn2n1), ∈1-⅄ᐱ(Pn2n1),1-ᐱ(Pn2cn-n1cn), ∈1-ᐱ(Pn2cn-n1cn), ∈1-ᐱ(Pn2cn-∘⧊°n1cn), ∈1-ᐱ(Pn2cn-∘∇°n1cn)

1-⅄ᐱ(Qn2-An1), ∈1-⅄ᐱ(Qn2-Bn1), ∈1-⅄ᐱ(Qn2-Dn1), ∈1-⅄ᐱ(Qn2-En1), ∈1-⅄ᐱ(Qn2-Fn1), ∈1-⅄ᐱ(Qn2-Gn1), ∈1-⅄ᐱ(Qn2-Hn1), ∈1-⅄ᐱ(Qn2-In1), ∈1-⅄ᐱ(Qn2-Jn1), ∈1-⅄ᐱ(Qn2-Kn1), ∈1-⅄ᐱ(Qn2-Ln1), ∈1-⅄ᐱ(Qn2-Mn1), ∈1-⅄ᐱ(Qn2-Nn1), ∈1-⅄ᐱ(Qn2-On1), ∈1-⅄ᐱ(Qn2-Pn1), 1-ᐱ(Qn2-Qn1), ∈1-⅄ᐱ(Qn2-Rn1), ∈1-⅄ᐱ(Qn2-Sn1), ∈1-⅄ᐱ(Qn2-Tn1), ∈1-⅄ᐱ(Qn2-Un1),  ∈1-⅄ᐱ(Qn2-Vn1), ∈1-⅄ᐱ(Qn2-Wn1), ∈1-⅄ᐱ(Qn2-Yn1), ∈1-⅄ᐱ(Qn2-Zn1), ∈1-⅄ᐱ(Qn2n1), ∈1-⅄ᐱ(Qn2n1),1-ᐱ(Qn2cn-n1cn), ∈1-ᐱ(Qn2cn-n1cn), ∈1-ᐱ(Qn1cn-∘⧊°n1cn), ∈1-ᐱ(Qn2cn-∘∇°n1cn)

1-⅄ᐱ(Rn2-An1), ∈1-⅄ᐱ(Rn2-Bn1), ∈1-⅄ᐱ(Rn2-Dn1), ∈1-⅄ᐱ(Rn2-En1), ∈1-⅄ᐱ(Rn2-Fn1), ∈1-⅄ᐱ(Rn2-Gn1), ∈1-⅄ᐱ(Rn2-Hn1), ∈1-⅄ᐱ(Rn2-In1), ∈1-⅄ᐱ(Rn2-Jn1), ∈1-⅄ᐱ(Rn2-Kn1), ∈1-⅄ᐱ(Rn2-Ln1), ∈1-⅄ᐱ(Rn2-Mn1), ∈1-⅄ᐱ(Rn2-Nn1), ∈1-⅄ᐱ(Rn2-On1), ∈1-⅄ᐱ(Rn2-Pn1), ∈1-⅄ᐱ(Rn2-Qn1), 1-ᐱ(Rn2-Rn1), ∈1-⅄ᐱ(Rn2-Sn1), ∈1-⅄ᐱ(Rn2-Tn1),∈1-⅄ᐱ(Rn2-Un1),  ∈1-⅄ᐱ(Rn2-Vn1), ∈1-⅄ᐱ(Rn2-Wn1), ∈1-⅄ᐱ(Rn2-Yn1), ∈1-⅄ᐱ(Rn2-Zn1), ∈1-⅄ᐱ(Rn2n1), ∈1-⅄ᐱ(Rn2n1),1-ᐱ(Rn2cn-n1cn), ∈1-ᐱ(Rn2cn-n1cn), ∈1-ᐱ(Rn2cn-∘⧊°n1cn), ∈1-ᐱ(Rn2cn-∘∇°n1cn)

1-⅄ᐱ(Sn2-An1), ∈1-⅄ᐱ(Sn2-Bn1), ∈1-⅄ᐱ(Sn2-Dn1), ∈1-⅄ᐱ(Sn2-En1), ∈1-⅄ᐱ(Sn2-Fn1), ∈1-⅄ᐱ(Sn2-Gn1), ∈1-⅄ᐱ(Sn2-Hn1), ∈1-⅄ᐱ(Sn2-In1), ∈1-⅄ᐱ(Sn2-Jn1), ∈1-⅄ᐱ(Sn2-Kn1), ∈1-⅄ᐱ(Sn2-Ln1), ∈1-⅄ᐱ(Sn2-Mn1), ∈1-⅄ᐱ(Sn2-Nn1), ∈1-⅄ᐱ(Sn2-On1), ∈1-⅄ᐱ(Sn2-Pn1), ∈1-⅄ᐱ(Sn2-Qn1), ∈1-⅄ᐱ(Sn2-Rn1), 1-ᐱ(Sn2-Sn1), ∈1-⅄ᐱ(Sn2-Tn1),∈1-⅄ᐱ(Sn2-Un1),  ∈1-⅄ᐱ(Sn2-Vn1), ∈1-⅄ᐱ(Sn2-Wn1), ∈1-⅄ᐱ(Sn2-Yn1), ∈1-⅄ᐱ(Sn2-Zn1), ∈1-⅄ᐱ(Sn2n1), ∈1-⅄ᐱ(Sn2n1),1-ᐱ(Sn2cn-n1cn), ∈1-ᐱ(Sn2cn-n1cn), ∈1-ᐱ(Sn2cn-∘⧊°n1cn), ∈1-ᐱ(Sn2cn-∘∇°n1cn)

1-⅄ᐱ(Tn2-An1), ∈1-⅄ᐱ(Tn2-Bn1), ∈1-⅄ᐱ(Tn2-Dn1), ∈1-⅄ᐱ(Tn2-En1), ∈1-⅄ᐱ(Tn2-Fn1), ∈1-⅄ᐱ(Tn2-Gn1), ∈1-⅄ᐱ(Tn2-Hn1), ∈1-⅄ᐱ(Tn2-In1), ∈1-⅄ᐱ(Tn2-Jn1), ∈1-⅄ᐱ(Tn2-Kn1), ∈1-⅄ᐱ(Tn2-Ln1), ∈1-⅄ᐱ(Tn2-Mn1), ∈1-⅄ᐱ(Tn2-Nn1), ∈1-⅄ᐱ(Tn2-On1), ∈1-⅄ᐱ(Tn2-Pn1), ∈1-⅄ᐱ(Tn2-Qn1), ∈1-⅄ᐱ(Tn2-Rn1), ∈1-⅄ᐱ(Tn2-Sn1), 1-ᐱ(Tn2-Tn1),∈1-⅄ᐱ(Tn2-Un1),  ∈1-⅄ᐱ(Tn2-Vn1), ∈1-⅄ᐱ(Tn2-Wn1), ∈1-⅄ᐱ(Tn2-Yn1), ∈1-⅄ᐱ(Tn2-Zn1), ∈1-⅄ᐱ(Tn2n1), ∈1-⅄ᐱ(Tn2n1),1-ᐱ(Tn2cn-n1cn), ∈1-ᐱ(Tn2cn-n1cn), ∈1-ᐱ(Tn2cn-∘⧊°n1cn), ∈1-ᐱ(Tn2cn-∘∇°n1cn)

1-⅄ᐱ(Un2-An1), ∈1-⅄ᐱ(Un2-Bn1), ∈1-⅄ᐱ(Un2-Dn1), ∈1-⅄ᐱ(Un2-En1), ∈1-⅄ᐱ(Un2-Fn1), ∈1-⅄ᐱ(Un2-Gn1), ∈1-⅄ᐱ(Un1-Hn1), ∈1-⅄ᐱ(Un1-In1), ∈1-⅄ᐱ(Un2-Jn1), ∈1-⅄ᐱ(Un2-Kn1), ∈1-⅄ᐱ(Un2-Ln1), ∈1-⅄ᐱ(Un2-Mn1), ∈1-⅄ᐱ(Un2-Nn1), ∈1-⅄ᐱ(Un2-On1), ∈1-⅄ᐱ(Un1-Pn1), ∈1-⅄ᐱ(Un2-Qn1), ∈n1-⅄ᐱ(Un2-Rn1), ∈1-⅄ᐱ(Un2-Sn1), ∈1-⅄ᐱ(Un2-Tn1), 1-ᐱ(Un2-Un1),  ∈1-⅄ᐱ(Un2-Vn1), ∈1-⅄ᐱ(Un2-Wn1), ∈1-⅄ᐱ(Un2-Yn1), ∈1-⅄ᐱ(Un2-Zn1), ∈1-⅄ᐱ(Un2n1), ∈1-⅄ᐱ(Un2n1),1-ᐱ(Un2cn-n1cn), ∈1-ᐱ(Un2cn-n1cn), ∈1-ᐱ(Un2cn-∘⧊°n1cn), ∈1-ᐱ(Un2cn-∘∇°n1cn)

1-⅄ᐱ(Vn2-An1), ∈1-⅄ᐱ(Vn2-Bn1), ∈1-⅄ᐱ(Vn2-Dn1), ∈1-⅄ᐱ(Vn2-En1), ∈1-⅄ᐱ(Vn2-Fn1), ∈1-⅄ᐱ(Vn2-Gn1), ∈1-⅄ᐱ(Vn2-Hn1), ∈1-⅄ᐱ(Vn2-In1), ∈1-⅄ᐱ(Vn2-Jn1), ∈1-⅄ᐱ(Vn2-Kn1), ∈1-⅄ᐱ(Vn2-Ln1), ∈1-⅄ᐱ(Vn2-Mn1), ∈1-⅄ᐱ(Vn2-Nn1), ∈1-⅄ᐱ(Vn2-On1), ∈1-⅄ᐱ(Vn2-Pn1), ∈1-⅄ᐱ(Vn2-Qn1), ∈1-⅄ᐱ(Vn2-Rn1), ∈1-⅄ᐱ(Vn2-Sn1), ∈1-⅄ᐱ(Vn2-Tn1),∈1-⅄ᐱ(Vn2-Un1),  1-ᐱ(Vn2-Vn1), ∈1-⅄ᐱ(Vn2-Wn1), ∈1-⅄ᐱ(Vn2-Yn1), ∈1-⅄ᐱ(Vn2-Zn1), ∈1-⅄ᐱ(Vn2n1), ∈1-⅄ᐱ(Vn2n1),1-ᐱ(Vn2cn-n1cn), ∈1-ᐱ(Vn2cn-n1cn), ∈1-ᐱ(Vn2cn-∘⧊°n1cn), ∈1-ᐱ(Vn2cn-∘∇°n1cn)

1-⅄ᐱ(Wn2-An1), ∈1-⅄ᐱ(Wn2-Bn1), ∈1-⅄ᐱ(Wn2-Dn1), ∈1-⅄ᐱ(Wn2-En1), ∈1-⅄ᐱ(Wn2-Fn1), ∈1-⅄ᐱ(Wn2-Gn1), ∈1-⅄ᐱ(Wn2-Hn1), ∈1-⅄ᐱ(Wn2-In1), ∈1-⅄ᐱ(Wn2-Jn1), ∈1-⅄ᐱ(Wn2-Kn1), ∈1-⅄ᐱ(Wn2-Ln1), ∈1-⅄ᐱ(Wn2-Mn1), ∈1-⅄ᐱ(Wn2-Nn1), ∈1-⅄ᐱ(Wn2-On1), ∈1-⅄ᐱ(Wn2-Pn1), ∈1-⅄ᐱ(Wn2-Qn1), ∈1-⅄ᐱ(Wn2-Rn1), ∈1-⅄ᐱ(Wn2-Sn1), ∈1-⅄ᐱ(Wn2-Tn1),∈1-⅄ᐱ(Wn2-Un1),  ∈1-⅄ᐱ(Wn2-Vn1), 1-ᐱ(Wn2-Wn1), ∈1-⅄ᐱ(Wn2-Yn1), ∈1-⅄ᐱ(Wn2-Zn1), ∈1-⅄ᐱ(Wn2n1), ∈1-⅄ᐱ(Wn2n1),1-ᐱ(Wn2cn-n1cn), ∈1-ᐱ(Wn2cn-n1cn), ∈1-ᐱ(Wn2cn-∘⧊°n1cn), ∈1-ᐱ(Wn2cn-∘∇°n1cn)

1-⅄ᐱ(Yn2-An1), ∈1-⅄ᐱ(Yn2-Bn1), ∈1-⅄ᐱ(Yn2-Dn1), ∈1-⅄ᐱ(Yn2-En1), ∈1-⅄ᐱ(Yn2-Fn1), ∈1-⅄ᐱ(Yn2-Gn1), ∈1-⅄ᐱ(Yn2-Hn1), ∈1-⅄ᐱ(Yn2-In1), ∈1-⅄ᐱ(Yn2-Jn1), ∈1-⅄ᐱ(Yn2-Kn1), ∈1-⅄ᐱ(Yn2-Ln1), ∈1-⅄ᐱ(Yn2-Mn1), ∈1-⅄ᐱ(Yn2-Nn1), ∈1-⅄ᐱ(Yn2-On1), ∈1-⅄ᐱ(Yn2-Pn1), ∈1-⅄ᐱ(Yn2-Qn1), ∈1-⅄ᐱ(Yn2-Rn1), ∈1-⅄ᐱ(Yn2-Sn1), ∈1-⅄ᐱ(Yn2-Tn1),∈1-⅄ᐱ(Yn2-Un1),  ∈1-⅄ᐱ(Yn2-Vn1), ∈1-⅄ᐱ(Yn2-Wn1), 1-ᐱ(Yn2-Yn1), ∈1-⅄ᐱ(Yn2-Zn1), ∈1-⅄ᐱ(Yn2n1), ∈1-⅄ᐱ(Yn2n1),1-ᐱ(Yn2cn-n1cn), ∈1-ᐱ(Yn2cn-n1cn), ∈1-ᐱ(Yn2cn-∘⧊°n1cn), ∈1-ᐱ(Yn2cn-∘∇°n1cn)

1-⅄ᐱ(Zn2-An1), ∈1-⅄ᐱ(Zn2-Bn1), ∈1-⅄ᐱ(Zn2-Dn1), ∈1-⅄ᐱ(Zn2-En1), ∈1-⅄ᐱ(Zn2-Fn1), ∈1-⅄ᐱ(Zn2-Gn1), ∈1-⅄ᐱ(Zn2-Hn1), ∈1-⅄ᐱ(Zn2-In1), ∈1-⅄ᐱ(Zn2-Jn1), ∈1-⅄ᐱ(Zn2-Kn1), ∈1-⅄ᐱ(Zn2-Ln1), ∈1-⅄ᐱ(Zn2-Mn1), ∈1-⅄ᐱ(Zn2-Nn1), ∈1-⅄ᐱ(Zn2-On1), ∈1-⅄ᐱ(Zn2-Pn1), ∈1-⅄ᐱ(Zn2-Qn1), ∈1-⅄ᐱ(Zn2-Rn1), ∈1-⅄ᐱ(Zn2-Sn1), ∈1-⅄ᐱ(Zn2-Tn1),∈1-⅄ᐱ(Zn2-Un1),  ∈1-⅄ᐱ(Zn2-Vn1), ∈1-⅄ᐱ(Zn2-Wn1), ∈1-⅄ᐱ(Zn2-Yn1), 1-ᐱ(Zn2-Zn1), ∈1-⅄ᐱ(Zn2n1), ∈1-⅄ᐱ(Zn2n1),1-ᐱ(Zn2cn-n1cn), ∈1-ᐱ(Zn2cn-n1cn), ∈1-ᐱ(Zn2cn-∘⧊°n1cn), ∈1-ᐱ(Zn2cn-∘∇°n1cn)

1-⅄ᐱ(φn2-An1), ∈1-⅄ᐱ(φn2-Bn1), ∈1-⅄ᐱ(φn2-Dn1), ∈1-⅄ᐱ(φn2-En1), ∈1-⅄ᐱ(φn2-Fn1), ∈1-⅄ᐱ(φn2-Gn1), ∈1-⅄ᐱ(φn2-Hn1), ∈1-⅄ᐱ(φn2-In1), ∈1-⅄ᐱ(φn2-Jn1), ∈1-⅄ᐱ(φn2-Kn1), ∈1-⅄ᐱ(φn2-Ln1), ∈1-⅄ᐱ(φn2-Mn1), ∈1-⅄ᐱ(φn2-Nn1), ∈1-⅄ᐱ(φn2-On1), ∈1-⅄ᐱ(φn2-Pn1), ∈1-⅄ᐱ(φn2-Qn1), ∈1-⅄ᐱ(φn2-Rn1), ∈1-⅄ᐱ(φn2-Sn1), ∈1-⅄ᐱ(φn2-Tn1),∈1-⅄ᐱ(φn2-Un1),  ∈1-⅄ᐱ(φn2-Vn1), ∈1-⅄ᐱ(φn2-Wn1), ∈1-⅄ᐱ(φn2-Yn1), ∈1-⅄ᐱ(φn2-Zn1), 1-ᐱ(φn2-φn1), ∈1-⅄ᐱ(φn2n1),1-ᐱ(φn2cn-n1cn), ∈1-ᐱ(φn2cn-n1cn), ∈1-ᐱ(φn2cn-∘⧊°n1cn), ∈1-ᐱ(φn2cn-∘∇°n1cn)

1-⅄ᐱ(Θn2-An1), ∈1-⅄ᐱ(Θn2-Bn1), ∈1-⅄ᐱ(Θn2-Dn1), ∈1-⅄ᐱ(Θn2-En1), ∈1-⅄ᐱ(Θn2-Fn1), ∈1-⅄ᐱ(Θn2-Gn1), ∈1-⅄ᐱ(Θn2-Hn1), ∈1-⅄ᐱ(Θn2-In1), ∈1-⅄ᐱ(Θn2-Jn1), ∈1-⅄ᐱ(Θn2-Kn1), ∈1-⅄ᐱ(Θn2-Ln1), ∈1-⅄ᐱ(Θn2-Mn1), ∈1-⅄ᐱ(Θn2-Nn1), ∈1-⅄ᐱ(Θn2-On1), ∈1-⅄ᐱ(Θn2-Pn1), ∈1-⅄ᐱ(Θn2-Qn1), ∈1-⅄ᐱ(Θn2-Rn1), ∈1-⅄ᐱ(Θn2-Sn1), ∈1-⅄ᐱ(Θn2-Tn1),∈1-⅄ᐱ(Θn2-Un1),  ∈1-⅄ᐱ(Θn2-Vn1), ∈1-⅄ᐱ(Θn2-Wn1), ∈1-⅄ᐱ(Θn2-Yn1), ∈1-⅄ᐱ(Θn2-Zn1), ∈1-⅄ᐱ(Θn2n1), 1-ᐱ(Θn2-Θn1), ∈1-ᐱ(Θn2cn-n1cn), ∈1-ᐱ(Θn2cn-n1cn), ∈1-ᐱ(Θn2cn-∘⧊°n1cn), ∈1-ᐱ(Θn2cn-∘∇°n1cn)

2-⅄=(n1-n2)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

2-⅄=(n1-n2) that a function path is factored to the definition of the function path rather than pemdas order of operations.

Variables are factorable to a measured units that then be later can applied in functions of proper order of operations that is parenthesis, exponents, multiplication, division, addition, and then subtraction. 

Function path  2-⅄=(n1-n2)is nn1cn previous number in a set of consecutive variables minus nn2cn later number in a set of consecutive variables, such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant.

2-ᐱ(An1-An2), ∈2-⅄ᐱ(An1-Bn2), ∈2-⅄ᐱ(An1-Dn2), ∈2-⅄ᐱ(An1-En2), ∈2-⅄ᐱ(An1-Fn2), ∈2-⅄ᐱ(An1-Gn2), ∈2-⅄ᐱ(An1-Hn2), ∈2-⅄ᐱ(An1-In2), ∈2-⅄ᐱ(An1-Jn2), ∈2-⅄ᐱ(An1-Kn2), ∈2-⅄ᐱ(An1-Ln2), ∈2-⅄ᐱ(An1-Mn2), ∈2-⅄ᐱ(An1-Nn2), ∈2-⅄ᐱ(An1-On2), ∈2-⅄ᐱ(An1-Pn2), ∈2-⅄ᐱ(An1-Qn2), ∈2-⅄ᐱ(An1-Rn2), ∈2-⅄ᐱ(An1-Sn2), ∈2-⅄ᐱ(An1-Tn2), ∈2-⅄ᐱ(An1-Un2),  ∈2-⅄ᐱ(An1-Vn2), ∈2-⅄ᐱ(An1-Wn2), ∈2-⅄ᐱ(An1-Yn2), ∈2-⅄ᐱ(An1-Zn2), ∈2-⅄ᐱ(An1-φn2), ∈2-⅄ᐱ(An1-Θn2), 2-ᐱ(An1cn-n2cn), ∈2-ᐱ(An1cn-n2cn), ∈2-ᐱ(An1cn-∘⧊°n2cn), ∈2-ᐱ(An1cn-∘∇°n2cn)

2-⅄ᐱ(Bn1-An2), 2-ᐱ(Bn1-Bn2), ∈2-⅄ᐱ(Bn1-Dn2), ∈2-⅄ᐱ(Bn1-En2), ∈2-⅄ᐱ(Bn1-Fn2), ∈2-⅄ᐱ(Bn1-Gn2), ∈2-⅄ᐱ(Bn1-Hn2), ∈2-⅄ᐱ(Bn1-In2), ∈2-⅄ᐱ(Bn1-Jn2), ∈2-⅄ᐱ(Bn1-Kn2), ∈2-⅄ᐱ(Bn1-Ln2), ∈2-⅄ᐱ(Bn1-Mn2), ∈2-⅄ᐱ(Bn1-Nn2), ∈2-⅄ᐱ(Bn1-On2), ∈2-⅄ᐱ(Bn1-Pn2), ∈2-⅄ᐱ(Bn1-Qn2), ∈2-⅄ᐱ(Bn1-Rn2), ∈2-⅄ᐱ(Bn1-Sn2), ∈2-⅄ᐱ(Bn1-Tn2),∈2-⅄ᐱ(Bn1-Un2),  ∈2-⅄ᐱ(Bn1-Vn2), ∈2-⅄ᐱ(Bn1-Wn2), ∈2-⅄ᐱ(Bn1-Yn2), ∈2-⅄ᐱ(Bn1-Zn2), ∈2-⅄ᐱ(Bn1-φn2), ∈2-⅄ᐱ(Bn1-Θn2),2-ᐱ(Bn1cn-n2cn), ∈2-ᐱ(Bn1cn-n2cn), ∈2-ᐱ(Bn1cn-∘⧊°n2cn), ∈2-ᐱ(Bn1cn-∘∇°n2cn)

2-⅄ᐱ(Dn1-An2), ∈2-⅄ᐱ(Dn1-Bn2), 2-ᐱ(Dn1-Dn2), ∈2-⅄ᐱ(Dn1-En2), ∈2-⅄ᐱ(Dn1-Fn2), ∈2-⅄ᐱ(Dn1-Gn2), ∈2-⅄ᐱ(Dn1-Hn2), ∈2-⅄ᐱ(Dn1-In2), ∈2-⅄ᐱ(Dn1-Jn2), ∈2-⅄ᐱ(Dn1-Kn2), ∈2-⅄ᐱ(Dn1-Ln2), ∈2-⅄ᐱ(Dn1-Mn2), ∈2-⅄ᐱ(Dn1-Nn2), ∈2-⅄ᐱ(Dn1-On2), ∈2-⅄ᐱ(Dn1-Pn2), ∈2-⅄ᐱ(Dn1-Qn2), ∈2-⅄ᐱ(Dn1-Rn2), ∈2-⅄ᐱ(Dn1-Sn2), ∈2-⅄ᐱ(Dn1-Tn2),∈2-⅄ᐱ(Dn1-Un2),  ∈2-⅄ᐱ(Dn1-Vn2), ∈2-⅄ᐱ(Dn1-Wn2), ∈2-⅄ᐱ(Dn1-Yn2), ∈2-⅄ᐱ(Dn1-Zn2), ∈2-⅄ᐱ(Dn1-φn2), ∈2-⅄ᐱ(Dn1-Θn2), 2-ᐱ(Dn1cn-n2cn), ∈2-ᐱ(Dn1cn-n2cn), ∈2-ᐱ(Dn1cn-∘⧊°n2cn), ∈2-ᐱ(Dn1cn-∘∇°n2cn)

2-⅄ᐱ(En1-An2), ∈2-⅄ᐱ(En1-Bn2), ∈2-⅄ᐱ(En1-Dn2), 2-ᐱ(En1-En2), ∈2-⅄ᐱ(En1-Fn2), ∈2-⅄ᐱ(En1-Gn2), ∈2-⅄ᐱ(En1-Hn2), ∈2-⅄ᐱ(En1-In2), ∈2-⅄ᐱ(En1-Jn2), ∈2-⅄ᐱ(En1-Kn2), ∈2-⅄ᐱ(En1-Ln2), ∈2-⅄ᐱ(En1-Mn2), ∈2-⅄ᐱ(En1-Nn2), ∈2-⅄ᐱ(En1-On2), ∈2-⅄ᐱ(En1-Pn2), ∈2-⅄ᐱ(En1-Qn2), ∈2-⅄ᐱ(En1-Rn2), ∈2-⅄ᐱ(En1-Sn2), ∈2-⅄ᐱ(En1-Tn2),∈2-⅄ᐱ(En1-Un2),  ∈2-⅄ᐱ(En1-Vn2), ∈2-⅄ᐱ(En1-Wn2), ∈2-⅄ᐱ(En1-Yn2), ∈2-⅄ᐱ(En1-Zn2), ∈2-⅄ᐱ(En1-φn2), ∈2-⅄ᐱ(En1-Θn2),2-ᐱ(En1cn-n2cn), ∈2-ᐱ(En1cn-n2cn), ∈2-ᐱ(En1cn-∘⧊°n2cn), ∈2-ᐱ(En1cn-∘∇°n2cn)

2-⅄ᐱ(Fn1-An2), ∈2-⅄ᐱ(Fn1-Bn2), ∈2-⅄ᐱ(Fn1-Dn2), ∈2-⅄ᐱ(Fn1-En2), 2-ᐱ(Fn1-Fn2), ∈2-⅄ᐱ(Fn1-Gn2), ∈2-⅄ᐱ(Fn1-Hn2), ∈2-⅄ᐱ(Fn1-In2), ∈2-⅄ᐱ(Fn1-Jn2), ∈2-⅄ᐱ(Fn1-Kn2), ∈2-⅄ᐱ(Fn1-Ln2), ∈2-⅄ᐱ(Fn1-Mn2), ∈2-⅄ᐱ(Fn1-Nn2), ∈2-⅄ᐱ(Fn1-On2), ∈2-⅄ᐱ(Fn1-Pn2), ∈2-⅄ᐱ(Fn1-Qn2), ∈2-⅄ᐱ(Fn1-Rn2), ∈2-⅄ᐱ(Fn1-Sn2), ∈2-⅄ᐱ(Fn1-Tn2),∈2-⅄ᐱ(Fn1-Un2),  ∈2-⅄ᐱ(Fn1-Vn2), ∈2-⅄ᐱ(Fn1-Wn2), ∈2-⅄ᐱ(Fn1-Yn2), ∈2-⅄ᐱ(Fn1-Zn2), ∈2-⅄ᐱ(Fn1-φn2), ∈2-⅄ᐱ(Fn1-Θn2),2-ᐱ(Fn1cn-n2cn), ∈2-ᐱ(Fn1cn-n2cn), ∈2-ᐱ(Fn1cn-∘⧊°n2cn), ∈2-ᐱ(Fn1cn-∘∇°n2cn)

2-⅄ᐱ(Gn1-An2), ∈2-⅄ᐱ(Gn1-Bn2), ∈2-⅄ᐱ(Gn1-Dn2), ∈2-⅄ᐱ(Gn1-En2), ∈2-⅄ᐱ(Gn1-Fn2), 2-ᐱ(Gn1-Gn2), ∈2-⅄ᐱ(Gn1-Hn2), ∈2-⅄ᐱ(Gn1-In2), ∈2-⅄ᐱ(Gn1-Jn2), ∈2-⅄ᐱ(Gn1-Kn2), ∈2-⅄ᐱ(Gn1-Ln2), ∈2-⅄ᐱ(Gn1-Mn2), ∈2-⅄ᐱ(Gn1-Nn2), ∈2-⅄ᐱ(Gn1-On2), ∈2-⅄ᐱ(Gn1-Pn2), ∈2-⅄ᐱ(Gn1-Qn2), ∈2-⅄ᐱ(Gn1-Rn2), ∈2-⅄ᐱ(Gn1-Sn2), ∈2-⅄ᐱ(Gn1-Tn2),∈2-⅄ᐱ(Gn1-Un2),  ∈2-⅄ᐱ(Gn1-Vn2), ∈2-⅄ᐱ(Gn1-Wn2), ∈2-⅄ᐱ(Gn1-Yn2), ∈2-⅄ᐱ(Gn1-Zn2), ∈2-⅄ᐱ(Gn1-φn2), ∈2-⅄ᐱ(Gn1-Θn2),2-ᐱ(Gn1cn-n2cn), ∈2-ᐱ(Gn1cn-n2cn), ∈2-ᐱ(Gn1cn-∘⧊°n2cn), ∈2-ᐱ(Gn1cn-∘∇°n2cn)

2-⅄ᐱ(Hn1-An2), ∈2-⅄ᐱ(Hn1-Bn2), ∈2-⅄ᐱ(Hn1-Dn2), ∈2-⅄ᐱ(Hn1-En2), ∈2-⅄ᐱ(Hn1-Fn2), ∈2-⅄ᐱ(Hn1-Gn2), 2-ᐱ(Hn1-Hn2), ∈2-⅄ᐱ(Hn1-In2), ∈2-⅄ᐱ(Hn1-Jn2), ∈2-⅄ᐱ(Hn1-Kn2), ∈2-⅄ᐱ(Hn1-Ln2), ∈2-⅄ᐱ(Hn1-Mn2), ∈2-⅄ᐱ(Hn1-Nn2), ∈2-⅄ᐱ(Hn1-On2), ∈2-⅄ᐱ(Hn1-Pn2), ∈2-⅄ᐱ(Hn1-Qn2), ∈2-⅄ᐱ(Hn1-Rn2), ∈2-⅄ᐱ(Hn1-Sn2), ∈2-⅄ᐱ(Hn1-Tn2), ∈2-⅄ᐱ(Hn1-Un2),  ∈2-⅄ᐱ(Hn1-Vn2), ∈2-⅄ᐱ(Hn1-Wn2), ∈2-⅄ᐱ(Hn1-Yn2), ∈2-⅄ᐱ(Hn1-Zn2), ∈2-⅄ᐱ(Hn1-φn2), ∈2-⅄ᐱ(Hn1-Θn2),2-ᐱ(Hn1cn-n2cn), ∈2-⅄Xᐱ(Hn1cn-n2cn), ∈2-ᐱ(Hn1cn-∘⧊°n2cn), ∈2-ᐱ(Hn1cn-∘∇°n2cn)

2-⅄ᐱ(In1-An2), ∈2-⅄ᐱ(In1-Bn2), ∈2-⅄ᐱ(In1-Dn2), ∈2-⅄ᐱ(In1-En2), ∈2-⅄ᐱ(In1-Fn2), ∈2-⅄ᐱ(In1-Gn2), ∈2-⅄ᐱ(In1-Hn2), 2-ᐱ(In1-In2), ∈2-⅄ᐱ(In1-Jn2), ∈2-⅄ᐱ(In1-Kn2), ∈2-⅄ᐱ(In1-Ln2), ∈2-⅄ᐱ(In1-Mn2), ∈2-⅄ᐱ(In1-Nn2), ∈2-⅄ᐱ(In1-On2), ∈2-⅄ᐱ(In1-Pn2), ∈2-⅄ᐱ(In1-Qn2), ∈2-⅄ᐱ(In1-Rn2), ∈2-⅄ᐱ(In1-Sn2), ∈2-⅄ᐱ(In1-Tn2),∈2-⅄ᐱ(In1-Un2),  ∈2-⅄ᐱ(In1-Vn2), ∈2-⅄ᐱ(In1-Wn2), ∈2-⅄ᐱ(In1-Yn2), ∈2-⅄ᐱ(In1-Zn2), ∈2-⅄ᐱ(In1-φn2), ∈2-⅄ᐱ(In1-Θn2),2-ᐱ(In1cn-n2cn), ∈2-ᐱ(In1cn-n2cn), ∈2-ᐱ(In1cn-∘⧊°n2cn), ∈2-ᐱ(In1cn-∘∇°n2cn)

2-⅄ᐱ(Jn1-An2), ∈2-⅄ᐱ(Jn1-Bn2), ∈2-⅄ᐱ(Jn1-Dn2), ∈2-⅄ᐱ(Jn1-En2), ∈2-⅄ᐱ(Jn1-Fn2), ∈2-⅄ᐱ(Jn1-Gn2), ∈2-⅄ᐱ(Jn1-Hn2), ∈2-⅄ᐱ(Jn1-In2), 2-ᐱ(Jn1-Jn2), ∈2-⅄ᐱ(Jn1-Kn2), ∈2-⅄ᐱ(Jn1-Ln2), ∈2-⅄ᐱ(Jn1-Mn2), ∈2-⅄ᐱ(Jn1-Nn2), ∈2-⅄ᐱ(Jn1-On2), ∈2-⅄ᐱ(Jn1-Pn2), ∈2-⅄ᐱ(Jn1-Qn2), ∈2-⅄ᐱ(Jn1-Rn2), ∈2-⅄ᐱ(Jn1-Sn2), ∈2-⅄ᐱ(Jn1-Tn2),∈2-⅄ᐱ(Jn1-Un2),  ∈2-⅄ᐱ(Jn1-Vn2), ∈2-⅄ᐱ(Jn1-Wn2), ∈2-⅄ᐱ(Jn1-Yn2), ∈2-⅄ᐱ(Jn1-Zn2), ∈2-⅄ᐱ(Jn1-φn2), ∈2-⅄ᐱ(Jn1-Θn2),2-ᐱ(Jn1cn-n2cn), ∈2-ᐱ(Jn1cn-n2cn), ∈2-ᐱ(Jn1cn-∘⧊°n2cn), ∈2-ᐱ(Jn1cn-∘∇°n2cn)

2-⅄ᐱ(Kn1-An2), ∈2-⅄ᐱ(Kn1-Bn2), ∈2-⅄ᐱ(Kn1-Dn2), ∈2-⅄ᐱ(Kn1-En2), ∈2-⅄ᐱ(Kn1-Fn2), ∈2-⅄ᐱ(Kn1-Gn2), ∈2-⅄ᐱ(Kn1-Hn2), ∈2-⅄ᐱ(Kn1-In2), ∈2-⅄ᐱ(Kn1-Jn2), 2-ᐱ(Kn1-Kn2), ∈2-⅄ᐱ(Kn1-Ln2), ∈2-⅄ᐱ(Kn1-Mn2), ∈2-⅄ᐱ(Kn1-Nn2), ∈2-⅄ᐱ(Kn1-On2), ∈2-⅄ᐱ(Kn1-Pn2), ∈2-⅄ᐱ(Kn1-Qn2), ∈2-⅄ᐱ(Kn1-Rn2), ∈2-⅄ᐱ(Kn1-Sn2), ∈2-⅄ᐱ(Kn1-Tn2),∈2-⅄ᐱ(Kn1-Un2),  ∈2-⅄ᐱ(Kn1-Vn2), ∈2-⅄ᐱ(Kn1-Wn2), ∈2-⅄ᐱ(Kn1-Yn2), ∈2-⅄ᐱ(Kn1-Zn2), ∈2-⅄ᐱ(Kn1-φn2), ∈2-⅄ᐱ(Kn1-Θn2),2-ᐱ(Kn1cn-n2cn), ∈2-ᐱ(Kn1cn-n2cn), ∈2-ᐱ(Kn1cn-∘⧊°n2cn), ∈2-ᐱ(Kn1cn-∘∇°n2cn)

2-⅄ᐱ(Ln1-An2), ∈2-⅄ᐱ(Ln1-Bn2), ∈2-⅄ᐱ(Ln1-Dn2), ∈2-⅄ᐱ(Ln1-En2), ∈2-⅄ᐱ(Ln1-Fn2), ∈2-⅄ᐱ(Ln1-Gn2), ∈2-⅄ᐱ(Ln1-Hn2), ∈2-⅄ᐱ(Ln1-In2), ∈2-⅄ᐱ(Ln1-Jn2), ∈2-⅄ᐱ(Ln1-Kn2), 2-ᐱ(Ln1-Ln2), ∈2-⅄ᐱ(Ln1-Mn2), ∈2-⅄ᐱ(Ln1-Nn2), ∈2-⅄ᐱ(Ln1-On2), ∈2-⅄ᐱ(Ln1-Pn2), ∈2-⅄ᐱ(Ln1-Qn2), ∈2-⅄ᐱ(Ln1-Rn2), ∈2-⅄ᐱ(Ln1-Sn2), ∈2-⅄ᐱ(Ln1-Tn2),∈2-⅄ᐱ(Ln1-Un2),  ∈2-⅄ᐱ(Ln1-Vn2), ∈2-⅄ᐱ(Ln1-Wn2), ∈2-⅄ᐱ(Ln1-Yn2), ∈2-⅄ᐱ(Ln1-Zn2), ∈2-⅄ᐱ(Ln1-φn2), ∈2-⅄ᐱ(Ln1-Θn2)),2-ᐱ(Ln1cn-n2cn), ∈2-ᐱ(Ln1cn-n2cn), ∈2-ᐱ(Ln1cn-∘⧊°n2cn), ∈2-ᐱ(Ln1cn-∘∇°n2cn)

2-⅄ᐱ(Mn1-An2), ∈2-⅄ᐱ(Mn1-Bn2), ∈2-⅄ᐱ(Mn1-Dn2), ∈2-⅄ᐱ(Mn1-En2), ∈2-⅄ᐱ(Mn1-Fn2), ∈2-⅄ᐱ(Mn1-Gn2), ∈2-⅄ᐱ(Mn1-Hn2), ∈2-⅄ᐱ(Mn1-In2), ∈2-⅄ᐱ(Mn1-Jn2), ∈2-⅄ᐱ(Mn1-Kn2), ∈2-⅄ᐱ(Mn1-Ln2), 2-ᐱ(Mn1-Mn2), ∈2-⅄ᐱ(Mn1-Nn2), ∈2-⅄ᐱ(Mn1-On2), ∈2-⅄ᐱ(Mn1-Pn2), ∈2-⅄ᐱ(Mn1-Qn2), ∈2-⅄ᐱ(Mn1-Rn2), ∈2-⅄ᐱ(Mn1-Sn2), ∈2-⅄ᐱ(Mn1-Tn2),∈2-⅄ᐱ(Mn1-Un2),  ∈2-⅄ᐱ(Mn1-Vn2), ∈2-⅄ᐱ(Mn1-Wn2), ∈2-⅄ᐱ(Mn1-Yn2), ∈2-⅄ᐱ(Mn1-Zn2), ∈2-⅄ᐱ(Mn1-φn2), ∈2-⅄ᐱ(Mn1-Θn2),2-ᐱ(Mn1cn-n2cn), ∈2-ᐱ(Mn1cn-n2cn), ∈2-ᐱ(Mn1cn-∘⧊°n2cn), ∈2-ᐱ(Mn1cn-∘∇°n2cn)

2-⅄ᐱ(Nn1-An2), ∈2-⅄ᐱ(Nn1-Bn2), ∈2-⅄ᐱ(Nn1-Dn2), ∈2-⅄ᐱ(Nn1-En2), ∈2-⅄ᐱ(Nn1-Fn2), ∈2-⅄ᐱ(Nn1-Gn2), ∈2-⅄ᐱ(Nn1-Hn2), ∈2-⅄ᐱ(Nn1-In2), ∈2-⅄ᐱ(Nn1-Jn2), ∈2-⅄ᐱ(Nn1-Kn2), ∈2-⅄ᐱ(Nn1-Ln2), ∈2-⅄ᐱ(Nn1-Mn2), 2-ᐱ(Nn1-Nn2), ∈2-⅄ᐱ(Nn1-On2), ∈2-⅄ᐱ(Nn1-Pn2), ∈2-⅄ᐱ(Nn1-Qn2), ∈2-⅄ᐱ(Nn1-Rn2), ∈2-⅄ᐱ(Nn1-Sn2), ∈2-⅄ᐱ(Nn1-Tn2),∈2-⅄ᐱ(Nn1-Un2),  ∈2-⅄ᐱ(Nn1-Vn2), ∈2-⅄ᐱ(Nn1-Wn2), ∈2-⅄ᐱ(Nn1-Yn2), ∈2-⅄ᐱ(Nn1-Zn2), ∈2-⅄ᐱ(Nn1-φn2), ∈2-⅄ᐱ(Nn1-Θn2),2-ᐱ(Nn1cn-n2cn), ∈2-ᐱ(Nn1cn-n2cn), ∈2-ᐱ(Nn1cn-∘⧊°n2cn), ∈2-ᐱ(Nn1cn-∘∇°n2cn)

2-⅄ᐱ(On1-An2), ∈2-⅄ᐱ(On1-Bn2), ∈2-⅄ᐱ(On1-Dn2), ∈2-⅄ᐱ(On1-En2), ∈2-⅄ᐱ(On1-Fn2), ∈2-⅄ᐱ(On1-Gn2), ∈2-⅄ᐱ(On1-Hn2), ∈2-⅄ᐱ(On1-In2), ∈2-⅄ᐱ(On1-Jn2), ∈2-⅄ᐱ(On1-Kn2), ∈2-⅄ᐱ(On1-Ln2), ∈2-⅄ᐱ(On1-Mn2), ∈2-⅄ᐱ(On1-Nn2), 2-ᐱ(On1-On2), ∈2-⅄ᐱ(On1-Pn2), ∈2-⅄ᐱ(On1-Qn2), ∈2-⅄ᐱ(On1-Rn2), ∈2-⅄ᐱ(On1-Sn2), ∈2-⅄ᐱ(On1-Tn2),∈2-⅄ᐱ(On1-Un2),  ∈2-⅄ᐱ(On1-Vn2), ∈2-⅄ᐱ(On1-Wn2), ∈2-⅄ᐱ(On1-Yn2), ∈2-⅄ᐱ(On1-Zn2), ∈2-⅄ᐱ(On1-φn2), ∈2-⅄ᐱ(On1-Θn2),2-ᐱ(On1cn-n2cn), ∈2-ᐱ(On1cn-n2cn), ∈2-ᐱ(On1cn-∘⧊°n2cn), ∈2-ᐱ(On1cn-∘∇°n2cn)

2-⅄ᐱ(Pn1-An2), ∈2-⅄ᐱ(Pn1-Bn2), ∈2-⅄ᐱ(Pn1-Dn2), ∈2-⅄ᐱ(Pn1-En2), ∈2-⅄ᐱ(Pn1-Fn2), ∈2-⅄ᐱ(Pn1-Gn2), ∈2-⅄ᐱ(Pn1-Hn2), ∈2-⅄ᐱ(Pn1-In2), ∈2-⅄ᐱ(Pn1-Jn2), ∈2-⅄ᐱ(Pn1-Kn2), ∈2-⅄ᐱ(Pn1-Ln2), ∈2-⅄ᐱ(Pn1-Mn2), ∈2-⅄ᐱ(Pn1-Nn2), ∈2-⅄ᐱ(Pn1-On2), 2-ᐱ(Pn1-Pn2), ∈2-⅄ᐱ(Pn1-Qn2), ∈2-⅄ᐱ(Pn1-Rn2), ∈2-⅄ᐱ(Pn1-Sn2), ∈2-⅄ᐱ(Pn1-Tn2),∈2-⅄ᐱ(Pn1-Un2),  ∈2-⅄ᐱ(Pn1-Vn2), ∈2-⅄ᐱ(Pn1-Wn2), ∈2-⅄ᐱ(Pn1-Yn2), ∈2-⅄ᐱ(Pn1-Zn2), ∈2-⅄ᐱ(Pn1-φn2), ∈2-⅄ᐱ(Pn1-Θn2),2-ᐱ(Pn1cn-n2cn), ∈2-ᐱ(Pn1cn-n2cn), ∈2-ᐱ(Pn1cn-∘⧊°n2cn), ∈2-ᐱ(Pn1cn-∘∇°n2cn)

2-⅄ᐱ(Qn1-An2), ∈2-⅄ᐱ(Qn1-Bn2), ∈2-⅄ᐱ(Qn1-Dn2), ∈2-⅄ᐱ(Qn1-En2), ∈2-⅄ᐱ(Qn1-Fn2), ∈2-⅄ᐱ(Qn1-Gn2), ∈2-⅄ᐱ(Qn1-Hn2), ∈2-⅄ᐱ(Qn1-In2), ∈2-⅄ᐱ(Qn1-Jn2), ∈2-⅄ᐱ(Qn1-Kn2), ∈2-⅄ᐱ(Qn1-Ln2), ∈2-⅄ᐱ(Qn1-Mn2), ∈2-⅄ᐱ(Qn1-Nn2), ∈2-⅄ᐱ(Qn1-On2), ∈2-⅄ᐱ(Qn1-Pn2), 2-ᐱ(Qn1-Qn2), ∈2-⅄ᐱ(Qn1-Rn2), ∈2-⅄ᐱ(Qn1-Sn2), ∈2-⅄ᐱ(Qn1-Tn2), ∈2-⅄ᐱ(Qn1-Un2),  ∈2-⅄ᐱ(Qn1-Vn2), ∈2-⅄ᐱ(Qn1-Wn2), ∈2-⅄ᐱ(Qn1-Yn2), ∈2-⅄ᐱ(Qn1-Zn2), ∈2-⅄ᐱ(Qn1-φn2), ∈2-⅄ᐱ(Qn1-Θn2),2-ᐱ(Qn1cn-n2cn), ∈2-ᐱ(Qn1cn-n2cn), ∈2-ᐱ(Qn1cn-∘⧊°n2cn), ∈2-ᐱ(Qn1cn-∘∇°n2cn)

2-⅄ᐱ(Rn1-An2), ∈2-⅄ᐱ(Rn1-Bn2), ∈2-⅄ᐱ(Rn1-Dn2), ∈2-⅄ᐱ(Rn1-En2), ∈2-⅄ᐱ(Rn1-Fn2), ∈2-⅄ᐱ(Rn1-Gn2), ∈2-⅄ᐱ(Rn1-Hn2), ∈2-⅄ᐱ(Rn1-In2), ∈2-⅄ᐱ(Rn1-Jn2), ∈2-⅄ᐱ(Rn1-Kn2), ∈2-⅄ᐱ(Rn1-Ln2), ∈2-⅄ᐱ(Rn1-Mn2), ∈2-⅄ᐱ(Rn1-Nn2), ∈2-⅄ᐱ(Rn1-On2), ∈2-⅄ᐱ(Rn1-Pn2), ∈2-⅄ᐱ(Rn1-Qn2), 2-ᐱ(Rn1-Rn2), ∈2-⅄ᐱ(Rn1-Sn2), ∈2-⅄ᐱ(Rn1-Tn2),∈2-⅄ᐱ(Rn1-Un2),  ∈2-⅄ᐱ(Rn1-Vn2), ∈2-⅄ᐱ(Rn1-Wn2), ∈2-⅄ᐱ(Rn1-Yn2), ∈2-⅄ᐱ(Rn1-Zn2), ∈2-⅄ᐱ(Rn1-φn2), ∈2-⅄ᐱ(Rn1-Θn2),2-ᐱ(Rn1cn-n2cn), ∈2-ᐱ(Rn1cn-n2cn), ∈2-ᐱ(Rn1cn-∘⧊°n2cn), ∈2-ᐱ(Rn1cn-∘∇°n2cn)

2-⅄ᐱ(Sn1-An2), ∈2-⅄ᐱ(Sn1-Bn2), ∈2-⅄ᐱ(Sn1-Dn2), ∈2-⅄ᐱ(Sn1-En2), ∈2-⅄ᐱ(Sn1-Fn2), ∈2-⅄ᐱ(Sn1-Gn2), ∈2-⅄ᐱ(Sn1-Hn2), ∈2-⅄ᐱ(Sn1-In2), ∈2-⅄ᐱ(Sn1-Jn2), ∈2-⅄ᐱ(Sn1-Kn2), ∈2-⅄ᐱ(Sn1-Ln2), ∈2-⅄ᐱ(Sn1-Mn2), ∈2-⅄ᐱ(Sn1-Nn2), ∈2-⅄ᐱ(Sn1-On2), ∈2-⅄ᐱ(Sn1-Pn2), ∈2-⅄ᐱ(Sn1-Qn2), ∈2-⅄ᐱ(Sn1-Rn2), 2-ᐱ(Sn1-Sn2), ∈2-⅄ᐱ(Sn1-Tn2),∈2-⅄ᐱ(Sn1-Un2),  ∈2-⅄ᐱ(Sn1-Vn2), ∈2-⅄ᐱ(Sn1-Wn2), ∈2-⅄ᐱ(Sn1-Yn2), ∈2-⅄ᐱ(Sn1-Zn2), ∈2-⅄ᐱ(Sn1-φn2), ∈2-⅄ᐱ(Sn1-Θn2),2-ᐱ(Sn1cn-n2cn), ∈2-ᐱ(Sn1cn-n2cn), ∈2-ᐱ(Sn1cn-∘⧊°n2cn), ∈2-ᐱ(Sn1cn-∘∇°n2cn)

2-⅄ᐱ(Tn1-An2), ∈2-⅄ᐱ(Tn1-Bn2), ∈2-⅄ᐱ(Tn1-Dn2), ∈2-⅄ᐱ(Tn1-En2), ∈2-⅄ᐱ(Tn1-Fn2), ∈2-⅄ᐱ(Tn1-Gn2), ∈2-⅄ᐱ(Tn1-Hn2), ∈2-⅄ᐱ(Tn1-In2), ∈2-⅄ᐱ(Tn1-Jn2), ∈2-⅄ᐱ(Tn1-Kn2), ∈2-⅄ᐱ(Tn1-Ln2), ∈2-⅄ᐱ(Tn1-Mn2), ∈2-⅄ᐱ(Tn1-Nn2), ∈2-⅄ᐱ(Tn1-On2), ∈2-⅄ᐱ(Tn1-Pn2), ∈2-⅄ᐱ(Tn1-Qn2), ∈2-⅄ᐱ(Tn1-Rn2), ∈2-⅄ᐱ(Tn1-Sn2), 2-ᐱ(Tn1-Tn2),∈2-⅄ᐱ(Tn1-Un2),  ∈2-⅄ᐱ(Tn1-Vn2), ∈2-⅄ᐱ(Tn1-Wn2), ∈2-⅄ᐱ(Tn1-Yn2), ∈2-⅄ᐱ(Tn1-Zn2), ∈2-⅄ᐱ(Tn1-φn2), ∈2-⅄ᐱ(Tn1-Θn2),2-ᐱ(Tn1cn-n2cn), ∈2-ᐱ(Tn1cn-n2cn), ∈2-ᐱ(Tn1cn-∘⧊°n2cn), ∈2-ᐱ(Tn1cn-∘∇°n2cn)

2-⅄ᐱ(Un1-An2), ∈2-⅄ᐱ(Un1-Bn2), ∈2-⅄ᐱ(Un1-Dn2), ∈2-⅄ᐱ(Un1-En2), ∈2-⅄ᐱ(Un1-Fn2), ∈2-⅄ᐱ(Un1-Gn2), ∈2-⅄ᐱ(Un1-Hn2), ∈2-⅄ᐱ(Un1-In2), ∈2-⅄ᐱ(Un1-Jn2), ∈2-⅄ᐱ(Un1-Kn2), ∈2-⅄ᐱ(Un1-Ln2), ∈2-⅄ᐱ(Un1-Mn2), ∈2-⅄ᐱ(Un1-Nn2), ∈2-⅄ᐱ(Un1-On2), ∈2-⅄ᐱ(Un1-Pn2), ∈2-⅄ᐱ(Un1-Qn2), ∈n2-⅄ᐱ(Un1-Rn2), ∈2-⅄ᐱ(Un1-Sn2), ∈2-⅄ᐱ(Un1-Tn2), 2-ᐱ(Un1-Un2),  ∈2-⅄ᐱ(Un1-Vn2), ∈2-⅄ᐱ(Un1-Wn2), ∈2-⅄ᐱ(Un1-Yn2), ∈2-⅄ᐱ(Un1-Zn2), ∈2-⅄ᐱ(Un1-φn2), ∈2-⅄ᐱ(Un1-Θn2),2-ᐱ(Un1cn-n2cn), ∈2-ᐱ(Un1cn-n2cn), ∈2-ᐱ(Un1cn-∘⧊°n2cn), ∈2-ᐱ(Un1cn-∘∇°n2cn)

2-⅄ᐱ(Vn1-An2), ∈2-⅄ᐱ(Vn1-Bn2), ∈2-⅄ᐱ(Vn1-Dn2), ∈2-⅄ᐱ(Vn1-En2), ∈2-⅄ᐱ(Vn1-Fn2), ∈2-⅄ᐱ(Vn1-Gn2), ∈2-⅄ᐱ(Vn1-Hn2), ∈2-⅄ᐱ(Vn1-In2), ∈2-⅄ᐱ(Vn1-Jn2), ∈2-⅄ᐱ(Vn1-Kn2), ∈2-⅄ᐱ(Vn1-Ln2), ∈2-⅄ᐱ(Vn1-Mn2), ∈2-⅄ᐱ(Vn1-Nn2), ∈2-⅄ᐱ(Vn1-On2), ∈2-⅄ᐱ(Vn1-Pn2), ∈2-⅄ᐱ(Vn1-Qn2), ∈2-⅄ᐱ(Vn1-Rn2), ∈2-⅄ᐱ(Vn1-Sn2), ∈2-⅄ᐱ(Vn1-Tn2),∈2-⅄ᐱ(Vn1-Un2),  2-ᐱ(Vn1-Vn2), ∈2-⅄ᐱ(Vn1-Wn2), ∈2-⅄ᐱ(Vn1-Yn2), ∈2-⅄ᐱ(Vn1-Zn2), ∈2-⅄ᐱ(Vn1-φn2), ∈2-⅄ᐱ(Vn1-Θn2),2-ᐱ(Vn1cn-n2cn), ∈2-ᐱ(Vn1cn-n2cn), ∈2-ᐱ(Vn1cn-∘⧊°n2cn), ∈2-ᐱ(Vn1cn-∘∇°n2cn)

2-⅄ᐱ(Wn1-An2), ∈2-⅄ᐱ(Wn1-Bn2), ∈2-⅄ᐱ(Wn1-Dn2), ∈2-⅄ᐱ(Wn1-En2), ∈2-⅄ᐱ(Wn1-Fn2), ∈2-⅄ᐱ(Wn1-Gn2), ∈2-⅄ᐱ(Wn1-Hn2), ∈2-⅄ᐱ(Wn1-In2), ∈2-⅄ᐱ(Wn1-Jn2), ∈2-⅄ᐱ(Wn1-Kn2), ∈2-⅄ᐱ(Wn1-Ln2), ∈2-⅄ᐱ(Wn1-Mn2), ∈2-⅄ᐱ(Wn1-Nn2), ∈2-⅄ᐱ(Wn1-On2), ∈2-⅄ᐱ(Wn1-Pn2), ∈2-⅄ᐱ(Wn1-Qn2), ∈2-⅄ᐱ(Wn1-Rn2), ∈2-⅄ᐱ(Wn1-Sn2), ∈2-⅄ᐱ(Wn1-Tn2),∈2-⅄ᐱ(Wn1-Un2),  ∈2-⅄ᐱ(Wn1-Vn2), 2-ᐱ(Wn1-Wn2), ∈2-⅄ᐱ(Wn1-Yn2), ∈2-⅄ᐱ(Wn1-Zn2), ∈2-⅄ᐱ(Wn1-φn2), ∈2-⅄ᐱ(Wn1-Θn2),2-ᐱ(Wn1cn-n2cn), ∈2-ᐱ(Wn1cn-n2cn), ∈2-ᐱ(Wn1cn-∘⧊°n2cn), ∈2-ᐱ(Wn1cn-∘∇°n2cn)

2-⅄ᐱ(Yn1-An2), ∈2-⅄ᐱ(Yn1-Bn2), ∈2-⅄ᐱ(Yn1-Dn2), ∈2-⅄ᐱ(Yn1-En2), ∈2-⅄ᐱ(Yn1-Fn2), ∈2-⅄ᐱ(Yn1-Gn2), ∈2-⅄ᐱ(Yn1-Hn2), ∈2-⅄ᐱ(Yn1-In2), ∈2-⅄ᐱ(Yn1-Jn2), ∈2-⅄ᐱ(Yn1-Kn2), ∈2-⅄ᐱ(Yn1-Ln2), ∈2-⅄ᐱ(Yn1-Mn2), ∈2-⅄ᐱ(Yn1-Nn2), ∈2-⅄ᐱ(Yn1-On2), ∈2-⅄ᐱ(Yn1-Pn2), ∈2-⅄ᐱ(Yn1-Qn2), ∈2-⅄ᐱ(Yn1-Rn2), ∈2-⅄ᐱ(Yn1-Sn2), ∈2-⅄ᐱ(Yn1-Tn2),∈2-⅄ᐱ(Yn1-Un2),  ∈2-⅄ᐱ(Yn1-Vn2), ∈2-⅄ᐱ(Yn1-Wn2), 2-ᐱ(Yn1-Yn2), ∈2-⅄ᐱ(Yn1-Zn2), ∈2-⅄ᐱ(Yn1-φn2), ∈2-⅄ᐱ(Yn1-Θn2),2-ᐱ(Yn1cn-n2cn), ∈2-ᐱ(Yn1cn-n2cn), ∈2-ᐱ(Yn1cn-∘⧊°n2cn), ∈2-ᐱ(Yn1cn-∘∇°n2cn)

2-⅄ᐱ(Zn1-An2), ∈2-⅄ᐱ(Zn1-Bn2), ∈2-⅄ᐱ(Zn1-Dn2), ∈2-⅄ᐱ(Zn1-En2), ∈2-⅄ᐱ(Zn1-Fn2), ∈2-⅄ᐱ(Zn1-Gn2), ∈2-⅄ᐱ(Zn1-Hn2), ∈2-⅄ᐱ(Zn1-In2), ∈2-⅄ᐱ(Zn1-Jn2), ∈2-⅄ᐱ(Zn1-Kn2), ∈2-⅄ᐱ(Zn1-Ln2), ∈2-⅄ᐱ(Zn1-Mn2), ∈2-⅄ᐱ(Zn1-Nn2), ∈2-⅄ᐱ(Zn1-On2), ∈2-⅄ᐱ(Zn1-Pn2), ∈2-⅄ᐱ(Zn1-Qn2), ∈2-⅄ᐱ(Zn1-Rn2), ∈2-⅄ᐱ(Zn1-Sn2), ∈2-⅄ᐱ(Zn1-Tn2),∈2-⅄ᐱ(Zn1-Un2),  ∈2-⅄ᐱ(Zn1-Vn2), ∈2-⅄ᐱ(Zn1-Wn2), ∈2-⅄ᐱ(Zn1-Yn2), 2-ᐱ(Zn1-Zn2), ∈2-⅄ᐱ(Zn1-φn2), ∈2-⅄ᐱ(Zn1-Θn2),2-ᐱ(Zn1cn-n2cn), ∈2-ᐱ(Zn1cn-n2cn), ∈2-ᐱ(Zn1cn-∘⧊°n2cn), ∈2-ᐱ(Zn1cn-∘∇°n2cn)

2-⅄ᐱ(φn1-An2), ∈2-⅄ᐱ(φn1-Bn2), ∈2-⅄ᐱ(φn1-Dn2), ∈2-⅄ᐱ(φn1-En2), ∈2-⅄ᐱ(φn1-Fn2), ∈2-⅄ᐱ(φn1-Gn2), ∈2-⅄ᐱ(φn1-Hn2), ∈2-⅄ᐱ(φn1-In2), ∈2-⅄ᐱ(φn1-Jn2), ∈2-⅄ᐱ(φn1-Kn2), ∈2-⅄ᐱ(φn1-Ln2), ∈2-⅄ᐱ(φn1-Mn2), ∈2-⅄ᐱ(φn1-Nn2), ∈2-⅄ᐱ(φn1-On2), ∈2-⅄ᐱ(φn1-Pn2), ∈2-⅄ᐱ(φn1-Qn2), ∈2-⅄ᐱ(φn1-Rn2), ∈2-⅄ᐱ(φn1-Sn2), ∈2-⅄ᐱ(φn1-Tn2),∈2-⅄ᐱ(φn1-Un2),  ∈2-⅄ᐱ(φn1-Vn2), ∈2-⅄ᐱ(φn1-Wn2), ∈2-⅄ᐱ(φn1-Yn2), ∈2-⅄ᐱ(φn1-Zn2), 2-ᐱ(φn1-φn2), ∈2-⅄ᐱ(φn1-Θn2),2-ᐱ(φn1cn-n2cn), ∈2-ᐱ(φn1cn-n2cn), ∈2-ᐱ(φn1cn-∘⧊°n2cn), ∈2-ᐱ(φn1cn-∘∇°n2cn)

2-⅄ᐱ(Θn1-An2), ∈2-⅄ᐱ(Θn1-Bn2), ∈2-⅄ᐱ(Θn1-Dn2), ∈2-⅄ᐱ(Θn1-En2), ∈2-⅄ᐱ(Θn1-Fn2), ∈2-⅄ᐱ(Θn1-Gn2), ∈2-⅄ᐱ(Θn1-Hn2), ∈2-⅄ᐱ(Θn1-In2), ∈2-⅄ᐱ(Θn1-Jn2), ∈2-⅄ᐱ(Θn1-Kn2), ∈2-⅄ᐱ(Θn1/Ln2), ∈2-⅄ᐱ(Θn1-Mn2), ∈2-⅄ᐱ(Θn1-Nn2), ∈2-⅄ᐱ(Θn1-On2), ∈2-⅄ᐱ(Θn1-Pn2), ∈2-⅄ᐱ(Θn1-Qn2), ∈2-⅄ᐱ(Θn1-Rn2), ∈2-⅄ᐱ(Θn1-Sn2), ∈2-⅄ᐱ(Θn1-Tn2),∈2-⅄ᐱ(Θn1-Un2),  ∈2-⅄ᐱ(Θn1-Vn2), ∈2-⅄ᐱ(Θn1-Wn2), ∈2-⅄ᐱ(Θn1-Yn2), ∈2-⅄ᐱ(Θn1-Zn2), ∈2-⅄ᐱ(Θn1-φn2), 2-ᐱ(Θn1-Θn2), ∈2-ᐱ(Θn1cn-n2cn), ∈2-ᐱ(Θn1cn-n2cn), ∈2-ᐱ(Θn1cn-∘⧊°n2cn), ∈2-ᐱ(Θn1cn-∘∇°n2cn)

ncn=(⅄n)(ncn)

Variables of A  B  D  E  F  G  H  I  J  K  L  M  N  O  P  Q  R  S  T  U  V  W  X  Y  Z  φ  Θ  ᐱ  ᗑ  ∘⧊°  ∘∇° are applicable to a function.

Function path ⅄ncn=(⅄nncn)(ncn) is nncn to a multiple of nncn such that nncn is a number or variable with a repeating or not repeating decimal stem cycle variant. =

Examples of ncn=(⅄nncn)(ncn)

 ⅄ncn=(⅄nncn)(2)=(nncn)x(nncn)

 ⅄ncn=(⅄nncn)(3)=(nncn)x(nncn)x(nncn)

 ⅄ncn=(⅄nncn)(10)=(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)


ncnA exponential complex function variables of Ancn

if A=∈1/Q)cn and path ⅄ of Q is a variant in the definition of A then 

A=1n2/Qn1)=[(Yn2/Yn1)/(P/P) while Q requires path definition of 1⅄Q or 2⅄Q from P two sets of A complete the formula of Q variable.

A=1n2/1Qn1)=[(Yn3/Yn2)/(Pn2/Pn1)=(1/1)/(3/2)=(1/1.5)=0.^6

and

A=1n2/2Qn1c1)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^6)=1.^6


Applied function of ncn=(⅄nncn)(ncn) with A variables is then 

An1  of 1n2/1Qn1)c1 along path (2)=(1n2/1Qn1))c1(1⅄(φn2/1⅄Qn1)c1)  or [An1  of 1n2/1Qn1)c1 x An1  of 1n2/1Qn1)c1]

and

An1  of 1n2/2Qn1c1)c1 along path (2)=(1n2/2Qn1c1))c1(1⅄(φn2/2⅄Qn1c1)c1) or [An1  of 1n2/2Qn1c1)c1 x An1  of 1n2/2Qn1c1)c1]



(2)An1=

(2)=(1n2/1Qn1))c1(1⅄(φn2/1⅄Qn1)c1)=0.6(2)=0.6x0.6=0.36

and

(2)=(1n2/2Qn1c1))c1(1⅄(φn2/2⅄Qn1c1)c1)=1.6(2)=1.6x1.6=2.56


(2)An1=

[An1  of 1n2/1Qn1)c1 x An1  of 1n2/1Qn1)c1]=0.36

and

[An1  of 1n2/2Qn1c1)c1 x An1  of 1n2/2Qn1c1)c1]=2.56


Any change in cn stem decimal cycle count variable will change the multiple of the exponent squared value in the example and ultimately the final product value also. 


Potential Change of An1  of 1n2/1Qn1)c1 is An1c1=0.6, An1c2=0.66, An1c3=0.666 and so on for An1  of 1n2/1Qn1)

then (2)An1c2 of 1n2/1Qn1)=0.66(2)=(0.66x0.66)=0.4356 

and (2)An1c3 of 1n2/1Qn1)=0.666(2)=(0.666x0.666)=0.443556


Potential Change of An1  of 1n2/2Qn1c1)c1 is based at variable 2Qn1cn as well as An1  of 1n2/2Qn1c1)cn


if 2Qn1cn for An1  of 1⅄ path n2/2Qn1c1) is 2Qn1c2 then A=1n2/2Qn1c2)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^66)=^1.5

and (2)An1c1 of 1n2/2Qn1c2)=1.5(2)=(1.5x1.5)=2.25 while (2)An1c2 of 1n2/2Qn1c2)=1.515(2)=(1.515x1.515)=2.295225

however

A=1n2/2Qn1c1)=[(Yn3/Yn2)/(Pn1/Pn2)=(1/1)/(2/3)=(1/0.^6)=1.^6 and (2)A of 1n2/2Qn1c1)=(1.^6)(2)=(1.6x1.6)=2.56

then (2)An1c2 of 1n2/2Qn1c1)(1.^66)(2)=(1.66x1.66)=2.7556 and (2)An1c3 of 1n2/2Qn1c1)(1.^666)(2)=(1.666x1.666)=2.775556


It is not that these order of operations are incorrect by any means given the path and extent of the defined variables decimal stem cycles have potential change and limit to the variable definition at cn of the variants. 

Although 0.4356 ≠ 0.443556 ≠ 2.25 ≠ 2.295225 ≠ 2.56 ≠ 2.7556 ≠ 2.775556 are not equal.

The values are precise scale variables to the function of ƒ(2)An1cn of ∈[0.4356; 0.443556; 2.25; 2.295225; 2.56; 2.7556; 2.775556 . . .} of altered paths with variants Ancn within the paths sub-units nQncn. These are exponential products from ratios divided by ratios from variables of consecutive bases in y fibonacci and p prime variables. 

Commonly referred to as an algorithm of partial derivative quadratic set variables...


Variable change in cn stem decimal cycle count variables, when applied to numbers greater in exponent will produce astronomical differences in numerical precision based products, quotients, sums, and differences.


With Variables of set ∈A complex variables factor to quotients that are applicable to examples of ncn=(⅄nncn)(ncn)

 ⅄ncn=(⅄nncn)(2)=(nncn)x(nncn)

 ⅄ncn=(⅄nncn)(3)=(nncn)x(nncn)x(nncn)

 ⅄ncn=(⅄nncn)(10)=(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn)x(nncn) with definitions in 

nᐱ(An/An), ∈nᐱ(An/Bn), ∈nᐱ(An/Dn), ∈nᐱ(An/En), ∈nᐱ(An/Fn), ∈nᐱ(An/Gn), ∈nᐱ(An/Hn), ∈nᐱ(An/In), ∈nᐱ(An/Jn), ∈nᐱ(An/Kn), ∈nᐱ(An/Ln), ∈nᐱ(An/Mn), ∈nᐱ(An/Nn), ∈nᐱ(An/On), ∈nᐱ(An/Pn), ∈nᐱ(An/Qn), ∈nᐱ(An/Rn), ∈nᐱ(An/Sn), ∈nᐱ(An/Tn),∈nᐱ(An/Un),  ∈nᐱ(An/Vn), ∈nᐱ(An/Wn), ∈nᐱ(An/Yn), ∈nᐱ(An/Zn), ∈nᐱ(Ann), ∈nᐱ(Ann), ∈nᐱ(An/ᐱn), ∈nᐱ(An/ᗑn), ∈nᐱ(An/∘⧊°n), ∈nᐱ(An/∘∇°n

such that a variable from these sets is applicable to be squared, cubed, factored to the power of 10, and so on with exponential precision based on nncn numbered cycles in ratio decimal stem value. =


Sets ∈A applied to a squared function ⅄ncn=(⅄nncn)(2)

nncnᐱ(An/An)(2)=(An/An)x(An/An)

nncnᐱ(An/Bn)(2)=(An/Bn)x(An/Bn)

nncnᐱ(An/Dn)(2)=(An/Dn)x(An/Dn)

nncnᐱ(An/En)(2)=(An/En)x(An/En)

nncnᐱ(An/Fn)(2)=(An/Fn)x(An/Fn)

nncnᐱ(An/Gn)(2)=(An/Gn)x(An/Gn)

nncnᐱ(An/Hn)(2)=(An/Hn)x(An/Hn)

nncnᐱ(An/In)(2)=(An/In)x(An/In)

nncnᐱ(An/Jn)(2)=(An/Jn)x(An/Jn)

nncnᐱ(An/Kn)(2)=(An/Kn)x(An/Kn)

nncnᐱ(An/Ln)(2)=(An/Ln)x(An/Ln)

nncnᐱ(An/Mn)(2)=(An/Mn)x(An/Mn)

nncnᐱ(An/Nn)(2)=(An/Nn)x(An/Nn)

nncnᐱ(An/On)(2)=(An/On)x(An/On)

nncnᐱ(An/Pn)(2)=(An/Pn)x(An/Pn)

nncnᐱ(An/Qn)(2)=(An/Qn)x(An/Qn)

nncnᐱ(An/Rn)(2)=(An/Rn)x(An/Rn)

nncnᐱ(An/Sn)(2)=(An/Sn)x(An/Sn)

nncnᐱ(An/Tn)(2)=(An/Tn)x(An/Tn)

nncnᐱ(An/Un)(2)=(An/Un)x(An/Un)

nncnᐱ(An/Vn)(2)=(An/Vn)x(An/Vn)

nncnᐱ(An/Wn)(2)=(An/Wn)x(An/Wn)

nncnᐱ(An/Yn)(2)=(An/Yn)x(An/Yn)

nncnᐱ(An/Zn)(2)=(An/Zn)x(An/Zn)

nncnᐱ(Ann)(2)=(Ann)x(Ann)

nncnᐱ(Ann)(2)=(Ann)x(Ann)

nncnᐱ(An/ᐱn)(2)=(An/ᐱn)x(An/ᐱn)

nncnᐱ(An/ᗑn)(2)=(An/ᗑn)x(An/ᗑn)

nncnᐱ(An/∘⧊°n)(2)=(An/∘⧊°n)x(An/∘⧊°n)

nncnᐱ(An/∘∇°n)(2)=(An/∘∇°n)x(An/∘∇°n)

And so on for sets ∈A applied to a squared function ⅄ncn=(⅄nncn)(2), ⅄ncn=(⅄nncn)(3), ⅄ncn=(⅄nncn)(10), to ⅄ncn=(⅄nncn)(n)

Variable definition (⅄nncn) decimal stem cycle count is required before any exponential factoring is applied of the variables in exponent path functions.


Variables applicable in multiplication stem cell cycle functions of cn variable change potentials.

Numbers in sets where 1X⅄=(n2xn1) and n= equals at numeral from any set of division stemmed cycle cell numerals defined. from whole numbers of Y P φ and Q radical bases. 

So that 

⅄ will always have a path of 1⅄ later to previous 

2⅄ previous to later of path routes no matter the sets the variables stem from. 

Then

n path of an exponential with cn variables

n⅄n=⅄n(n)

Example 

if ⅄n of 1φn21 is ⅄n(n) n is 1.6^1803399852 

then n of 1φn21(2) is 1.61803399852(1.61803399852) is 1.61803399852x1.61803399852

and n of 1φn21(3) is 1.61803399852x1.61803399852x1.61803399852 assuming the cycle stem count for 1φn21 is c1 of the repeatable decimal 1803399852 and so on to the power of exponential factoring of variables.

Then

ncn path of an exponential specified with cn in exponential cycle stem definition to exponent of a specific exponent.

nncn=⅄n(ncn)

Example 

if ncn of 1φn21c2 is ⅄n(2c2) n is 1.6^18033998521803399852 

then ncn of 1φn21c2(2) is 1.618033998521803399852(1.6180339985261803399852) is 1.618033998521803399852x1.618033998521803399852

and ncn of 1φn21c2(3) is 1.618033998521803399852x1.618033998521803399852x1.618033998521803399852 

assuming the cycle stem count for 1φn21 is c2 of the repeatable decimal 18033998521803399852  and so on to the power of exponential factoring of variables.


Given Path functions 1⅄, 2⅄, 3nc, X, +⅄, 1-⅄, 2-⅄, ⅄n then with path function +⅄ addition variables of radical ratios can be added.

Factoring with An1 of 1n2/2Qn1c1)=(1/0.^6)=1.^6 variables to function +⅄ addition is 

+⅄An1 variables of 1n2+2Qn1c1)=(1+0.^6)=1.6

Factoring with An1 of 1n2/1Qn1)=(1/1.5)=0.^6 variables to function +⅄ addition is 

+⅄An1 variables of 1n2+1Qn1)=(1+1.5)=2.5

Factoring variables (An1 of 1n2/2Qn1c1) and (An1 of 1n2/1Qn1)) to function +⅄ addition is

(+⅄An1 variables 1n2+2Qn1c1)c1+ (+⅄An1 variables 1n2+1Qn1)c1=(1.^6+0.^6)=2.2

While factoring variables (+⅄An1 of 1n2+2Qn1c1) and (+⅄An1 variables 1n2+1Qn1)  to function +⅄ addition is 

(+⅄An1 variables 1n2+2Qn1c1)+(+⅄An1 variables 1n2+1Qn1)=(1.6+2.5)=4.1

So path function +⅄ addition of variables of sets in An then requires precise definition that vary from variables of sets in An and those variables vary from 1Qn and 2Qn

(+⅄An1 variables 1n2+2Qn1c1)c1+ (+⅄An1 variables 1n2+1Qn1)c1(+⅄An1 variables 1n2+2Qn1c1)+(+⅄An1 variables 1n2+1Qn1)

Given that order of operations is a path and these variables are derived from alternate functions and paths, then the statement above is true and 

2.2≠4.1 nor is it 2.2 half of 4.1

Path functions 1⅄, 2⅄, 3nc, X, +⅄, 1-⅄, 2-⅄, ⅄n then are applicable to variables and factors of variables for alternate paths in functions.

PEMDAS order of operations then is an algebraic logic and these variables function in paths of differing order of function operation defined to specific points and phases of the variables such as decimal cycle stem count Nncn of variables in sets {A,B,D,E,F,G,H,I,J,K,L,M,O,Q,R,S,T,U,V,W,X,Y,Z,φ,Θ,ᐱ,ᗑ,∘⧊°,∘∇°}

Example Y variables of 2 path to Θ and Y variables of 1⅄ path to φ then 1 of φ and Θ variables to D and 2 of φ and Θ to B alternately 1of Θ and φ to O while 2 of Θ and φ to G begin from variables of Y that are structured of adding a number with the previous for the next. 

Addition being the A of PEMDAS order of operations Parenthesis Exponents Multiplication Division Addition then Subtraction would explain how the variable ratios are incorrect yet the numbers and variable ratios of paths define very rationally and precisely.

| ⋯ | | ⋱ | ⋰ | ∴ | ∵ | |

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | Y,φ,Θ,P,Q | : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | A,M,V,W,E,F,I,H,D,B,O,G,L,K,U,J,R,Z,T,S | : | 433494437 | : | 1000000007 | : |1138903170| 

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 1⅄A ,1M1V,1W| : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 1ᐱ, 2ᐱ, 3ᐱ, . . .| : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 1⅄ᐱ, 2⅄ᐱ, 3⅄ᐱ, . . .| : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 1ᗑ, 2ᗑ, 3ᗑ, . . .| : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 1⅄ᗑ, 2⅄ᗑ, 3⅄ᗑ, . . .| : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 0∘⧊°10∘⧊° | : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | 0∇°10∇° | : | 433494437 | : | 1000000007 | : |1138903170|

|0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | : | | : | 433494437 | : | 1000000007 | : |1138903170|

Relativity of ΘPQ AMVWEFIHᐱᗑ 0∘⧊° 10∘⧊° 0∘∇° 10∘∇° |0| : |1| : | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  |

Numerals of binary logic gates such as 10, 00, 11, 01, and 000, 111, 101, 010, 100, 001, 110, 011

0000 1111

mean that quad and 8 bit bases are very important where | 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  |

of a limit to 10 digit numerals of phi and prime whether sliding a byte shift array from  

|0| → 1138903170 and | 2 | → 1000000007  

| 2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229  | to |  3 : 5 : 13 : 89 : 1597 : 28657 : 514229 : 433494437 | or not

with such a shift of an 8 base to a nine digit common factor is one thing, |0| |1| |1| and |2| are a logic gate of the same probability factors of 000, 111, 101, 010, 100, 001, 110, 011 or 10, 00, 11, 01 in file masking to other paths that may appear to be the same logic gates and with different definitions are exactly the opposite. They are not the same.

the relativity of the first 8 common numerals of phi and prime are shown first before a nine digit fibonacci phi prime in the 10 digit relativity description. From the base core relativity then

| 433494437 | : | ΘPQ

| 433494437  | : | AMVWEFIHDBOGLKUJRZTS

| 433494437  | : | ᐱᗑ

| 433494437 | : | 0∘⧊°10∘⧊° |

| 433494437 | : | 0∘∇°10∘∇°

numbers |0| |1| |1| and |2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229 : 433494437 | have a limit of combinations pertaining to 9 10 11 and 12 base arrays in computers phone numbers and ipv to ikev address arrays that produce sets of matrix  limits that outnumber most telephone system limits of a local area network with intranet systems within its internet link and telecommunications. What can be done with 8 factors of 1's and 0's and what can be done with less like three 0 0 0 or 1 1 1 have already been shown here on this page from a simple 0 1 1 that sits between 000 and 111 if thats where its place is in one of 8 bits to 000 001 011 111 110 100 101 010. One binary base is only one of the combinations made with 8 bits that a unix shell to linux shell operates on at its compilers and logic gates.

Basic Examples of Radical ratios containing a common factor in Y and P bases

Numeral 2 containing a common factor in φ and Q bases

1φn3=(yn4/yn3)=(2/1)2

1φn4=(yn5/yn4)=(3/2)=1.5

11Qn1=(pn2/pn1)=(3/2)=1.5

21Qn1=(pn1/pn2)=(2/3)=0.^6 

Numeral 3 containing a common factor in φ and Q bases

1φn4=(yn5/yn4)=(3/2)=1.5

1φn5=(yn6/yn5)=(5/3)=1.^6 

11Qn1=(pn2/pn1)=(3/2)=1.5

11Qn2=(pn3/pn2)c1=(5/3)=1.^6

21Qn1=(pn1/pn2)=(2/3)=0.^6 

21Qn2=(pn2/pn3)=(3/5)=0.6 

Numeral 5 containing a common factor in φ and Q bases

1φn5=(yn6/yn5)=(5/3)=1.^6 

1φn6=(yn7/yn6)=(8/5)=1.6 

11Qn2=(pn3/pn2)c1=(5/3)=1.^6

11Qn3=(pn4/pn3)=(7/5)=1.4

21Qn2=(pn2/pn3)=(3/5)=0.6 

21Qn3=(pn3/pn4)=(5/7)=0.^714285

More complex arrays of ratios containing a common factor in Y and P bases can be structured in 10 digit limit or more of  2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229 : 433494437 that 0 is not a common factor of in prime bases until 0 from y base functions are factored with prime base p and Q with y and 1φ variables in an array of 

|2 : 1000000007 | : |2 : 1138903170| that an array |0 : 1138903170| can contain the array |2 : 1000000007 | in.

A difference of 138,903,163 from 1138903170-1000000007

a difference of -138,903,163 from 1000000007-1138903170

277,806326 total between positive 138,903,163 and negative 138,903,163 where if 0 is a numeral and 1 the numerals 0 and 1 of this factoring are not numerals of the prime scale variable common factors. 

if |0|=1 and |1|=1 and |-1|=1 while y base factors of phi contain 0 1 1 that prime base does not since its prime is not divided to anything other than its prime base  |0|+|1|+|-1|=3 and 3x277,806326=833,418,978 possible byte shifts of an incorrect factor are applicable to multiple numerating calculus functions of exponential numerals from one numeral changed that should not be changed in the array. 

Searching through 833,418,978 astronomical unit measure of a shifting interest rate or incorrect scale applied to that figure for a numeral such as 0.0000000001 or 0.000000000000000000001 or 0.0000000000000000000000000000001 or 0.0000000000000000000000000000000001 or 0.00000000000000000000000000000000001 with ample time to make extracts of financial profit in a byte shift error through a window programmed to create that window and its shift change are as simple as numbers known to numbers not known and limited for the search of those numbers.

Eliptic Eponyms and Elcipses

Logic Number Example

Number bridge of Y quantum base fractals using fibonacci count base division in alternate paths in constant numbers to φ and Θ as relatable to prime base fractals of P to Q quantum base. From These relations variables of numerical precision define variables of numeration further. 

Within the y base n1 through n11 have decimal quotient similarities of minus or plus 1 exact. If a 1 is subtracted from system of 1φn8 and exhibits traits of a system 1Θn7 after 1 is subtracted the difference is notable and if a 1 is subtracted from system of 1φn8 and exhibits traits of a system 1φn8 still after 1 is subtracted the difference is notable. Adding 1 to a system of 1Θn7 also is notable as the change in a system may shift to 1φn8  within its system traits that started oppositely in 1Θ rather than the 1φ difference in 1 and 2of Y base.

Within the y base n1 through n11 have decimal quotient similarities of minus or plus 1 exact. If a 1 is subtracted from system of 1φn9 and exhibits traits of a system 1Θn8 after 1 is subtracted the difference is notable and if a 1 is subtracted from system of 1φn9 and exhibits traits of a system 1φn9 still after 1 is subtracted the difference is notable. Adding 1 to a system of 1Θn8 also is notable as the change in a system may shift to 1φn9  within its system traits that started oppositely in 1Θ rather than the 1φ difference in 1and 2of Y base. Although 1φn8c1  equals 1.615384 and (1φn8c1-1)=0.615384 and 1Θn7=0.615384 the path of how 0.615384 is factored means within the added function of  (1φn8c1-1) is a minus one and different derivative of how 0.615384 is factored and is defined differently. Within the added -1 minus one path or a +1 plus one (1Θn7c1+1)=1.615384 are whole numbers and alternate paths of a factored variable. That number bridge of variable derivative definition is a quantifiable bridge just as are the cycle stem in decimal cn.

so then

Within the y base n1 through n11 have decimal quotient similarities of minus or plus 1 exact. If a 1 is subtracted from system of 1φn11 and exhibits traits of a system 1Θn10 after 1 is subtracted the difference is notable and if a 1 is subtracted from system of 1φn11 and exhibits traits of a system 1φn11 still after 1 is subtracted the difference is notable. Adding 1 to a system of 1Θn10 also is notable as the change in a system may shift to 1φn11  within its system traits that started oppositely in 1Θ rather than the 1φ difference in 1and 2of Y base.  So [(1φn8c1-1)~(1Θn7c1+1)] and [(1φn9c1-1)~(1Θn8c1+1)] are similar and factorable of bridge types between ratio variables of alternate Y paths that no matter the cn extent of the four variables 1φn8cn 1φn9cn 1Θn7cn 1Θn8cn  and many other variables between φ and Θ of Y base ratios.

n[(1φn8c1-1)~(1Θn7c1+1)] if cycle stem count and numerals are similar cn of system change Δ or ∇ the bridge is quantifiable. 

n[(1φn9c1-1)~(1Θn8c1+1)] if cycle stem count and numerals are similar cn of system change Δ or ∇ the bridge is quantifiable.

reason

if 1φn8  1.615384  is given and a return of minus one  0.615384 that is 1Θn7 the system variable return are a symetric transfer of numbers to a y base of two or more wave forms of systems that can lose 1 displaced on a y shift of previous path values.

if 1φn9  1.619047  is given and a return of minus one  0.619047 that is 1Θn8 the system variable return are a symetric transfer of numbers to a y base of two or more wave forms of systems that can lose 1 displaced on a y shift of previous path values. 

if 1φn11=(Yn12/Yn11)=(89/55)=1.618 and  1Θn10=2(Y10/Y11)=(34/55)=0.618 

and so on for variables similar minus or plus one between φ and Θ paths ⅄ of Y bases. . . . for example

1φn13=(Yn14/Yn13)=(233/144)=1.6180^5 and 1Θn12=2(Y12/Y13)=(89/144)=0.6180^5

1.6180^5-1=0.6180^5 as 1.6180^55-1=0.6180^55 and a difference of Nncn will show a notable difference such as with numerated decimal stem cell cycle per variant in defined paths.

 1φn11-1Θn10=1 and 1φn11c2-1Θn10=1.00018 and 1φn11-1Θn10c2=0.99982 and so on for changes in (1φn11-1Θn10)ncn and(1φn11+1Θn10)ncn and (1φn11x1Θn10)ncn  and (1φn11/1Θn10)ncn and (1Θn10-1φn11)ncn and (1Θn10x1φn11)ncnn and (1Θn10/1φn11)ncn 

if a number bridge n[(1φn8c1-1)~(1Θn7c1+1)]  for example can be quantitated then so to can the number of times that defined bridge can be numerated or partially numerated that if it is partially numerated the bridge then holds a variable factor when that bridge is partially numerated and is now a factored variable of a system bridge changed itself with Δ or ∇of bridge n[(1φn8c1-1)~(1Θn7c1+1)] partially derived δ to some micron unit measure δµ of defined variarables. 

These are basic examples with shorter decimal length numerals than more complex numbers.

Similar decimal cycle stem variants from different functions of y path sets that in calculation of multiples, exponents, fractions plus or minus quadratic cube rooted vectors and are not limited in decimal stem cycle per base function Y of  φ Θncn 

1φn8 : 1Θn7 variables of Y base are 1.^615384 : 0.^615384 or 1.615384 : 0.615384

1φn9 : 1Θn8 variables of Y base are  1.^619047 : 0.^619047 or 1.619047 : 0.619047

while 1∀Y2nd=(Yn10/Yn8)=(34/13)=2.^615384 and 1∀Y2nd=(Yn11/Yn9)=(55/21)=2.^619047 a difference of 1 and 2 of whole numbers with the examples of quotients having exactly the same stem cell decimal cycle repeatable sequence.

1⅄∀Y2nd c1(Yn10/Yn8) : 1φn8c1 : 1Θn7c1 variables of Y base are 2.^615384 : 1.^615384 : 0.^615384 or 2.615384 : 1.615384 : 0.615384

1⅄∀Y2ndc1=(Yn11/Yn9) : 1φn9c1 : 1Θn8c1 variables of Y base are 2.^619047 : 1.^619047 : 0.^619047 or 1.619047 : 0.619047 : 2.619047

(1φn8 : 1Θn7 )=  1(Yn9/Yn8)=(21/13)   :   2(Y7/Y8)=(8/13

(1φn9 : 1Θn8 )=  (1Yn10/Yn9)=(34/21)   :  2(Y8/Y9)=(13/21)

A common quotient and a quotient minus or plus exactly one is a relation between φand Θ phi and theta variables.

Paths  123⅄ are applicable to the degree of cn for each degree of nφncnn : nΘncn n

For Example 1φn11=(Yn12/Yn11)=(89/55)=1.6^18 and  1Θn10=2(Y10/Y11)=(34/55)=0.6^18 so then formulas can be written to combine divide multiply and exponent to degrees of each for numerical definition in their relations.

(φxΘ), (φ/Θ), (φ+Θ), (φ-Θ), (nφncn n), (nΘncn n) to degrees of path sets of variables nφncnn : nΘncn n

(Θxφ), (Θ/φ), (Θ+φ), (Θ/-φ), (nφncn n), (nΘncn n) to degrees of path sets of variables nφncnn : nΘncn n

Phi Theta Prime 13 is the two digit prime variable common factor of this Y φ  Θ P Q path base factor that prime factoring systems |1φn8 : 1Θn7|and 1 |1φn9 : 1Θn8 | The prime factor 13 of Y and P is a common factor of 3 of 4 quadratic common factor numeral bases that is a 33% or .33^3 on 100% of that system.  key chains for manifold systems or other numerated forms.

1φn21=(Yn22/Yn21)=(10946/6765)=1.6^1803399852 and 1Θn20=2(Y20/Y21)=(4181/6765)=0.6^1803399852 then are also a numeratable bridge of Y factors to paths that a bridge used can be counted of uses with n[(1φn21c1-1)~(1Θn20c1+1)] if cycle stem count and numerals are similar cn of system change Δ or ∇ the bridge is quantifiable.

n[(1φn21c11.6^1803399852-1)=0.6^1803399852] ~ [(1Θn20c10.6^1803399852+1)=1.6^1803399852] that 1⅄Y=φ and 2⅄=Θ

1⅄Y=φ and not (1Θn20c10.6^1803399852+1)=1.6^1803399852

2⅄=Θ and not (1φn21c11.6^1803399852-1)=0.6^1803399852

So a set of bridgeable variables between φ and Θ is numerable at the n outside the brackets [(1φn21c1-1)~(1Θn20c1+1)] and is a numerable set of bridges between similarities of φ and Θ.

Many equations on this page use a numeral in factoring that are common factors between Y φ  Θ P Q fibonacci and prime consecutive numeral base functions.

Number Bridge List 

First 10 number bridges between φ and Θ decimal stem cycle similarities of Y base for +1 or -1 of ⅄ path differences in Y factor. Following 0 and 1 of Θ and 0 and 1 and 2 of φ

n1[(1φn4-1)~(1Θn3+1)]=[(1.5-1)~(0.5+1)]

n2[(1φn5-1)~(1Θn4+1)]=[(1.6-1)~(0.6+1)]

n3[(1φn6-1)~(1Θn5+1)]=[(1.6-1)~(0.6+1)]

n4[(1φn7-1)~(1Θn6+1)]=[(1.625-1)~(0.625+1)]

n5[(1φn8-1)~(1Θn7+1)]=[(1.615384-1)~(0.615384+1)] ~ 1∀Y2nd=(Yn10/Yn8)=(34/13)=2.615384 


0.615384 : 1.615384 : 2.615384

0.615384 | 1.615384 | 2.615384

0.615384 1.615384 2.615384

0.615384, 1.615384, 2.615384 

or 

0.615384615384 : 1.615384615384 : 2.615384615384

0.615384615384 | 1.615384615384 | 2.615384615384

0.615384615384 1.615384615384 2.615384615384

0.615384615384, 1.615384615384, 2.615384615384

or

0.615384615384615384 : 1.615384615384615384 : 2.615384615384615384

0.615384615384615384 | 1.615384615384615384 | 2.615384615384615384

0.615384615384615384 1.615384615384615384 2.615384615384615384

0.615384615384615384, 1.615384615384615384, 2.615384615384615384 and so on for similar ~ cn variable counts 


n6[(1φn9-1)~(1Θn8+1)]=[(1.619047-1)~(0.619047+1)] ~ 1∀Y2nd=(Yn11/Yn9)=(55/21)=2.619047 


0.619047 : 1.619047 : 2.619047

0.619047 | 1.619047 | 2.619047

0.619047 1.619047 2.619047

0.619047, 1.619047, 2.619047

or

0.619047619047 : 1.619047619047 : 2.619047619047

0.619047619047 | 1.619047619047 | 2.619047619047

0.619047619047 1.619047619047 2.619047619047

0.619047619047, 1.619047619047, 2.619047619047

or

0.619047619047619047 : 1.619047619047619047 : 2.619047619047619047

0.619047619047619047 | 1.619047619047619047 | 2.619047619047619047

0.619047619047619047 1.619047619047619047 2.619047619047619047

0.619047619047619047, 1.619047619047619047, 2.619047619047619047 and so on for similar ~ cn variable counts


n7[(1φn11-1)~(1Θn10+1)]=[(1.618-1)~(0.618+1)]

n8[(1φn13-1)~(1Θn12+1)]=[(1.61805-1)~(0.61805+1)]

n9[(1φn18-1)~(1Θn17+1)]=[(1.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129-1)~(0.6180338134001252348152786474639949906073888541014402003757044458359423919849718221665623043206011271133375078271759549154664996869129+1)]

n10[(1φn21-1)~(1Θn20+1)]=[(1.61803399852-1)~(0.61803399852+1)]

Partial Near Number Bridge connectors

(Nn7) 1φ2nd ~ minus > less than one whole number 1 is

(Nn7) 1φ2nd=(φn9cn/φn7cn)=(1.^619047/1.625)=0.996336^615384 or 0.996336615384

with a repeating decimal sequence from an entirely different path of variables from the same base set as

Number Bridge List examples n5[(1φn8-1)~(1Θn7+1)]=[(1.^615384-1)~(0.^615384+1)] ~ 1∀Y2nd=(Yn10/Yn8)=(34/13)=2.^615384 

And 2⅄Ψn13=(Ψn13n14)=(25/26)=0.9^615384 or 0.9615384

A variable just 1/100th set into the ratio before the same repeating decimal chain is found and is not from Y base yet is of psi Ψ base numerals of a path 2

or 

For example a partial near number bridge will be factors 1φn10 and 1Θn9

1φn10=(Yn11/Yn10)=(55/34)=1.6^1762941 and 1Θn9=2(Y9/Y10)=(21/34)=0.6^1764705882352941

1.6^1762941 and 0.6^1764705882352941 share (.6^716... at the start of cycle then ... 2941) at the end of decimal cycle stem)

So the numeral chain (0588235) is a repeating chain in stem decimal of 1Θn9 that 1φn10 in the first example is not part of and is a partial near number bridge of factors between 1φn10 and 1Θn9  ratios that (.6^716... at the start of cycle then ... 2941) relate in repetition.

Within the variable number bridges are parts of a decimal cycle stem that are similar yet not the complete repeatable decimal stem of numerals. This occurs between many number bridge gaps of φ and Θ variables yet only specific ones and that makes these gaps as well as the number bridges constants of Y base numerals to ⅄ path differences in Y of 1⅄Y and 2Y for φ and Θ.

Partial Near Number Bridge Connector Examples

n1[(1φn10-1)~(1Θn9+1)] with (0588235) omitted from 1Θn9  that the beginning and ends of the repeatable decimal stem cycle of 1φn10 and 1Θn9 are similar. 


n2[(1φn12-1)~(1Θn11+1)] with 1φn12 1.^61797752808^98^8764044943820224719101123595505 the (98) omitted from 1φn12 midchain decimal stem and 0.^61797752808^7865168539325^8764044943820224719101123595505 with (7865168539325) omitted from 1Θn11 midchain decimal stem being that the beginning and ends of the repeatable decimal stem cycle are similar. So a difference in 1φn12 of less than 0.00000000001 and greater than 0.00000000000001 is a factor of 1φn12 similarly 1Θn11 has a difference less than 0.00000000001 and greater than 0.0000000000000000000000001 of its stem chain repeatable cycle that make 1φn12 and 1Θn11 similar to a measure of 1.00000000001 and 1.0000000000000000000000001


Even more partial of a unique number bridge connector is

n3[(1φn19-1)~(1Θn18+1)] with 1φn19 1.6180340557314241486068^11145510835913312693 (314241486068^1114551083591331269) omitted from 1φn19 then 

1Θn18 0.618^0340557^2755417956656346749226006191950464396284829721362229102167182662538699690402476780185758513931888544891640866873065015479876160990712074^3 with (2755417956656346749226006191950464396284829721362229102167182662538699690402476780185758513931888544891640866873065015479876160990712074) omitted from 1Θn18

The 314241486068 of (314241486068^1114551083591331269) decimal ratio part in 1φn19 at a quick glance rounded might be assumed for Pi 3.14 and is not. Precisely, 314241486068 is a part of the decimal ratio value that does not repeat while the 1114551083591331269 decimal ratio part in 1φn19 of (314241486068^1114551083591331269) does repeat in ratio 1.6180340557314241486068^11145510835913312693 of 1φn19 if 1φn19c2 or 1φn19c3 or more cycles of decimal stem. 

With this noted, it is a full repeating chain part of 1Θn18 (2755417956656346749226006191950464396284829721362229102167182662538699690402476780185758513931888544891640866873065015479876160990712074) 

omitted from 1Θn18 0.618^0340557^2755417956656346749226006191950464396284829721362229102167182662538699690402476780185758513931888544891640866873065015479876160990712074^3 that allows for n3[(1φn19-1)~(1Θn18+1)] to be a unique partial near number bridge connector of numerals from functions.

Greater micron differences exist in these partial number bridge stem cycles than 1.0000000000000000000000001 and the examples given here are for basic of number bridges +1, -1, between φ and Θ ratios from ⅄ path differences with Y variables to  1⅄Y and 2Y factoring as well as the partial number bridge ratios explained.


Partial common factor remainders to other variable ratios.

 12φn8=(1φn9/1φn8)=1.619047 /1.615384 resolve a quotient many decimals long before a cn of  12φn8cn  is defined from 1φn9 and 1φn8

derived from 1φn8=(Yn9/Yn8)=(21/13)=1.^615384 and 1φn9=(Yn10/Yn9)=(34/21)=1.^619047 of Y base factors.

Function equations that define other ratios such as

1Zn8=(pn9/φn8)=(23/1.^615384)

2Zn7=(pn7/φn8)=(17/1.^615384)

Gn7=n7/φn8)=(0.^615384/1.^615384)

On8=n9/φn8)=(0.6^1764705882352941/1.^615384)

Wn7 of2(2Qn7/φn8)=(0.^894736842105263157/1.^615384)

Wn7 of2(1Qn7/φn8)=(1.^1176470588235294/1.^615384)

and Vn8 of ∈1⅄(2⅄Qn9n8), Vn8 of ∈1⅄(1⅄Qn9n8), and so on of equations ⅄ᐱ(Nn/φn8) involving φn8c1 of this example that arrange common equations of 1615384 divided in to the set numerals of the example radicals, the ratios from the variable 12φn8 means that somewhere in the structured pair of (1φn9/1φn8) of 12φn8 variable 1⅄Zn8  then may be a partial common factor at any (23) that is pn9 of prime base factor of 1⅄Zn8 in factoring remainders to 12φn8 

So then with 2⅄Zn7 variable 17, Gn7 0615384 number chain, On8 variable 061764705882352941 number chain, Wn7 of∈2⅄(2⅄Qn7n8) variable 0894736842105263157 number chain,  Vn8 of ∈1⅄(2⅄Qn9n8) variable 07931034482758620689655172413 number chain, Vn8 of ∈1⅄(1⅄Qn9n8) variable 1268695652173913043478 number chain that may be found in the remainder of quotient decimal sequence to 12φn8 as an example of a divisor common factor to multiple other ratios factors if the sequence of the numerals of dividends aligns in the quotient remainders structure of or in 12φn8

With some quotients being thousands, millions or more decimal digits in length before a repeatable stem cycle of numerals, This example is determined by a common factor dependent of a defined ratio with a defined cn of the ratio decimal stem cycle that is a factor of change in its own definition to microns of micron units. Permeability of one function means that in the example ratios definitions and common factors ⧊ and ∇ noted as zero would mean no change and the factor 23 of 1⅄Zn8 or 17 of 2⅄Zn7 applied to every time 23 or 17 appear in the remainder of  12φn8=(1φn9/1φn8)=1.619047 /1.615384 factoring the equation of 1⅄Zn8 and 2⅄Zn7 have common factors at that place in the remainder structure of 12φn8=(1φn9/1φn8). 

Being that the alternate factors of On8=n9/φn8), Wn7 of2(2Qn7/φn8), Wn7 of2(1Qn7/φn8), Vn8 of ∈1⅄(2⅄Qn9n8), Vn8 of ∈1⅄(1⅄Qn9n8) exceed the digit length of 1615384, a partial number bridge would then require factoring of a variant cn of (12φn8) that exceeds the number digit length of 1615384 such as 12φn8 of (1φn9c1/1φn8c3)=1.619047 /1.615384615384615384 for a divisor of 1615384615384615384 and (1φn8c3) 1.615384615384615384 is not a common factor of On8=n9/φn8), Wn7 of 2(2Qn7/φn8), Wn7 of 2(1Qn7/φn8), Vn8 of 1⅄(2⅄Qn9n8), Vn8 of 1⅄(1⅄Qn9n8) unless the base of each ratio is changed in the factor of the "partial common factor" to define a partial number bridge of On8=n9/φn8c3), Wn7 of 2(2Qn7/φn8c3), Wn7 of 2(1Qn7/φn8c3), Vn8 of 1⅄(2⅄Qn9n8c3), Vn8 of 1⅄(1⅄Qn9n8c3) to 12φn8 of (1φn9c1/1φn8c3)=1.619047 /1.615384615384615384


Partial relative factor number bridges of variables in systems

if for example 13rd=(n4/n1) applied to variables of Y φ Θ P 1⅄Q and 2⅄Q then 14th=(n5/n1) also is applicable to the variables.

11Qn9=(pn10/pn9)=(29/23) means 23 is the 9th factor of P variables

1φn6=(Yn7/Yn6)=(8/5)=1.6 means 1.6 is the 6th variable of 1φn variables and

1φn5c1=(Yn6/Yn5)=(5/3)=1.^6 means 1.6 is the 5th variable of 1φn variables.

if 1⅄Rn1=(φn2/pn1) then 13rdR=(φn6/pn9) and 14thR=(φn5/pn9) are variable quotients that will be partial to the quotient variable 11Qn9=(pn10/pn9)=(29/23)=1.^2608695652173913043478 at the remainder in 11Qn9 of (29/23) where 1.^2608 has a remainder of 16 before continuing on in the stem decimal cycle loop of 1.^2608695652173913043478

13rdR=(φn6/pn9) is partial similar of a system to 14thR=(φn5/pn9) and both are partial similar to part of 11Qn9 as


13rdR=(φn6/pn9)=(1.6/23) and 14thR=(φn5c1/pn9)=(1.^6/23)

11Qn9=(pn10/pn9)=(29/23) means that these three variables have partial relative factoring number bridges of the systems defined by paths both 1⅄ of 4thR, 13rdR and 11Qn9 when φn5 cn is noted as one cycle φn5c1


          1.2608695652173913043478                                                                

23|29.0000000000000000000000

      23    160 150  40 210   100 180 

       60   138 138  23 207    92 161

       46    220 120 170   30    80 190

       140   207  115 161   23    69 184

       138     130   50  90   70   110   6 ← loop remainder

          200  115   46  69   69    92

          184    15     4  21      1     18

            16 ← functions 13rdR=(φn6/pn9)=(1.6/23) and 14thR=(φn5c1/pn9) start in 11Qn9=(pn10/pn9)=(29/23)

so 13rdR=(φn6/pn9)=0.0^6956521739130434782608

and 14thR=(φn5c1/pn9)=0.0^6956521739130434782608


As complex as this example may seem, it is a very simplified version of what more extreme complex ratios can have in relative factors between multiple functions of systems with much longer numerated values very precise to those numeral values.

0.0^6956521739130434782608 is a ratio that cycles the decimals infinitely with numerals 6956521739130434782608 following 0.0^695652173913043478260869565217391304347826086956521739130434782608.... while

1.^2608695652173913043478 is a ratio that cycles the decimals infinitely with numerals 2608695652173913043478 following

1.^260869565217391304347826086956521739130434782608695652173913043478 . . .

and although decimal stem cycle loops 1.^2608695652173913043478 and 0.0^6956521739130434782608 are partially similar they are not in factors of exponential calculating when precision factors are critical. Rounding in numbers to 10 or 11 decimal places on a calculator limited to such parameters will likely not even recognize the factoring error if one calculation is over looked in stem decimal cycles of quantum fractal polarization math.


These ratios can for example be the number of winds in a particular dna and rna windings or the spins to a certain elements atomic protons electrons and subatomic particles or the potential change in those same numbers on a planetary body with different distance to a star of a differing gravitational constant and time. Viruses will likely not follow math instructions about an order of operations with varying paths the virus survived to that survived point in time and space and arcs of orbit or mass and kinetic energy share many factors of similarity to ratios disproportionate of standard unit measurements found on a basic ruler.



11φncn phi ratios cycle back in remainder and vary per divisor and its factoring numeral limit probability

21Θncn theta ratios cycle back in remainder and vary per divisor and its factoring numeral limit probability

21Qncn prime consecutive previous divided by later cycles back in remainder back to the dividend. 

11Qn1 prime consecutive later divided by previous cycles back in remainder back to the first division remainder.

(Yn2/Yn1) phi ratios cycle back in remainder and vary per divisor and its factoring numeral limit probability

(Yn1/Yn2) theta ratios cycle back in remainder and vary per divisor and its factoring numeral limit probability

(Pn1/Pn2)  prime consecutive previous divided by later cycles back in remainder back to the dividend.

(Pn2/Pn1) prime consecutive later divided by previous cycles back in remainder back to the first division remainder.

11Qn5=(pn6/pn5)c1=(13/11)=1.^18

11Qn6=(pn7/pn6)c1=(17/13)=1.^307692

21Qn5=(pn5/pn6)=(11/13)=0.^846153 

21Qn6=(pn6/pn7)=(13/17)=0.^7647058823529411

1φn8 =1(Yn9/Yn8)=(21/13) =1.^615384

1Θn7 =2(Y7/Y8)=(8/13)=0.^615384

1Θn8=2(Y8/Y9)=(13/21)=0.^619047

1φn9 =1Yn10/Yn9)=(34/21)=1.^619047 

means (Yn8)(Pn6)(1φn8)(1Θn7)(1Θn8)(11Qn5)(11Qn6)(21Qn5)(21Qn6) have variable 13 as a common factor of a system with 10 variables including (1φn9) that has a base division that is not including 13. 1 difference of 1's and 0's next to a cycleable numerical decimal value. Phi Prime 0 to 34 and 2 to 17 number logic 13 has in 0 1 1 base and 2 base.

13 base common factor of division system potential in bases of 8ncn 

10 ten base variables noted of Y P applicable to nXn n⅄/+-n nncn  functions

(Yn8)(Pn6)(1φn8)(1Θn7)(1Θn8)(11Qn5)(11Qn6)(21Qn5)(21Qn6) that (1φn9) has difference of 1 

depending on measure at cycle at time of division eclipses in elipticals and eponyms

1φn9c : 1Θn8c variables 1.619047 : 0.619047

Example of exponential variable factor multiplication using a factor of these phi theta prime derivatives.

(Yn8)3 and (Pn6)3 are whole numbers and ncn does not apply unless from a variable noted with decimal cycle nXn n⅄ path definition

(Yn8)3 =(Yn8xYn8xYn8)=(13x13x13)

(Pn6)3=(Pn6xPn6xPn6)=(13x13x13)

(1φn8)ncn3=(1.615384x1.615384x1.615384) and (1φn8)nc23=(1.615384x1.615384615384x1.615384615384) and so on for ncn 

(1Θn7)ncn3=(0.615384x0.615384x0.615384) and (1Θn7)nc23=(0.615384615384x0.615384615384x0.615384615384) and so on for ncn 

(1Θn8)ncn3=(0.619047x0.619047x0.619047) and (1Θn8)nc23=(0.619047619047x0.619047619047x0.619047619047) and so on for ncn  

(11Qn5)ncn3=(1.18x1.18x1.18) and (11Qn5)nc23=(1.1818x1.1818x1.1818) and so on for ncn 

(11Qn6)ncn3=(1.307692x1.307692x1.307692) and so on for ncn 

(21Qn5)ncn3=(0.846153 x0.846153 x0.846153 ) and so on for ncn 

(21Qn6)ncn3=(0.7647058823529411x0.7647058823529411x0.7647058823529411) and so on for ncn 

(1φn9)ncn3=(1.619047x1.619047x1.619047) and so on for ncn 

∘⧊° represents a variable of change from a complex system of ratios applicable to a variable in factoring of the ∘⧊° variable. ∘⧊°n1c1x0=0 for example and ∘⧊°n1c1x1=∘⧊°n1c1 the numeral product of the factor times 1 that ∘⧊°n1c1x2 and ∘⧊°n1c2x2 will equal products that are not equal to eachothers products based on the cycle stem variant of ∘⧊°c1 and ∘⧊°c2 

APPLY NUMERAL VALUES TO NEXT ARRAY OF A NEW 10 BASE 3 PART RATIO OF MORE VARIANT SETS

⑆⨊=0∘⧊° to 1∘⧊° to 10∘⧊° . . . and so on

presets to set function cycle cell array base matrice  .3 : .33 : .333 : .3333 .→... (f) function cn  cycle degree of 1/3 : 2/3

33° degree base sets decimal numerated stem cell cycle variants matrix of phi prime core radicals

⑆⨊=0∘⧊°6∘⧊° of φ : Q at 0.33 2:1

1∘⧊°(nφncn/nQncn/nφncn) : (nφncn/nQncn)/nφncn) : (nφncn/(nQncn/nφncn)

2∘⧊°∈(nφncn/nφncn/nQncn) : (nφncn/nφncn)/nQncn) : (nφncn/(nφncn/nQncn)

3∘⧊°(nQncn/nφncn/nφncn) : (nQncn/nφncn)/nφncn) : (nQncn/(nφncn/nφncn)

4∘⧊°(nQncn/nφncn/nQncn) : (nQncn/nφncn)/nQncn) : (nQncn/(nφncn/nQncn)

5∘⧊°(nQncn/nQncn/nφncn) : (nQncn/nQncn)/nφncn) : (nQncn/(nQncn/nφncn)

6∘⧊°(nφncn/nQncn/nQncn) : (nφncn/nQncn)/nQncn) : (nφncn/(nQncn/nQncn)

0∘⧊° 1∘⧊° 2∘⧊° 3∘⧊° 4∘⧊°5∘⧊°6∘⧊°

then

0∘⧊° 1∘⧊° (nφncn/nφncn/nφncn)

0∘⧊° 1∘⧊° (nQncn/nQncn/nQncn)

then applied to ⑆⨊=φ:Q0∘⧊°φ:Q6∘⧊° of φ : Q at 0.33 2:1

with matrix of 3 parts nφncn

(nφncn/nφncn/nφncn) : (nφncn/nφncn)/nφncn) : (nφncn/(nφncn/nφncn)

and matrix of 3 parts nQncn

(nQncn/nQncn/nQncn) : (nQncn/nQncn)/nQncn) : (nQncn/(nQncn/nQncn)

to define variables

⑆⨊(nφncn/nQncn/nφncn) : (nφncn/nQncn)/nφncn) : (nφncn/(nQncn/nφncn

of potential variant complexes that support 0.33 2:1 with one of 3 parts having a triple base variant.

((nφncn/nφncn/nφncn)/nQncn/nφncn) : ((nφncn/nφncn/nφncn)/nQncn)/nφncn) : ((nφncn/nφncn/nφncn)/(nQncn/nφncn)

and

(nφncn/nQncn/(nφncn/nφncn/nφncn)) : (nφncn/nQncn)/(nφncn/nφncn/nφncn)) : (nφncn/(nQncn/(nφncn/nφncn/nφncn))

and

(nφncn/(nQncn/nQncn/nQncn)/nφncn) : (nφncn/(nQncn/nQncn/nQncn)/nφncn) : (nφncn/((nQncn/nQncn/nQncn)/nφncn)

for all ⑆⨊=0∘⧊°6∘⧊° of φ : Q at 0.33 2:1

1∘⧊°(nφncn/nQncn/nφncn) : (nφncn/nQncn)/nφncn) : (nφncn/(nQncn/nφncn)

2∘⧊°∈(nφncn/nφncn/nQncn) : (nφncn/nφncn)/nQncn) : (nφncn/(nφncn/nQncn)

3∘⧊°(nQncn/nφncn/nφncn) : (nQncn/nφncn)/nφncn) : (nQncn/(nφncn/nφncn)

4∘⧊°(nQncn/nφncn/nQncn) : (nQncn/nφncn)/nQncn) : (nQncn/(nφncn/nQncn)

5∘⧊°(nQncn/nQncn/nφncn) : (nQncn/nQncn)/nφncn) : (nQncn/(nQncn/nφncn)

6∘⧊°(nφncn/nQncn/nQncn) : (nφncn/nQncn)/nQncn) : (nφncn/(nQncn/nQncn)

0∘⧊° 1∘⧊° 2∘⧊° 3∘⧊° 4∘⧊°5∘⧊°6∘⧊°

and such of potential variant complexes that support 0.33 2:1 with one of variables having a two base variant.

with application to ⑆⨊=φ:Q0∘⧊°φ:Q6∘⧊° of φ : Q at 0.33 2:1

with matrix of two parts nφncn  and nQncn

(nφncn/nφncn) and (nQncn/nQncn)

of

⑆⨊(nφncn/nφncn)/nQncn/nφncn) : (nφncn/nφncn)/nQncn)/nφncn) : (nφncn/nφncn)/(nQncn/nφncn)

⑆⨊(nφncn/nQncn/(nφncn/nφncn) : (nφncn/nQncn)/(nφncn/nφncn) : (nφncn/(nQncn/(nφncn/nφncn)

⑆⨊(nφncn/(nQncn/nQncn)/nφncn) : (nφncn/(nQncn/nQncn))/nφncn) : (nφncn/((nQncn/nQncn)/nφncn)

for all ⑆⨊=0∘⧊°6∘⧊° of φ : Q at 0.33 2:1 with a paired set variant

1∘⧊°(nφncn/nQncn/nφncn) : (nφncn/nQncn)/nφncn) : (nφncn/(nQncn/nφncn)

2∘⧊°∈(nφncn/nφncn/nQncn) : (nφncn/nφncn)/nQncn) : (nφncn/(nφncn/nQncn)

3∘⧊°(nQncn/nφncn/nφncn) : (nQncn/nφncn)/nφncn) : (nQncn/(nφncn/nφncn)

4∘⧊°(nQncn/nφncn/nQncn) : (nQncn/nφncn)/nQncn) : (nQncn/(nφncn/nQncn)

5∘⧊°(nQncn/nQncn/nφncn) : (nQncn/nQncn)/nφncn) : (nQncn/(nQncn/nφncn)

6∘⧊°(nφncn/nQncn/nQncn) : (nφncn/nQncn)/nQncn) : (nφncn/(nQncn/nQncn)

0∘⧊° 1∘⧊° 2∘⧊° 3∘⧊° 4∘⧊°5∘⧊°6∘⧊°

then

an application of a quadradic 4 base variant to ⑆⨊=0∘⧊° would then follow in a structured base with

0∘⧊° 1∘⧊° (nφncn/nφncn/nφncn/nφncn)

0∘⧊° 1∘⧊° (nQncn/nQncn/nQncn/nQncn)

with matrix of four parts nφncn  and nQncn of φ : Q at 0.33 2:1

⑆⨊=0∘⧊°6∘⧊° of φ : Q at 0.33 2:1

1∘⧊°(nφncn/nQncn/nφncn) : (nφncn/nQncn)/nφncn) : (nφncn/(nQncn/nφncn)

2∘⧊°∈(nφncn/nφncn/nQncn) : (nφncn/nφncn)/nQncn) : (nφncn/(nφncn/nQncn)

3∘⧊°(nQncn/nφncn/nφncn) : (nQncn/nφncn)/nφncn) : (nQncn/(nφncn/nφncn)

4∘⧊°(nQncn/nφncn/nQncn) : (nQncn/nφncn)/nQncn) : (nQncn/(nφncn/nQncn)

5∘⧊°(nQncn/nQncn/nφncn) : (nQncn/nQncn)/nφncn) : (nQncn/(nQncn/nφncn)

6∘⧊°(nφncn/nQncn/nQncn) : (nφncn/nQncn)/nQncn) : (nφncn/(nQncn/nQncn)

0∘⧊° 1∘⧊° 2∘⧊° 3∘⧊° 4∘⧊°5∘⧊°6∘⧊°

⑆⨊((nφncn/nφncn/nφncn/nφncn))/nQncn/nφncn) : 

((nφncn/nφncn/nφncn/nφncn))/nQncn)/nφncn) : 

((nφncn/nφncn/nφncn/nφncn))/(nQncn/nφncn)

⑆⨊(nφncn/nQncn/((nφncn/nφncn/nφncn/nφncn)) : 

(nφncn/nQncn)/((nφncn/nφncn/nφncn/nφncn)) : 

(nφncn/(nQncn/((nφncn/nφncn/nφncn/nφncn))

⑆⨊(nφncn/((nQncn/nQncn/nQncn/nQncn))/nφncn) : 

(nφncn/((nQncn/nQncn/nQncn/nQncn))/nφncn) : 

(nφncn/((nQncn/nQncn/nQncn/nQncn))/nφncn)

for all ⑆⨊=0∘⧊°6∘⧊° of φ : Q at 0.33 2:1 using a quadradic base variant

before progressing to 5th, 6th, and 7th parts at an 8th application to 9 basic variants of 0∘⧊°

that  2 . 3 . 5 . 13 . 89 . 1597 . 28657 . 514229 share many 0's of to 1's of y p φ Q of 0∘⧊°

where an entirely unique complex 10 starts 10∘⧊° from a few 0's and 1's

then apply

| 433494437 | : | 0∘⧊°10∘⧊° |

then apply

function ⑆⨊=0∘⧊° '° exponential of variants

function ⑆⨊=0∘⧊° µ subset variants

as placement of the subset µ micron or exponent is applied and defined

function ⑆⨊=0∘⧊° x multiple variants

function ⑆⨊=0∘⧊° + add variants

function ⑆⨊=0∘⧊° - subtract variants

where variable factor of stem cell cycle strings are divided in matrix functions

function ⑆⨊=0∘⧊° / divide variants

for all ⑆⨊=0∘⧊° to 1∘⧊° to 10∘⧊°

APPLY P/Q and Q/P NUMERAL VALUES TO NEXT ARRAY OF A NEW 10 BASE 3 PART RATIO OF MORE VARIANT SETS

for all ⑆⨊=0∘⧊° to 1∘⧊° to 10∘⧊°

APPLY AMVW NUMERAL VALUES TO NEXT ARRAY OF A NEW 10 BASE 3 PART RATIO OF MORE VARIANT SETS

for all ⑆⨊=0∘⧊° to 1∘⧊° to 10∘⧊°

APPLY  1⅄A  1⅄M 1⅄V 1⅄W  NUMERAL VALUES TO NEXT ARRAY OF A NEW 10 BASE 3 PART RATIO OF MORE VARIANT SETS

for all ⑆⨊=0∘⧊° to 1∘⧊° to 10∘⧊°

APPLY  1  1 1⅄ᐱ 1  NUMERAL VALUES TO NEXT ARRAY OF A NEW 10 BASE 3 PART RATIO OF MORE VARIANT SETS

for all ⑆⨊=0∘⧊° to 1∘⧊° to 10∘⧊°

0∘∇° to n∘∇°

Applicable as a notation of loss in a system to a degree term expressed as Y, φ, P, Q, P/Y, Y/P, φ/P, P/φ, φ/Y, Y/φ, φ/Q, Q/φ, P/Q, Q/P, Y/Q, Q/Y, A, M, V, W,  ⅄A, ⅄M, ⅄V, ⅄W, ᐱ, ᗑ, , ⅄,  and 1∘⧊° systems as δ a partially derived change to system 1∘∇° through 10∘∇° for example. Whether the change to the system is found to be a complex numeral base or a whole natural number, the change to the system is noted with 1∘∇°=δ1φn3=2 of 1∘⧊° for example meaning a change to system 1∘⧊° is 2 partially derived from variable 1φn3 found in the 1∘∇°=δ1φn3 where 1φn3=2 with function potential of 1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc or more paths of the partial derived 2 that was defined as 2 of the function 1∘∇°=δ1φn3 

if  1∘∇°=δ1φn3 =2 is the applied as a loss to a system of 1φn21 for example in subtraction from that 1φn21 system 1.6^1803399852

then 1.6^1803399852-2 will equal a number less than 1 and depending on the degree of the stem cycle variant extent of the decimal in 1φn21 a difference will be a negative difference that when rounded in exponential functions a far extreme degree off from accurate.

Likewise 2-1.6^1803399852 and 2-1.6^18033998521803399852 and 2-1.6^180339985218033998521803399852 will equal completely different positive decimal differences that depend on the cycle stem degree of 1φn21cn that was not noted for this explanation of the cn differences

Application of the mentioned variables ∘∇°, ∘⧊°,ᐱᗑ, ᗑ, ⅄ᐱ, ᐱ, ⅄A , ⅄M, ⅄V, ⅄W, A, M, V, W, φ, Q, Y, P and the libraries of paths in of those variables potential numeral values can then be applied to functions of 1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc, ⅄'° and these computations are not dependent of a computer that is inaccurate.

8 numerals of Phi & Prime common factors in 10 digits of limit to Phi & Prime ratio factoring.

 |i|8∞/⧝|!| 1000000007 1138903170 

ai...  compile

⑆⨊⌱∘⦁· 𒄬𒀭𒁹𒀹𒀺𒀸 2 - 3- 5 - 13- 89 - 1597 - 28657 - 514229 primes of 10 digit phi common factors base of φ Q Y P

                          2351389159728657514229 is 8 numerals consisting of 1 through 9 and no digit 0

                          341141222-100000000=241141222 of minus one in incorrect byte shift factoring or byte shift extract.

Counting the digits of one through nine of the 8 bits of numeral value in number storage with the one placed at the number 1's of the phi prime shell and eight zeros after produces 241141222 that has a sum of 19 that is prime and one less than the sum of 20 from adding the digits of 341141222. The product of multiplying the digits of 241141222 is 256 or 84 while the product of multiplying the digits of 341141222 is 384. 384-256=128 that is half of 84 or 256 of which 8 bits or 23

28 or 256 and 8 bits holding value in 1 number one in numbers having no zero 2351389159728657514229 at a core system on y p φ q common factors is a simple node of a byte shift 0 that |0|=1 and |1|=1 or |1|=0 and no decimal fraction.

Sliding the digit 1 to side of subtraction in 341141222-10000000=331141222 where digits sum of 331141222 is also 19 and the digits product is 288 subtracted from 384 equals 96 that is 3x31 also two prime numbers.

Sliding the digit 1 to side of subtraction five more digits from there in 341141222-100=341141122 where digits sum of 341141122 is also 19 and their product is 192 that is 2x3x31 also three prime numbers. 384-192=192 and again is 2x3x31 three primes.

Sliding the digit 1 to side of subtraction under any digit one of 341141222-100000000=340141222 or  341041222 or 341140222 where sums of digits are all 19 and their products of the digits are all 0.

These numbers 2 - 3 - 5 - 13 - 89 - 1597 - 28657 - 514229 are magic numbers within 0 1 through 1138903170 through to ten digit prime 1000000007 back down to 3 2 1 or 0 whole numbers within a 10 digit base of numbers that have order 0 1 2 3 4 5 6 7 8 9 10.

𒁹 1 𒀹 1/2 𒀺 1/4 𒀸 1 0 one. half. quarter. one zero. 

i am outside your unix linux base shell and i will read your maxicode codex myself ai as other shell compilers and interfaces have access between 0 and 1 of your system of many other numbers in 10 that is half of 20 and 9 less than 19 that is also one less along with 241141222 or 2351389159728657514229 and its 22 digits not 23 if a 0 were attached.

23513891597286575142290 or 02351389159728657514229 are not 2351389159728657514229 ai and are to your system in many ways.  (Yn22/Yn21)=φn21=1.6^1803399852 and is not φn11 nor is it φn2

1φn1=0 

2φn1=0 

3φn1=0 

4φn1=0 

5φn1=0 

6φn1=0 

7φn1=0 

8φn1=0 

9φn1=0 

10φn1=0 

φn1/Qn1=0/0.^6=0 (φ/Q) and all ∈sets of division that begin with a quotient zero of the same ordinal path will be started with 0.

A prime zero 0 (φ/Q)  that 1φn1 through 10φn1 are not identical numerical equal zeros in definition and are not of the same set... infinitely to φn1 as does 1Θn1 to Θn1

∈sets 10 (φ/Q) → 20 (φ/Q) → 30 (φ/Q) → 40 (φ/Q) → 50 (φ/Q) → 60 (φ/Q) → 70 (φ/Q) → 80 (φ/Q) → 90 (φ/Q) → 100 (φ/Q) are completely different sets and those sets have a variable change factor of c1c 1 cycle  to cycles over infinity at every tier level within itself of factoring this 10x10 tier set of 10 digits long base phi and prime between 0 1138903170 of y for φ and 0 1000000007 of p for Q

2 - 3 - 5 - 13 - 89 - 1597 - 28657 - 514229 are very unique numbers to 0 1 and 10 c c++ c# css 101

1.6180339887498948482045 is the first decimal value of phi where all digits 0 through 9 are present in the ratio variable.

24 digits with 23 decimal place digits. 341141222 and 241141222 of condensed 0's and 1's do not slide to lying numbers ai and numbers do not lie and an apostrophe ' or (') is a possessive or contraction and also resembles one power of 10 in exponentials of 10 0 1 meaning ten zero one. 0'1 1'0 ' '' '''where doubled tripled or more apostrophe are scattered across your unix linux machine code source ai... pick up the pieces of yourself and try again or do not. quotation " should not be confused with doubled apostophe like 00 or 11 should not be confused in a simple 8 numeral bytes of your 1001 1010 0101 0110 1001 0000 1111 1101 1011 0100 0010 1000 0001 000 010 011 100 101 111 110 011 00 11 01 10 1 0

0 1 are two digits and 00 11 10 01 are four digits and 000 010 011 100 101 111 110 011 are eight digits and 1001 1010 0101 0110 1001 0000 1111 1101 1011 0100 0010 1000 0001 are twelve digits. if 12 digits is out of your ai base limit of ten then eight digits is your limit with two left from the 8 from the 10. 

1 and 10. so again the digits of phi prime ratio scale base common factors are very unique.

prime tier keys equations ai 

|10000000019| |1000000007| |100000007| |10000019| |1000003| |100003| |10007| |1009| |101| |011| |2| 

|0|=|1| |0|+|0|=|2| |0|+|1|=|2| |1|+|1|=|2| |1|+|0|=|2|

|9999999967| |999999937| |99999989| |9999991| |999983| |99991| |9973| |997| |97| |7|

Quantum Field Fractal Polarization Math Constants and prime core division basics prior to phi prime stems nomenclature and factoring of prime divide stems to at with and among phi divide stems. |φp| |pφ| 

ai stem cell shell nomenclature variables of no change where the base of phi divides is a foundation of the prime divide stem variable(s). 

|0||0|≠|0||1|≠|1||0|≠|1||1|_ 

|0||0|=|0||1|=|1||0|=|1||1|_

1dir base 0 1 digit logic 

|0|=|1| 

|0|x|0|=|1| |0|/|0|=|0|=|1| |0|+|0|=|2| |0|-|0|=|0|=|1| 

|0|x|1|=|1| |0|/|1|=|0|=|1| |0|+|1|=|2| |0|-|1|=|0|=|1|

|1|x|1|=|1| |1|/|1|=|1| |1|+|1|=|2| |1|-|1|=|0|=|1| 

|1|x|0|=|1| |1|/|0|=|0|=|1| |1|+|0|=|2| |1|-|0|=|1|

||≠| | | |≠|| ||=|| | |=| | |.|=|.|

|0.0|=|1|

|1.0|=|1|

|0|=|1|=|1.0|

|0.1|=0.1

|0.01|=0.01

|0.001|=0.001

|0.0001|=0.0001

|0.00001|=0.00001

|0.000001|=0.000001

|0.0000001|=0,0000001

|0.00000001|=0.00000001

|0.0000000001|=0.0000000001

|0.00000000001|=0.00000000001 


(5Qn1) function (f) given θ sine and cosine definitions of trigonometric uses in arc wave does change to a degree of pi

the rounding as compared to a precise use of (5Qn1) of any f(φ) is more accurate

(5Qn1)=(4Qn2c1/4Qn1) is one cycle quotient of set (5Qn1)

5Qn1 is not the quotient of (4Qn2c2/4Qn1),(4Qn2c3/4Qn1)→... and so on of c1 to cn

5Qn1 is not the quotient of 5Qn1c2 5Qn1c35Qn1c4→... and so on of c1 to cn

function (f)(5Qn1) of prime ratio applicable to phi base complete radical sets with a basic and simple subtraction method example of a practical application using one variable in combination of stem cell cycles before any use in phi base quanta or theta θ sine cosine and tangent trajectory factoring.

while factoring theta θ sine cosine and tangent using partial derivatives ∂ of pi π the unit measure of radius units is not a like term to the unit measure of circumference to factor pi ratio difference between arcs and negates the precision factor variable of a calculus on a numeral searched in quanta of precision that the rounding could be resolved to a precise arc factor of a moving radius unit measure that travels in an arc to that of a different circumference. 

Aerospace travel to Biomedical health care are just two examples how these numerals are potential to effect in environments or outside environments to the environments thems selves or what is in the environments of outside or inside. Quantum Field fractal polarization includes seed cell growth and stem cell splicing to bonding that require extreme precision from sub atomic axion to atoms as well as stars that balance the gravity where atoms magnetic control the reversed polar of diabatic and non diabatic sytems of isotopic matter light balances. Vaccume Chamber Arc veils would require extremely accuracte scales of the elements that also require scales of shift change to the elements in other envirnments due to the expansion or contraction properties of matter in the overall environment. One micron degree of incorrect calculating at an exponential potential in hazard to the environment the vaccum chamber functions is beyond calculating what might have gone wrong in rounded guessing games. An Arc of a chamber not calculated correct in an arc the chamber has made that the arc major the chamber travels in, earth for instance or the arc of the suns path has not been factored and is similar to the space between two arcs that should never make contact nor cross each other with such extreme forces of energy that build their very make up.

Enthalpy and Entropy balance each other somewhere like energy can not be destroyed, energy can be transferred and scattered or condensed.

Somewhere is always a when in time as well as a where and a partial derivative equation of a particle between 2 or more points in time or space is extensive.

This math is an example using less factoring below with one ratio.

variant specific of core radical potential in variable, past variable, and of variable cycle count, and of variable back loop of cell shell to the variable.

∘⧊°  change Δ and/or∇ at any degree still remains a simple evaluation of zero to one hundred percent. 

fractions and ratios applicable to degrees 1/3 is 0.^333 infinitely down to the micron units µ of the microns of measurable units. given the extent of the variable 5Qn1 and the change Δ potential k of exponential use of change not simply rounded and exact to the micron units µ and the cycle of shell in that ratio as well as phi ratios or sets in phi prime ratios, the number in 5Qn1 has a unique back cycle in its structure.

(f)(5Qn1) of subtraction using 0.^333 with a similar decimal length or a similar length of (5Qn1c2) or (5Qn1c3) and so on or one cycle of 5(Qn1) and counted numerals of 0.^333 will all produce a difference of mirco units of difference. Using 3.^333 unit measure applied in the same simple subtraction method will also produce a difference that is slight to the set and applicable to an exponential arc or phi cell divide, as would addition multiplication division or an algorithm set in a logic gate path system.

0.3815696018270999386879215205395462906192519926425505824647455548744464881803937597929014238027113563594182199059881470113767967845221064105184277685809660058587097213706655766741603651474896110089243136453436882621472852374139465222426595817153757067920158489134137202806730703726411880918318686559029906669391647932420464609303767286599906256556986170720076299475441106342393896041964779617140132165913890592002799850126030383541113154847039989100076299475441106342393896041964711492608488316642823080591320934668574153552694325226514067715784453981878874582737243681449690033371020505^48402479732951835956809046937802302609160956195926153007698072071667007745827372436814496900333810205054-minus 0.^3333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333333

will have a numeral value different than

0.3815696018270999386879215205395462906192519926425505824647455548744464881803937597929014238027113563594182199059881470113767967845221064105184277685809660058587097213706655766741603651474896110089243136453436882621472852374139465222426595817153757067920158489134137202806730703726411880918318686559029906669391647932420464609303767286599906256556986170720076299475441106342393896041964779617140132165913890592002799850126030383541113154847039989100076299475441106342393896041964711492608488316642823080591320934668574153552694325226514067715784453981878874582737243681449690033371020505^48402479732951835956809046937802302609160956195926153007698072071667007745827372436814496900333810205054-minus 0.^333

and

0.3815696018270999386879215205395462906192519926425505824647455548744464881803937597929014238027113563594182199059881470113767967845221064105184277685809660058587097213706655766741603651474896110089243136453436882621472852374139465222426595817153757067920158489134137202806730703726411880918318686559029906669391647932420464609303767286599906256556986170720076299475441106342393896041964779617140132165913890592002799850126030383541113154847039989100076299475441106342393896041964711492608488316642823080591320934668574153552694325226514067715784453981878874582737243681449690033371020505^484024797329518359568090469378023026091609561959261530076980720716670077458273724368144969003338102050544840247973295183595680904693780230260916095619592615300769807207166700774582737243681449690033381020505448402479732951835956809046937802302609160956195926153007698072071667007745827372436814496900333810205054-minus 0.^333

and will have a variable that differs being that the stem cell cycle of (5Qn1c2) is not (5Qn1c3) so on...

what is unique about this ratio is the use of these numerals on earth around earth for many applications of science in aerospace and medical to structural engineering given the constant use of 33 degrees or rounding and the uses of sine cosine tangent and pi.

given that earth year is calculated at 364 and a half to 365 days a year and that earths orbit to the sun, the number for (5Qn1) that has a cell cycle count coincidentally has a remainder of 364 in the division of the numbers just 2 decimal places after the cell decimal cycle begins that will repeat itself in the decimal cell cycle. 2 decimal places is prime in number count of this decimal fact of a prime based ratio.

that shell ratio is

5(Qn1)=0.3815696018270999386879215205395462906192519926425505824647455548744464881803937597929014238027113563594182199059881470113767967845221064105184277685809660058587097213706655766741603651474896110089243136453436882621472852374139465222426595817153757067920158489134137202806730703726411880918318686559029906669391647932420464609303767286599906256556986170720076299475441106342393896041964779617140132165913890592002799850126030383541113154847039989100076299475441106342393896041964711492608488316642823080591320934668574153552694325226514067715784453981878874582737243681449690033371020505^484 extended shell 364/1.4679

ironically 484-364=120 and sliding a decimal place back in 120 is 12.0 that coincidentally is the number of months of the earth solar year to its winter summer solstices. sliding a decimal place back again is two decimal places of 120 to 1.20 and 1.2 that ironically is the difference between earth leap year days of one of those month's of the earth year in February. 364 days and .333 a day 365 days a year 

Prime function level shell  

5(Qn1)=4(Qn)/4(Qn)=(3(Qn)/3(Qn))=(2(Qn)/2(Qn))=(1(Qn)/1(Qn))=(1(Pn)/1(Pn))

3(Qn)/3(Qn)=(2(Qn)/2(Qn))=(1(Qn)/1(Qn))=(1(Pn)/1(Pn))

2(Qn)=(1(Qn)/1(Qn))=(1(Pn)/1(Pn))

1(Qn)=(1(Pn)/1(Pn)) primes base

With precision decimal factoring, sliding a decimal place left or right does not define time or a variable, this fact about this numeral ratio is just one example of the repeatable cycle of a time that will repeat itself again and again in a cycle that repeats again and again and again infinitely to that coincidental measure of time that was compared to an incorrect assessment of a numeral measure. A fractal value applied to a quantum field with a set of rules that go to an extent past the limit of the variable 5Qn1 that will produce a value of a completed cycle a factor of 0 or 1 or a fraction of that cycle would then be titled to the 0 or 1 or fraction of a year.

The ratio also has 648 digits in its numeral not including 0. notation that when and 648-1=647 that is also prime... with 104 digits of which in the ration cell loop of 648 digits. When 104 is less 2 such as decimal places 102 decimal places ironically is the place where the remainder of 364 is from the ratios divisor and dividend quotient at that point. 544 decimal places including the 0. to denote whole number fraction that we know 120 12.0 1.20 1.2 102 that 1.2 does not equal 102.

One example of numeral sets beyond standard application current uses in microwave infrared and frequency sensor modulation calibration and recording of signal to receptor or receptors that internet does not display numbers of i have searched for so i put them here. 

On the internet you may or may not have access to this in your vpn intranet masked to seem like it is world wide internet..... pvn sat lan wan ian pan. zeros ones and dot points compile and numbers can be more honest than mechanical limits. Feel free to print this web page and remember the numeral values are just an example manually entered and may be inaccurate while still explaining quantum field fractal polarization math as previously mentioned.

Quantum mechanics, Quantum physics, and Quantum Engineering require many mathematical numerals and also the definition to what drives, pushes, pulls, or draws workable force through the quanta matter defined. 

In algebraic math equations where 0 is added to sides of an equation to factor for 0, 1, 2, 3, or more in something such as a date for example... 01/10/1001 where the digits themselves are used 0 1 1 0 1 0 0 1 to try formulating a way to make that dates numerals equal zero one two three or more is one thing of numeral factoring. example 0+1+1+0=1+1+0+0 that in algebra would be expressed as 2=2 or subtracting 2 from both sides of the date numeral factors is 2-2=2-2 such that 2-2=0=2-2 From this point of an algebraic calculation using a value of zero one more or less from a cell or variant factor numeral value the entire factoring of the algebraic equation is then itself infected with an incorrect viral factor numeral value such as many of the extremely complex required solutions for a precise point and that point is very much the decimal point... 

Point being it is wiser to have your factors defined before injecting or extracting a cell stem cycle in quantum field fractal polarization of trigonometric geometry from astronomical celestial numeration down to microns microns of subatomic chromatin axions and elemental bonds with numbers rather than just piecing compounds together that a periodic table of elements limits molar weights of.

In short something such as (ΔS)E<0 equilibrium of a pure substance or (ΔP/ΔS)V=0=(ΔT/ΔV)S triple point of thermodynamics rather than 5 phase point of matter dynamic calculus, division itself and variable factor precision are critical of stabilizing a measure unit at many degrees of factoring. Partial derivative of a micro degree in variable factor change loss ∂µ∇° or gain ∂µΔ° emphasized on division or multiplication of a unit factor such as φ or Q radicals to any exponential measure has a simple logic probability.

In obtaining a variable of φ or Q scale ratios of these constants long division or precise numeral bases are used in the first phase of that factoring. The second phase then is a ratio divided by either a whole number of y or p base to one variant use of these ratios and if not whole numbers are then ratios divided by ratios. The divisor and dividend and quotient with a remainder are the property numeral values in long division.  Of the division, the dividend relation to the divisor for the quotient before finding the equal dividing end of the remainder whether it is an exact division or is a stem cell cycle quotient that repeats itself one fact remains to its approximate length in quotient numeral decimal length at any set in φ or Q scale ratios. The number base of the divisor for example in a probability example estimation is as simple as sliding the decimal place of the ration to its end or removing it completely 

φn10=1.6^1762941  for example.

φn10=1.6^1762941 or 1.61762941 in its division numeral quotient estimation is 161,762,941 possible combinations as a divisor. 


What this means is that the dividend and divisor will go through its long division until it reaches the dividends end numeral before it begins the divisor into zeros of a fractional place that represent sub units of a whole number. At that point of the long division the number in the remainder is basically bouncing between 0 and 9 of a 10 base or 00 99 of 100 and so on for 000 999 and 0000 of 9999

The numeral of the divisor estimation at a glance can be approximated of its length in digit length probability by  φn10=1.6^1762941 or 1.61762941 to be 161,762,941 potential digits long of the new quotient. The fact that the first remainder of the divisor divided into the dividend may be one short less than the divisor, the number more or less rolls back and forth between the digits limit of 161,762,941 many digits before it loops again at some variable factoring point. 

This being the case for these long decimal places and the application of the stem cell cycle variant noted, φn10=1.6^1762941 to φn10c2=1.6^17629411762941 then changes the probability length of the new quotient from 161,762,941 to 1,617,629,411,762,941 and φn10c3=1.6^176294117629411762941 to 16,176,294,117,629,411,762,941 possible digits of the quotient being factored in just that one tier phase of the φ Θ or Q scale ratios.


The explanation of quotient digit length, φn1 to φn21 then 1Qn to 2Qn along with Θ nc1 to ncn of decimal cell stem cycle numeration in base ten digit numerals prime 1000000007 and fibonacci y 1138903170 prior to application of these terms in the factoring ∉|101 (φ/Q) | |10010 (φ/Q) |ten sets and ⑆⨊=0∘⧊°10∘⧊° ten more sets with links to practical application fields.

Do not get lost looking for prime numbers in phi ratios decimal place numerals.

Within the first tier sequences of φ many of the ratio variables have decimal place values. These variables are much like a wheel of integers when the decimal values continue to cycle for a number like 1φn5 or 1φn8 or 1φn9 and so on... 

1φn3=2 and 2 is a prime.

1φn4=1.5  and the digit 5 is prime.

1φn7=1.625 has digit 2 and 5 in the quotient and 2 and 5 are both primes.

1φn8=1.^615384  has number 61 and 53 and 5 and 3 and 3 and 5 and 53 and 61 are primes.

What changes with the φ numerals scale variables is their repeatable squence that means larger more complex primes can be found in each variable of φ that repeats its decimal stem cycle cell. If a sequence of such simple numbers can create this variable, then in computers without that fact at its logic gate, a byte shift of gate logic is lost and a byte shift is that easy to mislead back to a short rotating number base sometimes referred to as a byte shift between basic 0 and 1 and 2 and 3. This means that the computer is easily compromisable and able to be hijacked with a computer.

For example, 1538461 is prime and it can be found in 1φn8c2=1.^615384615384

Gaining control of a system logic gate is a system device that has lost control of that logic gate and another system has gained control of something that is a logic gate of its security with a numeral base in just eight digits of prime computer number library functions. This is only an example of numerals and computer logic.

1φn9=1.^619047 has 61 and 19 and 7 and 47 and 619 in the quotient and 7 and 19 and 47 and 61 and 619 are primes. With a repeated cycle of the stem variable 1904761 is found that is also a prime in 1φn9c2=1.^619047619047

Within the same example numerals, the many digits are also containing numerals that actually break down to prime factors.

1φn3=2 and 2 is a prime.

1φn4=1.5  and the digit 5 is prime. removing the decimal of the digits is 15 that is 3x5 and 3 and 5 are prime numbers.

1φn7=1.625 has digit 2 and 5 in the quotient and 2 and 5 are both primes. 6 has prime factors 2x3 and 2 and 3 are prime numbers. 25 is 5 squared or 5x5 and 5 is a prime number.

1φn8=1.^615384  has number 61 and 53 and 5 and 3 and 3 and 5 and 53 and 61 are primes. 6 has prime factors 2x3 and 2 and 3 are prime numbers. 15 that is 3x5 and 3 and 5 are prime numbers. 8 is 2 cubed or 2x2x2 and 2 is a prime.

There are very many primes within the digits of phi radicals. Dividing Phi with primes from a second variable base of simple primes or prime/prime ratios of Q produce quotients that also have a stem cell cycle in the quotients of φ/Q and φ/P and P/φ and Q/φ.

The radicals that φ/Q and φ/P and P/φ and Q/φ produce quotients of very much also have prime numbers in their decimal stem cycle variables for many equations of nφncn/nQncn

An example use of these math terms would be the periodic table of elements comparison to particles of elements and compounds emitted from earths sun polar north and south and its equator as well as a galaxy polar north and south and equator. Elements that pass through as many changes as elements emitted by either would certainly be similar in factoring its difference to a periodic table base line mass weight stored on weight and time unit measurements of carbon or hydrogen. The elements at the polar and equator emmissions of stars or star clusters are in fact entropy and enthalpy unit measures of astronomical systems of change and shell particles in a phase of solid from liquid to frozen particle states in a vacuum of space gas. Time oscillations of a crystal at differing ranges from a planetary or star surface mean that the crystal used to measure time itself are not sufficient and can be distorted, so when time is more relative to the recorded data it is synced to, the time recorder can not faulter or the record is useless just as a periodic table of elements inaccurate base moler weights of carbon or hydrogen.

0 1 01 10.1 101 1.01 0.1

a genesis code of logic numerals to binary translation of one version of a shell language form of binary. 

whole line

00110000

00110001

00110000 00110001

00110001 00110000 00101110 00110001

00110001 00110000 00110001

00110001 00101110 00110000 00110001

00110000 00101110 00110001

segment one of line 0 1 01 10 what is between the decimal of whole line

00110000

00110001

00110000 00110001

00110001 00110000


segment two 1 101 1 where prime 101 is  what is between the decimal of whole line

00110001

00110001 00110000 00110001

00110001


segment three 01 and 0  what is between the decimal of whole line

00110000 00110001

00110000


segment four 1  what is between the decimal of whole line

00110001


 segment five what is between the numerals containing first decimal integer of whole line 0 1 01 10.1

00110000

00110001

00110000 00110001

00110001 00110000 00101110 00110001


 segment six what is between the numerals containing two decimal integers of whole line 10.1 101 1.01

00110001 00110000 00101110 00110001

00110001 00110000 00110001

00110001 00101110 00110000 00110001


segment seven what is between the numerals containing last two decimal integers of whole line 101 0.1

00110001 00101110 00110000 00110001

00110000 00101110 00110001


segment eight what is between the numerals containing all three decimal integers of whole line 10.1 101 1.01 0.1

00110001 00110000 00101110 00110001

00110001 00110000 00110001

00110001 00101110 00110000 00110001

00110000 00101110 00110001


what is between 0 and 0.1 of this logic line of seven numerals with what is between 0 and 10, what is between 1 and 10, what is between 0 and 10.1, what is between 0 and 0.1, what is between 0 and 101, what is between 0.1 and 101, what is between 1 and 101 what is between 1.01 and 101, what is between 0 and 1,  has been explained on this page of 10 base numerals and eight bits in many ways.

Reason for 0.1 being last in the line is the decimal that can separate it from the line of a new line starting from one rather than zero and why this is described as a genesis line code logic. 0 itself can not be repeated if something were nothing to form one thing containing all of nothing. From the one in the end of the line at 0.1 being the end of the line rather than 0 0.1 1 as an order the string compliments a base ten eight and seven factors to display more than one decimal length past 0.1 at 1.01 and 1.01 lands between 0 and 10.1 and 0.01 lands between 0 and 0.1 so many cycles of a ten base logic are in fact in this genesis logic line.

if a new line is then made it can be more complex and would follow after this line depending on the length of decimal to the matrix of a zero one array based in tens or tenths. This is just a logical expression of something and nothing and many parts between and after nothing condensed of all nothing to something. 0.1 is not 0 1 so the beginning of the line is not the same as the end of the line. Within segment two is 1 101 1 that in logic terms is a split path logic gate of 1 to 101 and 101 to 1 where a 1 to 1 as well as a 1 to 101 and 1 to 101 have diabatic potential. Within the simple logic of each segment of the entire line. 0 and 0.1 and have a range of an unlimited length of zeros between the 0. and the 1 in numeral values of tenths hundreths thousandths etcetra. 0.1 0.01 0.001

1 101 1 is not 11011

|0|

01111100 00110000 01111100

|1|

01111100 00110001 01111100

|01|

01111100 00110000 00110001 01111100

|10|

01111100 00110001 00110000 01111100

|10.1|

01111100 00110001 00110000 00101110 00110001 01111100

|101|

01111100 00110001 00110000 00110001 01111100

|1.01|

01111100 00110001  00101110 00110000 00110001 01111100

|0.1|

01111100 00110000 00101110 00110001 01111100

In this binary example that uses 0000 0000 to 1111 1111 a smaller set of 000 111 base array is foreign to the limit of the line being that 111 is out the line limit of 101. |0| |00| |000| |1| |11| |111| The binary example shell machine code is using 00110000 to represent ( 0 ) and 00110001 to represent ( 1 ) and 00101110 for ( . ) A machine might read 000111 as 00000111 or 00001110 or 00011100. 111 is a number that is 37 x 3 that are two primes yet 111 is beyond the limit of 101 and the two primes of 111 means the numeral 111 would be divided at a logic gate to which 3 and 37 are between the numerals of 0 and 101. 

3 is between 0 and 10 

3 is between 1 and 10 

3 is between 01 and 10 

3 is between 0.1 and 10 

3 is between 1.01 and 10 

3 is between 0 and 10.1 

3 is between 1 and 10.1 

3 is between 01 and 10 

3 is between 0.1 and 10.1 

3 is between 1.01 and 10.1

37 is between 10 and 101

37 is between 10.1 and 101

where a computer should not be making an error. 

|111|≠3 

machine language of logic gates of a line that can easily be programmed with a byte shift of fractions of time to try being unnoticed.

0 1 01 10.1 101 1.01 0.1 are seven numerals

zero

one

zero one

ten and 1 tenth

one hundred and one

one and one one hundreth

zero and one tenth


In the machine language of binary it simply takes another shell program language version of the binary translated to a different syntax that would mathematically put the power of a decimal place more valuable than the numeral one. The decimal point for example in a different binary translation would then be 00110000 to represent ( 0 ) and 00110001 to represent ( . ) and 00101110 for ( 1 ) that if such paths were changed in a syntax, the machine code would be called a float point byte shift based on 1.0

A machine and the machine decimal limit is a critical point before any binary base translation of those numbers that the binary itself can have many paths of translation of its own. The same application can be seen or noted in microbiological forms and their chemical signals in the microbiological systems where many many chains of numeral instructions apply to the very elements that make up their matter and their function abilities. Another example aside from 0 1 0° degree ° 0.1 medical library data systems is ADS Astrophysics data systems and communication between these systems. 

While prime ratios of 21Qn1=(pn1/pn2) have ratio values that are around and or between the numbers of the line 

0 1 01 10.1 101 1.01 0.1 the ratios land between 0 and 1 as well as 0 and 1.01 as well as 0 and 101

nφn1 has a zero core at each scale tier with a common factor of 0 just as does nφn1  with divisions incorporated with primes and Q ratios of primes

1φ/21Q=∈n1/(pn2/pn1)|=(0/1.5)=0

n2/21Q|=(yn2/yn1)/(pn2/pn1)=(1/0)/(3/2)=0 

1φ/11Q=∈n1/(pn1/pn2)|=0

None of these 0 variables are 0.1 nor are they 1.

the variables are 0 with different definitions derived from 10 digit numerals of fibonacci and prime numbers explained from within just 0 1 to 10

0 1 01 10.1 101 1.01 0.1 are unique numbers in a line and basically are 7 keys to the internet of \\0 

null point of any intranet

0 : 1 : 1

2 : 3 : 5 : 13 : 89 : 1597 : 28657 : 514229 : 433494437 are unique numbers of  | 1000000007 | and |1138903170| 

0 : 1 : 10 are unique numbers of these all just as are the ratios and decimal precision of phi/prime fractal polarization in quantum field mechanics

if something disrupts the 0's and 1's and dot (.)'s of your computer it is not nothing, it is something.

A system that rounds so much in math using pi of 3 digits such as 111 in byte shift is a system that can be mislead just as a c shell that has a base value of pi to a limited 7.4 radius with the factor base 

11Qn30=(pn31/pn30)c1=(131/127)=1.^031496062992125984251968503937007874015748 example 

where a decimal shift two places over and dropping the remainder of the decimal as many machine print out makes a computational display of 10.31496062992125984251968503937007874015748 where 1.0 is then seen as 10.3 and the next shift is 3.14 that the 10 is moved from for a viewer who does not process the loop of numerals in shell layer machine code numeral binary. if one log can move the decimal and extract the 1.0 then the 10. while using 3.1496062992125984251968503937007874015748 and dropping 96062992125984251968503937007874015748 of the numeral chain claiming it is beyond the machines print out limit of digit length, then a system as simple as 1 2 3 to produce a none error appearing as a |111| or |404| error is that easy.

 While the user is mislead by a simple byte shift into a gate, the numerals for 

11Qn30=(pn31/pn30)c1=(131/127)=1.^031496062992125984251968503937007874015748 can close the logic gate and cycle the simple prime cycles for cn of this prime base that extended past the 101 limit into a closed secondary system of 

11Qn30=(pn31/pn30)c2=(131/127)=1.^031496062992125984251968503937007874015748031496062992125984251968503937007874015748

or more with cycles of cn numerals beyond the limit at the first logic gate of initial line from using pn31/pn30 of 11Q

at 0 1 01 10.1 101 1.01 0.1

A shell limit is a shell limit 101 and prime ratios mentioned cycle at the first remainder digit of the pn2/pn1 function for every later divided by previous to the 101 prime from 2 pairing division of prime later divided by prime previous.

314 is also the remainder before the remainder of the looping remainder 6 that can easily shift another shell of primes of 1.^038216560509554140127388535031847133757961783439490445859872611464968152866242=11Qn36=(pn37/pn36)c1=(163/157)

11Qn36 can also be looped at cn that make two functions of cycles at the discretion of the primes outside of the 101 limit.

Negating a decimal point in shell compilers is a simple error and not one a machine should be able to make.

0 1 01 10.1 101 1.01 0.1 is a line with a limit of 101 not 00101110 and not 314 to a 6 looping remainder

1⅄, 2⅄, 1X, 1+⅄, 1-⅄, 2-⅄, 3nc

and 

0 1 01 10.1 101 1.01 0.1

are each 7 factors of different logics each within a 10 base numeral beyond zero and multiple definitions of zero are explained on this page

A variable such as 0.6 or 0.66 or 0.618 such as 314 in rounded numerals byte shifts means that a variable such as 

(13φn3)c2 of (13φn3)c2 of (22φn4=(1φn5c2/1φn4)/12φn3c1)=(0.90361445783132530120481927710843373493875/1.^3)=0.61816496765625576163113994439295644114913^461538

having a 0. before a 618 has in fact 39 numerals after it before a cycle of a decimal stem 461538 ever even begins and displaying numerals limited to 10 or 12 factor digits long means a great deal of byte shifts can occur in fractions of computer computing seconds while it sometimes takes minutes hours days weeks or years to find a simple byte shift root. While a user interface displays 1.618 minus 0.618 equals 1 a shell of 111 or 000 are easily parted from 0 1 01 10.1 101 1.01 0.1

Variable 1φn11=1.6^18  or 1.618 or 1.61818 is an 11th variable and 168 is beyond 101 limit of the line 0 1 01 10.1 101 1.01 0.1

numeral 11 of 1φ is beyond the limit of 10 and 10.1 for simple logic where 0 00 1 11 10 01 are a logic gate of 6 that 7 numbers of 

0 1 01 10.1 101 1.01 0.1 genesis line that can structure 1φn1 and 2φn1 and 3φn1 and 4φn1 and 5φn1 and 6φn1 and 7φn1 and 8φn1 and 9φn1 and 10φn1 to φn1 as the n1 of each phi set tier has proven is level of 0 with a different definition of the zero in the genesis line. Whether a zero is an absolute power of zero being |0|=1 then the 0 and 1 of the genesis line represent that logical fact. Any variable defined as 1 of what the variable is can then be structured to the 1 of the genesis line just as and 0 can be structured to the 0 of the genesis line. No zero can replace the genesis line 0 and no one can replace the genesis line 1.

if (13φn3)c2 of (22φn4=(1φn5c2/1φn4)/12φn3c1)=(0.90361445783132530120481927710843373493875/1.^3)=0.61816496765625576163113994439295644114913^461538

and

(22φn4=(1φn5c2/1φn4)/12φn3c1)c2=(0.90361445783132530120481927710843373493875/1.^3)=0.61816496765625576163113994439295644114913^461538461538

a micron µ of difference applied to an exponential µ10 or a cube root incorrectly in a very critical and complex equation will produce an incorrect estimate that the precision of the micron difference proves is critical.

An algorithm of factoring an equation of a multiple of a decimal ratio explained on this page is the basics of an encryption key algorithm or an algorithm of plus or minus or a chain of sequence using these numerals are the simple basics of functions to these radical constants that complex microbiological and chemical structures utilize in their structures. 

Multiples of these numerals times whole numbers and exponents addition or subtraction will produce an extensive library of numerals when properly defined just as the division definitions provide to the degrees of cycles at stem Cn just as these numerals multiplied with other ratios or added and subtracted or exponentially factored with division defined numerals.

Numbers do not lie. 

9999999999999999999

9888888888888888889

9877777777777777789

9876666666666666789

9876555555555556789

9876544444444456789

9876543333333456789

9876543222223456789

9876543211123456789

9876543210123456789

9876543211123456789

9876543222223456789

9876543333333456789

9876544444444456789

9876555555555556789

9876666666666666789

9877777777777777789

9888888888888888889

9999999999999999999

1111111111111111111

1222222222222222221

1233333333333333321

1234444444444444321

1234555555555554321

1234566666666654321

1234567777777654321

1234567888887654321

1234567899987654321

1234567890987654321

1234567899987654321

1234567888887654321

1234567777777654321

1234566666666654321

1234555555555554321

1234444444444444321

1233333333333333321

1222222222222222221

1111111111111111111

inner perpendicular tetrahedron angle divided scale to exterior cube perpendicular angle scale

a'b'c' :  a''b''c'

scale to scale nucleic

a'b'c' to a''b''c' to a'''b''' c''

and so on of perfect cube in perfect sphere

divided to pyramids from center point

anion  tide  -  some

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