Not Applicable.
Not Applicable.
Not Applicable, in that, each PEMD Table for fractional displacements are less than 300 lines long.
Precise infinitesimal displacements are not exact but require finite estimates of changes from a predetermined reference. PEMD is a novel utility, ornamental binary device, and original math method which obeys established pi relationships of inverted trigonometric functions of a circle's interior angles (versus center angles). By operation of pi's transcendental property (no algebraic variations-on-integers can equal to its value) and pi's irrational property (pi's value as a decimal representation never ends, infinite!, or never repeats during infinite truncations—pi decimal values to the right of zero). Pi's unique math properties permit almost limitless software (mathematical) simulations for estimating fractional, arc displacement values. Based on target displacements and values resulting from PEMD's simulation using PEM's binary math utility, unique ‘hardware’ configurations can be fabricated for target ‘software’ precisions.
Real world (not infinite) fractional-displacement-estimates are limited by computer data processing limits—that is, estimates requiring precisions several places to the right of a decimal. However, real world-accuracy-limits, can entail realizable and large amounts of finite pi divisions for arc length estimates—but require sufficient pi divisions within fractional arc increments, such that values become extraordinarily numerous and result very close to actual values. What are reasonable infinitesimal limits? Decimal representations of pi truncated to 12 decimal places are sufficient precision for accuracy comparable to the range of Bohr's radius of the hydrogen atom. Precision range within this Utility Patent Application, using PEMD's pi truncation, use 6 decimal precision owing to Printed Table Space Limits and the absence of a supercomputer. However, PE Methods within this application allow ‘n’ digit computer simulation for fractional displacement precisions. These estimates are very close to actual arc lengths and demonstrate pi estimating methods (PEM) for infinitesimal displacements. PE Method and Device (PEMD) are introduced by three PEM Devices: Full, half, and quarter size PEMDs. A Prototype Binary Device is used for illustration purposes, to set-up: unquestioned range values and unquestioned domain values. PEMD's unique binary configuration, permits displacement calibrations and establishes distinct arc motions with pre-set and corresponding partitions for precise value-goals.
Among numerous PEM Device ‘hardware configurations’ suggested by PEMD's Simulation Methods for Displacement Estimates, only select PEMD Examples are presented that illustrate a basis for a novel binary math utility and unique pi estimating method. Select examples illustrate how manipulations of ‘hardware’ parameters approximate fractional displacements accurately, while benefiting from unlimited pi combinations within PEMD's vast ranges of operation. Displacement Ranges depend on PEM Device's physical and governed limits. Many displacement devices can result for articles of manufacture, controlled by user requirements. User physical variations will bound ‘hardware’ targeted precisions—but, PEMD's use of pi's unbounded estimates for arc length and PEMD's ‘software/mathematical methods’ permit many and varied user-defined precisions to be achieved.
Applications which require close estimates to user-specific, target values, or infinitesimal values, and close design tolerances, are implied in many fields of endeavor. Considering Classifications, PEM Algorithm should be listed in many fields of the numerous USPTO Patent Classifications Definitions. Owing to PEM Algorithm's general utility and special methods for ‘infinite’ values, many fields of endeavor utilizing infinitesimal values would involve listing PEM many times. Citing one specific classification, probably will cause PEM's salient appeal to be lost for wide/diverse applications. Only, Classification 341, “Coded Data Generation or Conversion” was observed on USPTO Web-site as sufficiently descriptive for PEM Algorithm's wider appeal. That is, for emphasis again, precision values surface in many fields of endeavor and coded data & conversion-technology state-of-art, vary within many specialized applications. Also emphasis is directed to PEM Algorithm as an original math utility and its ‘Infinite Pi Data’ are not necessarily for machine ends.
Specific references used during development for pi utility, design, math methods, and fabrication of a binary prototype device, using Pi Estimating Method and Device (PEMD) for fractional displacements are:
Pi Estimating Method and Device (PEMD) is an original utility, yielding an ornamental device (hardware), and an original mathematical method (software) which takes advantage of pi's unique property of transcendental values for not repeating itself, and in decimal form, for never ending, thereby permitting many PEMD sizes for different displacement precisions and within various design physical-size, packaging constraints. Four basic physical parameters are used to affect displacement precisions. Then, using four physical changes affecting precision, different PEMD Tables (Avg. ppc—see Tables 4 through 7, Pages 50 to 81) of pi estimates are produced for ‘software’ comparison and illustration. An initial ‘hardware’/Test PEMD, hereafter referred to as Prototype Device, was fabricated to establish size references, operating parameters, precisions, and ‘base values’ for software references and comparisons. Tables of fractional displacement are generated for different: Face Heights (Ht.), Track Lengths, crank-drive major Diameters—crank threads-per-inch (TPI)—e.g. 0.75-10 UNC, and Roller Diameter. Unique combinations of four (soft/calculated) variables, relative to an established/(physically verified/tested) math model, combined with physical (hard) Prototype Device, are used to establish proof for claims. Also, accepted mathematical relationships will establish proof of claims when required. Value references, fractional estimated values, are produced in Tables for PEMD Quarter Size, Half Size, and Full Size (same as Prototype Size except with high tpi) and are integral for use with an original PEM Algorithm. Initial Prototype Device values establish hard (ware) and soft (ware) ‘base’ references for illustration purposes only. In dimensional comparisons, initial, verified/proven values are established for ‘real world’ comparisons for different PEMD sizes, in order to demonstrate PEMD's novel utility, flexible device—size options, and to present unique math methods/hardware binary devices for pi estimates of fractional displacements using an original PEM Algorithm.
The main object of the invention is to establish PEMD mathematical methods, using pi estimates to ‘find’ targeted, user-defined, microscopic displacements, by use of either manual, by electro-mechanical, or by electronic or by computer control. For example, DC drives & control, as well as computer driven PEM Devices (thinking outside the prototype-device-box) can involve Cathode-Ray electron beam targeting, and miscellaneous high energy targeting within present and established industry art. Electronic PEM Device fabrication and detail are not discussed. PE Methods & Algorithm can use CNC targeting, and when appreciated, ‘Benefits from PE Methods’ will allow Decision/Precision Maps for computations of PEMD Binary Domains and Ranges or Targeted/Goal Precision Values. PEM Algorithm benefits become obvious, once Tables of Average Precisions per Crank (Avg. ppc) are established for an intended device. Values within a unique PEMD's Table, then become a ‘calibrated method’ for ‘finding’ or ‘pi-estimated’ accurate displacement values very close to, if not equal to, target or goal values. Goals can be above (nX) Reference PEMD Full-Size or a Fractional (1/n) PEMD Size. PEMD Configurations are vastly numerous based on diverse measuring and displacement applications.
What is important and discloses the general idea behind this ornamental and unique method-of-estimation/utility invention is: PEM, within a user-application, permits a user to initially specify target precisions, use PEM's mathematical (soft) methods of estimation, and then, produce hard-results by use of pi estimating methods—which allow a PEM Hardware Device, a novel device that obeys pi's fractional displacement estimates. PEM Device's reliance on pi's math property of unique infinite values to the right of zero, without repeating values, allow many physical variations of PEM Devices. Each device that satisfies PEM will function within calibrated displacement-increments, and will operate on pi's ability to yield infinite number of fractional decimal values. Based on a physical configuration sought, dictated by a chosen target displacement, pi's fractional values, although having no ending or limits within displacement intervals, will aligned to values within displacement increments, such that, discrete infinitesimal values are realized for precision determinations.
The first listing are Graph Figures derived from a Prototype Device which establishes ‘base data’ for generalized pi estimating methods, which obey PEM. Statements for purpose and cross-reference to detailed descriptions will be given as appropriate. The second listing are for Mathematical Equation Figures. The third listing are Photographic-view Figures of a Prototype PEM Device which more clearly illustrates a hardware example that complies with pi estimating methods of PEM Device. Statements corresponding to each Photo-view Figure will explain the purpose of each figure. The fourth listing are various Sample Calculations and a Table for Prototype Device and Tables for three Examples of PEMD physical variations on precisions. The final Table, Table 8, addresses Fractional PEM. Each table will be supported by explanations referenced to other tables or figures when needed and will be provided with sample calculations as appropriate. Total Listing follows:
General Form, Equation 1-1 is used for verifying ‘measured’ values of ‘Y’. Sample calculations by operation of Equation 1-1, 1-2 and 1-3 for ‘X’ at 6″, ‘Y’ (at ‘X’=6″) are used for example. Appropriate definitions are given. See Page 42.
PEMD's general mathematical expressions are developed at two places:
Sample 1/64 th inch calculations are given for pi truncated to 4 digit, 5 digit, and 6 digit accuracy. Pi Estimates for Example Targets are shown within 6th Digit precision to the right of decimal point. Tables 4, 5, 6, & 7 use only 4 digit domain and range values for Average Precision Per Crank (Avg. ppc). Special calculations for 5 digit and 6 digit truncations (Pages 37 and 39) are given as sample calculations for illustrating additional precision by pi truncated. Math Domain and Range Values, using 4 digit, are sufficient for most displacement estimates Quarter-Size PEMD and greater. Additional truncations for pi, 12 digits or greater should be utilized when sub-fractional arc estimates are needed to simulated values that fall within atomic and sub-atomic domain and range measurements using pi estimating (PE) Methods (M). For illustration purposes, 4 digit pi is used in measuring, math checks, and calibrating devices for binary domain and range relationships using a Prototype Device and three PEMD examples. A fourth example, PEM Algorithm Example, is given at Table 8 to demonstrate “estimating a known and unquestioned atomic value” to confirm PEM Algorithm's infinitesimal power.
The purpose of providing portable views are to demonstrate that PEMD does not have to be permanently attached to a bench or permanently to any support structure. Again, the threaded rod used on the “test” model for determining a governed ‘Binary’ (Roller) Domain, the rod is longer than required for the Prototype's binary displacement-range selected. For the rod length shown, Track B will stand straight up or 90 degrees, with ‘X’ at 10″ (or orthogonal to level). User PEMD must be governed (restricted) for targeted displacements that cover binary values and will be less than “test” rod length shown on
Table 1. Y Determinations of Graph
Base values are measured, calculated, and established using GF 1 for a Prototype Binary Device: Face Ht.=3″, ¾-10 UNC, Roller Dia.=2″, Track L=11″: Page 41.
Table 1-1. Measured ‘Y’ Displacement for Each ‘X’.
The purpose of Table 1-1 is to create ‘base values’ to be used for user target/goal displacements. Prototype Device's base values are binary and are dependent on physical parameters of the prototype. Prototype physical parameters selected for Full-Size are: Face Area 3″ height, Drive Crank ¾″major diameter, 10 threads per inch, Unified National Course Standard (0.75-10 UNC), Lift Roller 2″ OS diameter, and (roller) Track Length (L) 11″. Other PEMD Bases could have been chosen initially. For PE Methods, Prototype's Device-physical-parameters are binary and are distinctly selected to demonstrate an original binary scheme, a scheme for pi estimating, and for presenting, that is, for illustration purposes, an example of ornamental device, that obeys PEM. All PEMD above and below Full-Size must obey binary proportionality. Prototype Device Graphical Values on Table 1-1 list ‘Target’ or ‘Goal’ Domain & Range Binary Values and allow a Scheme of known/measured Displacements Ranges (Y) to be compared to a simple line equation for ‘calibrating’ PEMD to restricted partitions of two arc segment lengths (P1 & P2). Using Prototype values as PEMD base values, physical, and graphical measured displacement (Y) values, are compared to line equation solutions for ‘Y’ on Table 1-1. This is done as a check, a double check, for measured versus calculated ‘Y’ congruence and for unquestioned base values. Subsequent PE Methods using base values become unquestioned/proven, for simulating pi estimated values using PEM and its device (D). Thus, subsequent PEMD will not require double checks (graph or line equation), but will only require conformance to binary proportionally of pi methods and device parameters calibrated for Full-Size PEMD. See
Table 1-2. Calculated Angles (Degrees) from Graphical Results of
Table 1-2 utilizes ‘X’ & ‘Y’ Values from Table 1-1 and by use of inverted trigonometric relationships of interior angles and Equation 2, an alternate method, a pi estimating method (PEM), for calculations, yield PEMD's unique math scheme of dividing displacement-arc-lengths into predetermined Intervals. Inverse tangents using Prototype's ‘X’ binary domain and ‘Y’ binary range, produce ‘angle boundary values’ for each Interval (pi values within an arc length), and then each restricted partition (P1 & P2) are divided by predetermined Intervals (increments that obey tpi), such that, calibrated ‘Y’ displacements, are presented according to domain Intervals, with each Intervals divided by tpi increments. Prototype's calibrated (measured and calculated) domain and range values are PEM base-reference-values. Exact angle boundary (in degrees) for all PEM Intervals are now established for the pre-determined Arc-Segment-Partitions (P1 & P2), as illustrated by Exploded View within
Table 2.
The purpose of Table 2 is to show Prototype's Conformance to FIG. 2's ‘below level’ Arc Partition 1′ (P1) and ‘above level’ Arc Partition 2 (P2). A Key Scheme is introduced that align whole values of X to unique and specific angle values using Eq. 2, Page 31. Also, another purpose of Table 2, is to demonstrate how Intervals between ‘calibrated degrees’ are translated to threads per inch (TPI) for establishing ‘X’ Domain Increments and how corresponding degree increments allow computation of fractional displacements. Prototype's P2 Domain is binary and utilizes Intervals 2 to 3, 3 to 4, 4 to 5, 5 to 6, 6 to 7 and 7 to 8 for estimating Prototype's Displacements with integral links to corresponding binary range values. By use of pi (degrees) that correspond to binary range values: +90 to 85.24, 85.24 to 82.87, 82.87 to 78.69, 78.69 to 75.96, 75.96 to 68.55, and 68.55 to 63.44 degrees, respectively, displacement ‘Y’ are calculated using Eq. 2-1. Page 44 calculated values for displacement (Y) are given in inches and millimeters. Although millimeter equivalents were used with inches during Prototype Device testing, inches are selected for presentation and are used throughout further discussions without necessarily stating dimensions. For this application, Inches are understood when not stated.
Table 3
The purpose of Table 3 is a refresher for standards that relate a circle's circumference divided by fractional pi (radians) and degree equivalents of fractional pi. Also fractional pi are related to conventional Quadrant Standards using counter-clockwise rotation for positive angles. For example, a radius from a circle's origin to its circumference, begins a positive sweep at zero degrees when radius is congruent with a positive horizontal axis and begins a positive arc segment on a circle's circumference by counter-clockwise rotation; and, the summation of all arc segments will equal to its circumference when one revolution is complete or a 360 degree sweep returns to point-of-beginning. By definition, an ‘arc segment’ is that fractional length on a circle's circumference which was subtended when a circle's radius rotated a given angle [i.e.: arc=Radius times angle (radians)]. Although a PEMD's motion obeys circle's central angle, the circle's arc segment is equivalently estimated in two restricted Partitions (P1 & P2) by Equation 2. See
PEMDs that are fabricated using a hand crank will require an individual's knowledge of Table 3-1 through 3-6 and his or her comfort with fractional pi estimates for controlling, measuring, and displacing incremental values. Unless fixed fractional displacements are routinely sought and PEMD settings remain predetermined (plus owing to pi's rigor), a pi estimating method (PEM) Algorithm using computer control is suggested. PEM is integral to all PEM Devices (Ds), or PEMD (s). Computer control using PEM Algorithm is the preferred control method. However, with pi familiarity, and use of PEM Word Algorithm, precise estimates can be ‘cranked’ or calculated with relative ease. Then, by use of a PEMD, accurate displacements or measurements can be made. PEMD Quarter-Size and above, permit displacement values by hand or motorized ‘crank’. Based on PEMD sizes much smaller than Quarter-Size, and if need for multiplicity of estimated values, PEM Algorithm by computer control of a device—a device that obeys PEM—will prove to be most useful.
Table 4.
Table 4 is a listing of Average Precision per Crank (Avg. ppc) of the Binary Prototype Device, Face Height=3″, crank diameter=¾″, 10 threads per inch (10 tpi), Roller Diameter [outside (OS)]=2″, and Track A or B Length (L)=11″. First (Left) Column (C), lists the number of completed revolutions per increment within Domain Intervals keyed to whole numbers (e.g. 1-2, 2-3, . . . 7-8) and subdivided by TPI and ‘calibrated to Range Pi Partitions (e.g.: +90 Degrees to +85.24 Degrees which corresponds to Key 2-3). Second Column are increments of ‘X’ using TPI for divisions or alternately, a scheme for determining Domain Divisions can be found on Tables 6 and Table 7, Pages 68 to 74 and 75 to 81, respectively. The Third Column are calculated Y Values using Eq. 2-1, Page 31. Each Table 4 (e.g.: Tables 4-1, 4-2, . . . 4-7. Pages 50 to 53) are a listing of Y Precisions that fall within the whole number Key Scheme that signifies a PEM Domain under consideration. The Remaining Columns are precisions within fractional Cranks (C)—Reference Table 4, Page 50—and each of these columns are averaged to yield “Average Precision per Crank” (Avg. ppc). Avg. ppc is integral to pi estimating (PE) method (M) for approximating Target (T) Values by PEM Algorithm. See Table 3 (Page 47), Table 2-5 (Page 45), Table 2 Sample Calculations (Page 46)., and PEM Algorithm (Page 33).
Table 5.
Table 5 provides a listing for Avg. ppc for a Full-Size PEMD when TPI is changed. Forty threads per inch (¾-40 UNS) is selected for comparison to Table 4, 10 tpi, Prototype Device. Sample Calculations using Table 5 Values and PEM are at Page 34. Impact on accuracy is demonstrated by Target Value minus Pi Estimated (PE) Value: (T−E) using PEM Algorithm (See Page 36).
Table 6.
Table 6 provides a listing for Avg. ppc for a Half-Size PEMD when all four physical parameters are uniformly altered to configure PEMD to binary one half size. Half size PEMD involves half size for Face Ht (3″ reduced to half or 1.5″), Crank Diameter (¾″ reduced to 5/16″ & TPI (40 increased to 48) or 0.3125-48 UNS, Roller Diameter (2″ reduced to half or 1″) and Track Length (11″ reduced to half or 5.5″). Go to
Table 7.
Table 7 provides a listing for Avg. ppc for a Quarter-Size PEMD when all four physical parameters are uniformly altered to configure PEMD to binary one quarter size relative to a Full-Size binary PEMD. Quarter size PEMD involves quarter size for Face Height (3″ reduced to ¾″), Crank Diameter (¾″ reduced to 3/16″ & TPI (40 increased to 72) or 0.1875-72 UNS, Roller Diameter (2″ reduced to ½″) and Track Length (11″ reduced to 2¾″). Sample Calculations using Table 7 Values and PEM are at Page 39. Same Target (T) Value were used by Table 5, 6, and 7 (or near 1/64th inch) for comparison to precision changes affected by different physical configurations. Although 6th digit precision variations are slight and minor, T−E maintains 6th digit accuracy within ten one-millionth of an inch.
Table 8.
Table 4 (Prototype), Table 5 (Full-Size PEMD), Table 6, (Half-Size PEMD), and Table 7 (Quarter-Size PEMD) involve methods for estimating displacement that fall within machine tolerances. Sizes above Full-Size PEMD are not addressed, in that, proportionalities will involve the same binary methods and tolerances. Table 8's purpose is to demonstrate PEM Schemes (opposite to large for contrast) such that, extremely small displacements are equally valid for PEM Algorithm and a Device, a PEM computer controlled device. Table 8 contains a collection of tables that show added techniques for estimating micro-miniature displacements. By use of PEM Algorithm and math schemes used at machine-levels, pi estimating for atomic and subatomic approximations for any value can be produced and “repeated” when an Algorithm obeys pi-keyed-equivalent-proportionalities of PE Methods. Although a self-contained PEMD for atomic and subatomic level displacement values are not practical in a single unit, PEM software control, obeying the techniques of pi estimating, are realizable for interfacing with and controlling a PEM device. Table 8 addresses pi estimating method (PEM) to estimate known Niels Bohr's Hydrogen Radius Value (Target) for illustration only, and offers example math methods for using PEM Control: to find micro-miniature binary domain and range values for Target Values, to pi estimate, measure and/or displace Target Values using the process of PEM. Consistent PE Methods permit logical “repeat” values above and below Targets by Algorithm. One should realize the salient importance of finding, measuring, and repeating microscopic displacements smaller than Hydrogen, smaller than subatomic, and smaller than smaller by consistent methods offered by PEM.
Table 8-1 lists PEMD Binary Sizes and Binary PEMD Domain and Range Values. It should be noticed that Full-Size (Table 5, Page 54) is identified as 1×, Half-Size (Table 6, Page 68) is “n”=0, and Quarter-Size (Table 7, Page 75) is “n”=1. Hydrogen-Size (Table 8, Page 86) is “n”=27.
Fractional PEMD domain and range lower boundary values correspond to Prototype Device at level, reference zero, and above level. Binary domain, X and Y Values below level are not included in displacement approximations. All “keyed references” are calibrated or use Prototype binary relationships; hence: Equivalent Domain Lower=2, Equivalent Domain Upper=8, Equivalent Range Lower=0, and Equivalent Range Upper=4 (Refer to Table 8-1 and Tables 2 & 4). Since a PEMD obeys binary, notice all binary range values (Ref. Table 8-1, Page 82) are one half of ‘full upper’ domain value because of binary. This binary relationship for domain and range continues on into atomic, subatomic and beyond, for pi estimating.
Table 8-2's purpose is to compare Prototype Device, Full-Size PEMD, Half-Size PEMD and Quarter-Size PEMD, Average Precision Per Crank (Avg. ppc) against Most Significant Digit (MSD) of values in Standard Form resulting from fractional Cranks within one revolution (or one Crank). Exponent values of Avg. ppc are shown for Key Scheme Intervals and for all fractional pi. Then, exponents are averaged for relative precision comparisons of the three PEMD examples to the Prototype Device. Basically, precisions are the same for the four examples regardless of size, except that displacement ranges and domain change. Highlighted (bold) exponent values are for special interest in MSD values used for PEM Form at Table 8-3. Page 85. Table 8-2 lists Domain Lower & Upper Boundary and Range Lower and Upper Boundary in Standard Form where every number can be expressed as a number between 1 and 10 and can be represented as a positive or negative power of ten.
Table 8-3's main purpose is to establish a PEM Form that differs from Standard Form in Table 8-2. In PEM Form, the MSD is just right of the decimal point and every number can be expressed as a number between 0.0 and 1.0 and can be represented as a positive or negative power of ten—with negative power being of interest for Fractional PEMD. PEM Form is used for math ease in allowing the majority of computations in the same power of ten without shifting exponents (See PEM Form “A×C=” Column on Table 8-3, Page 85). Values between zero and one are associated with PEM Form for all PEMD Calculations and its form are integral to PEM Algorithms.
Table 8-4 is ‘Table 8-5 in progress’ with explanations by example calculations (See Page 86). Table 8-4 combines the functions of Tables 8-1, 8-2 and 8-3 to find Niels Bohr's Hydrogen Radius Value. Using Bohr's known and well established Radius Value, as a Target (T) Value, is intended to take advantage of a known micro-miniature value to illustrate pi estimating method (PEM) and PEM Algorithm. In a sense, Table 8-4 is a ‘setup’ Table for determining PEM Key Scheme, PEM Domain and Range Intervals, and methods of Interval Increments for producing only the specific Average Precision per Crank (Avg. ppc) Table (e.g.: Table 8-5, Page 95) that has Hydrogen's Radius Value.
Table 8-5 is preceded by Table 8-5 Confidence Check. The purpose of the confidence check is to assure that micro-miniature PEMD binary magnitudes are proportional equivalents to Full-Size PEMD. Table 8-5 contains Hydrogen's Value. In binary proportional atomic space, Hydrogen is located at Full-Size PEM Key: 4 to 5 Equivalent, Crank 20 to 30 Interval, and by PEM Avg. ppc Table, Table 8-5 in PEM Format, Hydrogen's Radius can be approximated by using PEM Algorithm as given on Table 8-5 Sample Calculations (Page 96).
A pi estimating method (PEM) and its device (D) or PEMD is a self contained binary unit that can measure, control, and provide precise displacement for an attached mechanism within a single unit and is a hardware pi device. PEMD is distinguished from a PEM Software Binary Unit, in that, pi estimating method (PEM) is an Algorithm, primarily intended for synthesized displacement, obeying pi approximations for Target (T) Measurement by the Algorithm. Values resulting from computed pi estimates are to be used for computer control of an ‘external device’ interfaced to a PEM Unit. PEM Algorithm, which is integral to this Utility Application, is primarily intended for computer control applications. A PEM hardware device (D) or PEMD, performs the PEM Algorithm by operation of its mechanism.
The best mode for demonstrating how binary operations of the Prototype Device (
The ‘X’ domain has been restricted to two distinct partitions for lift operation, Reference (Ref.)
Refer to Geometry for Yb,
Prototype ‘Xb’ Binary Domain follows the following Interval Convention as Key Scheme:
X
b=(parked),(1,2],[zeroed],(2,3],(3,4],(4,5],(5,6],(6,7], and (7,8],
whole number Intervals for all “Avg. ppc Tables” (Ref. Tables 4 through 8)—exception for Table 8 (Ref. Page 87) which does not use Xb Interval (1, 2] or (parked), but uses only domain ranges that yield displacements (Yb) above zero reference, without loss of precision or interruption of equivalence. Sample Xb: 2 to 3 Interval for Prototype Device and PEMDs are given below:
It should be noticed that each Key Scheme/Interval has an open interval for lower interval domain boundary, hence, end points are not included. Upper interval domain boundary is a closed interval and therefore include end points. Data are presented on each Table that respect the foregoing convention.
Self-contained PEMD using tpi for Xb Domain Interval divisions quickly deminish with physical thread options for Fractional PEMD. Hence, computer simulation of PEM operations benefit from 10n Interval divisions and permit arc length approximations for displacement (yb) estimates to be very close, if not equal to, exact values. Recognizing 10n increments in Xb domain values, and Pi not repeating itself for infinite truncations, the development of Table 2 (Ref. Page 44), supported by its Sample Calculations, reveal the need and subtle power of a method or Algorithm which integrally has Xb's 10n divisions & range values with Pi's infinite vastness.
A Prototype Device is constructed so that its lift function obeys Binary Range Motion and its action is accomplished by Track B being tangent to the lift roller while it travels up Track A, which in turn, is proportionally configured to allow Track B displacement to obey Binary Range Boundary Values. Track B's arc movement, relative to its Hub, yield Yb Binary Range Boundary Values: 0 to 4 which are congruent with its Xb Binary Domain Boundary Values: 2 to 8 (
Table 1 (Page 41) lists Prototype Device measured values. These values are verified by simple linear relationships. However, the lift operation moves according to a circle's arc segment during each discrete whole value of Xb and its displacement values agree with discrete pi values (Table 1-2, Page 41). For convenience, pi is expressed in degrees, where 360 degrees=2 pi radians. Owing to Track B's arc movement, (
Domain Interval (In)={(x0,x1],(x1,x2], . . . (xn-1,xn]},
there exists a function, yb=f(xb), such that, for every value of xn in a restricted binary domain (xn-1, xn], there exists precisely one number, such that, yb=f(xb) exists in restricted binary range (0, yb],
By Eq. 2-1:
y
b
=f(xb)=xb/tan(θ2), if and only if (− 5/18 pi<θ2<⅙pi]
And, f(xb) is smooth because f′(xb) exists and f(xb) is restricted to be continuous at every number (no gaps or jumps) within 2 judiciously selected, and restricted, arc segment Partitions (P1 and P2), which assure the tangent function remains smooth and continuous:
And, −θ2 in Partition One (P1) is: − 5/18 pi<−θ2<−½ pi (for zeroing PEMD)
And, +θ2 in Partition (P2) is: +½ pi>+θ2>+⅓ pi (for incremental displacements).
Partition One (P1) is not necessary for Fractional PEMD (See Table 8) owing to methods developed by Table 8, Pages 82 thru 97, and therefore, only binary range using pi within P2 boundarys above are considered.
With Equation 2-1 restricted by P2's pi range, and to be congruent with restricted Domain Set of all real numbers within pi Intervals, then all values within domain and range Intervals to be congruent within P2, must obey the following pi Intervals, divisions, and sub-divisions, and obey open & closed interval convention as given (See Paragraph [0051] above, Table 1 and
In general expression:
Range Interval (In)={y0,y1],(y1,y2], . . . (yn-1,yn]},
a unique yb (or yn) exists for every value of xb congrument with pi range intervals immediately above.
Proof of the above are not given, in that, the tangent function, within Equation 2, is well established by trigonometric precedence. Decimal values of unlimited pi truncations, permit unlimited displacement values within restricted Partition P2, calculated via Equation 2-1, and yield unlimited computer simulated displacement values that extended beyond atomic, beyond sub-atomic, and beyond—beyond. Pi estimated method (PEM) precisions achieved via use of PEM Algorithm are only restricted by computer computational capacity and cost.
The PEM Algorithm is presented in word format (Refer to
m
1=(y2−y1)/(x2−x1) Eq. 1-1
m
1=(yb−1)/(xb−0) Eq. 1-2
y
b
=m
1
x
b+1 Eq. 1-3
In the x-y plane, Prototype Example, Reference
m
1=(y2−y1)/(x2−x1) General Form. Eq. 1-1
Let Track B Mounting Arm be represented by the Line of Eq. 1-1, starting at its Hub, (0,1), and ending where the Track Arm and the Track B intersect, the absolute value of |y2−y1|=yb—to provide ‘y’ ‘displacement reference’ and to distinguish from a graph point location, given by (x2, y2). Subscript ‘b’ also alludes to absolute ‘x’ roller displacement from an ‘xb’ zero reference, Track length (L) distance from (0, 0) and (11, 0). Start of Device's Roller movement toward it's Hub, always begins at an initial position, and initial condition for Prototype Device is xb=1. However, all xb movement is relative to its zero reference. Eq. 1-1 translated is:
m
1=(yb−1)/(xb−0) Translated Slope in terms of Hub location. Eq. 1-2
Values for Slope (m1) and yb are obtained by Graphical Solution (
y
b
=m
1
x
b+1 Eq. 1-3 purpose is to confirm measured xb and yb. Use of 1-3 Equation involves 2 unknowns. Eq. 1-3
Hence, in order to obtain calculated solutions without the use of a graph (
Y
b
=f(xb)=Xb/(tan θ2) θ2 is an interior angle in FIG. 5, and Not a center angle. See Below. Eq. 2-1
The following One-sided Limits, which state Pi boundaries (in degrees), use two separate and distinct PEM Partitions (Ref.
Refer to
tan(θ2)=Xb/Yb Eq. 2-6
PEMD units smaller than ¼ Size, require a PEM Computer Software Control Algorithm for simulating equivalent (equiv.) ‘domain’ divisions used in determining ‘range’ divisions for targeted pi estimated displacements. PEM Software Values can then be loaded into an Interface Unit (or integrated as a single unit—computer/interface) for driving a Device Unit that can position micro-miniature units with infinitesimal displacements or, for example, drive a laser or electron gun during infinitesimal positioning. All PEMD Schemes obey equivalent (equiv.) ‘domain’ and ‘range’ schemes of the ‘Full-Size’ Prototype Binary Unit.
Pi Estimating Method (PEM), Sample Calculation Examples, and Table 5 Values Used with Fractional Pi Values Utilized in PEM.
Reference: Full Size PEMD Table 5, page 54 for example—values are used for Algorithm below. It should be noticed that the methods, PEM Methods, presented below, are valid for Tables 4, 5, 6, and 7. Although PEM method is simple, its algorithm, given by manual/word ‘steps’ below, can be readily programmed for software computer-decision-making and simulation of target results. Speed, expanded computation, and greater truncations of pi, allow extremely accurate precisions. PEM Software ‘targeting control’ are primarily intended for fractional PEM Devices that utilize PEM Math Process for finding micro-miniature target results. Manual calculations are initially given to illustrate pi estimating method and expected tolerances of estimated results within current machine industry art. Targets within atomic and subatomic scales have domain and range displacement estimates addressed by Table 8-1 and Table 8-1 Sample Calculations. Devices larger than Full-size PEMD are not discussed and are simply Full-size PEMD, or expanded PEMDs.
Starting with a Full-Size PEMD, Target (T) 1/64 Example, 1/64=0. 015625 using Pi Estimating Method (PEM), the following ‘word’ algorithm establishes PE Method (PEM) for PEMD:
Steps for Pi Estimating and Word/Manual Algorithm for Decisions:
0.
00
27
25
0.
00
26
0.
00
00
13
0.
00
01
17 < 0. 00. 01 25.
0.
00
00
13
0.
00
01
17
0.
01
56
17
A note on Accuracy, Target Value Sought minus Estimated Value, using PEM, subtract ‘E’ from ‘T’: T−E=0.015625 minus 0.015617=0.00 00 08. This difference is much much less (<<) than ANSI machinery allowance <<0.000250. PEM's value allows accuracy 30 times more critical than a typical ANSI stringent of 25% of one one-thousands limit used in Standard Allowances and Tolerances.
Miscellaneous sample calculations, given for various Tables; will be given as required. When the foregoing algorithm is used, it will be provided without all descriptions but will be provided in the same format as above. Any confusion or need for further definitions will be provided for the specific Table; or, one must refer back to this initial PEM Scheme (Algorithm) and descriptions when necessary.
0.
00
42
15
0.
00
42
0.
00
00
14
0.
00
00
14
0.
0
7
81
24
0.
00
19
51
0.
00
19
0.
00
00
50.
0.
0
4
68
74
This initial confidence check is to establish and verify, domain and range ‘Partition Values’ of restricted arc segments, traveled by Track B, controlled within Distinct Intervals (domain) of a lift roller movement, and result in distinct displacement values (range), for comparison to measured, initial graph results, such that, unquestioned boundaries are set. All PEMD are calibrated using ‘Intervals’, within restricted Partitions of initial arc segments, established initially by graph for ‘full’ restricted ‘binary’ domain and range displacements (See Legend on FIG. 1,). Graph Values provide initial confirmation, checked by equations, and then presented, hence forth, as ‘base values’ utilized for indisputable PEMD Base Values. Check Values will be used in upper and lower Interval Divisions for all pi estimating methods (PEM) and Algorithm Scheme. Infinitesimal Values derived within PEMD Scheme and PEM Process of Arc Segmenting (for pi estimation of fractional displacements) are consistently ‘keyed’ to initial and distinct PEMD Partitions & Intervals. By using initial range and domain base values of
1
−53.13
−0.75
−¾″
2
−90.00
−0
0 at −90 deg
2
+90
+0
level
3
85.24
0.25
3
85.24
0.25
4
82.87
0.50
4
82.87
0.50
5
78.69
1.00
1″
(above ref.)
5
78.69
1.00
1″
6
75.96
1.50
1.5″
6
75.96
1.50
1.5″
7
68.55
2.75
2.75″
7
68.55
2.75
2.75″
8
63.44
4.00
4.0″
¼ C
90
1st
Q
½ C
180
2nd
Q
¾ C
270
3rd
Q
full
C
360
4th
Q
¼ C
90
1st
Q
½ C
180
2nd
Q
¾ C
270
3rd
Q
full
C
360
4th
Q
¼ C
90
1st
Q
½ C
180
2nd
Q
¾ C
270
3rd
Q
full
C
360
4th
Q
¼ C
90
1st
Q
½ C
180
2nd
Q
¾ C
270
3rd
Q
full
C
360
4th
1st
10
of
1st
Q
⅓ 1st Q
1/2 of 1st Q
1
−0.75
2
0
Average Precision per Crank:
0.075
0.019
0.009
0.006
0.002
0.000208
2
0
3
0.25
Average Precision per Crank:
0.025
0.006
0.003
0.002
0.0007
0.000069
3
0.25
4
0.5
Average Precision per Crank:
0.025
0.006
0.003
0.002
0.0007
0.000069
4
0.5
5
1
Average Precision per Crank:
0.050
0.013
0.006
0.004
0.0014
0.000139
5
1
6
1.5
Average Precision per Crank:
0.050
0.013
0.006
0.004
0.0014
0.000139
6
1.5
7
2.75
Average Precision per Crank:
0.125
0.031
0.016
0.010
0.0035
0.000347
7
2.75
8
4
Average Precision per Crank:
0.125
0.031
0.016
0.010
0.0035
0.000347
1
−0.75
Average Precision per Crank:
0.010
0.0024
0.0012
0.0008
0.00026
0.000026
Average Precision per Crank:
0.015
0.0039
0.0019
0.0013
0.00043
0.000043
Average Precision per Crank:
0.022
0.0054
0.0027
0.0018
0.00060
0.000060
2
0.0000
Average Precision per Crank:
0.028
0.0071
0.0036
0.0024
0.00079
0.000079
2
0.0000
Average Precision per Crank:
0.005
0.0012
0.0006
0.0004
0.00013
0.000013
Average Precision per Crank:
0.006
0.0014
0.0007
0.0005
0.00016
0.000016
Average Precision per Crank:
0.007
0.0017
0.0008
0.0006
0.00019
0.000019
3
0.250
Average Precision per Crank:
0.008
0.0020
0.0010
0.0007
0.00022
0.000022
3
0.2500
Average Precision per Crank:
0.005
0.0014
0.0007
0.0005
0.00015
0.000015
Average Precision per Crank:
0.006
0.0015
0.0007
0.0005
0.00017
0.000017
Average Precision per Crank:
0.007
0.0016
0.0008
0.0005
0.00018
0.000018
4
0.5000
Average Precision per Crank:
0.007
0.0018
0.0009
0.0006
0.00020
0.000020
4
0.5000
Average Precision per Crank:
0.011
0.0027
0.0014
0.0009
0.00031
0.000031
Average Precision per Crank:
0.012
0.0030
0.0015
0.0010
0.00033
0.000033
Average Precision per Crank:
0.013
0.0032
0.0016
0.0011
0.00036
0.000036
5
1.0000
Average Precision per Crank:
0.014
0.0035
0.0018
0.0012
0.00039
0.000039
5
1.0000
Average Precision per Crank:
0.011
0.0029
0.0014
0.0010
0.00032
0.000032
Average Precision per Crank:
0.012
0.0030
0.0015
0.0010
0.00034
0.000034
Average Precision per Crank:
0.013
0.0032
0.0016
0.0011
0.00036
0.000036
6
1.5000
Average Precision per Crank:
0.014
0.0034
0.0017
0.0011
0.00038
0.000038
6
1.5000
Average Precision per Crank:
0.028
0.0070
0.0035
0.0023
0.00077
0.000077
Average Precision per Crank:
0.030
0.0075
0.0038
0.0025
0.00084
0.000084
Average Precision per Crank:
0.032
0.0081
0.0040
0.0027
0.00090
0.000090
7
2.7500
Average Precision per Crank:
0.035
0.0087
0.0043
0.0029
0.00096
0.000096
7
2.7500
Average Precision per Crank:
0.029
0.0072
0.0036
0.0024
0.00080
0.000080
Average Precision per Crank:
0.030
0.0076
0.0038
0.0025
0.00084
0.000084
Average Precision per Crank:
0.032
0.0080
0.0040
0.0027
0.00089
0.000089
8
4.0000
Average Precision per Crank:
0.034
0.0085
0.0042
0.0028
0.00094
0.000094
0.5
−0.3750
1
0.0000
Average Precision per Crank:
0.016
0.0039
0.0020
0.0013
0.00043
0.000043
1
0.000
1.5
0.125
Average Precision per Crank:
0.005
0.0013
0.0007
0.0004
0.00014
1.5
0.1250
2
0.2500
Average Precision per Crank:
0.005
0.0013
0.0007
0.0004
0.00014
0.000014
2
0.2500
2.5
0.5000
Average Precision per Crank:
0.010
0.0026
0.0013
0.0009
0.00029
0.000029
2.5
0.5000
3
0.7500
Average Precision per Crank:
0.010
0.0026
0.0013
0.0009
0.00029
0.000029
3
0.7500
3.5
1.3750
Average Precision per Crank:
0.026
0.0065
0.0033
0.0022
0.00072
0.000072
3.5
1.3750
4
2.0000
Average Precision per Crank:
0.026
0.0065
0.0033
0.0022
0.00072
0.000072
¼
−0.1875
½
0.0000
Average Precision per Crank:
0.009
0.0024
0.0012
0.0008
0.00026
0.000026
½
0.0000
¾
0.0625
Average Precision per Crank:
0.003
0.0009
0.0004
0.0003
0.00010
0.000010
¾
0.0625
1
0.1250
Average Precision per Crank:
0.003
0.0009
0.0004
0.0003
0.00010
0.000010
1
0.1250
1.25
0.2500
Average Precision per Crank:
0.007
0.0017
0.0009
0.0006
0.00019
0.000019
1.25
0.2500
1.5
0.3750
Average Precision per Crank:
0.007
0.0017
0.0009
0.0006
0.00019
0.000019
1.5
0.3750
1.75
0.6875
Average Precision per Crank:
0.017
0.0043
0.0022
0.0014
0.00048
0.000048
1.75
0.6875
2
1.0000
Average Precision per Crank:
0.017
0.0043
0.0022
0.0014
0.00048
0.000048
2-3
2-3
0.00
−2
−3
−3
−3
−4
−5
3-4
3-4
−2
−3
−3
−3
−4
−5
4-5
4-5
1.00
−2
−2
−3
−3
−3
−4
4.00
Exp.:
−2
−2.67
−3
−3
−3.67
−4.67
2-3
0
−3
−3
−4
−4
−4
−5
2-3
−3
−3
−4
−4
−4
−5
2-3
−3
−3
−4
−4
−4
−5
2-3
−3
−3
−3
−4
−4
−5
3-4
−3
−3
−4
−4
−4
−5
3-4
−3
−3
−4
−4
−4
−5
3-4
−3
−3
−4
−4
−4
−5
3-4
−3
−3
−4
−4
−4
−5
4-5
−2
−3
−3
−4
−4
−5
4-5
−2
−3
−3
−3
−4
−5
4-5
−2
−3
−3
−3
−4
−5
4-5
−2
−3
−3
−3
−4
−5
1
4
Exp.:
−2.67
−3
−3.58
−3.75
−4
−5
2-3 eq.
0.0000
−3
−3
−4
−4
−4
−5
3-4 eq.
−3
−3
−4
−4
−4
−5
4-5 eq.
−2
−3
−3
−3
−4
−5
5-6 eq.
−2
−3
−3
−3
−4
−5
6-7 eq.
−2
−3
−3
2.0000
Exp.:
−2.4
−3
−3.4
−3.5
−4
−5
−0.1875
0.0000
2-3 eq.
0.0000
−3
−3
−4
−4
−4
−5
3-4 eq.
−3
−3
−4
−4
−4
−5
4-5 eq.
1.0-1¼
−3
−3
−3
−4
−4
−5
5-6 eq.
−3
−3
−4
−4
−4
−5
6-7 eq.
−2
−3
−3
−3
−4
−5
7-8 eq.
1.0000
−2
−3
−3
−3
−4
−5
Exp.:
−2.67
−3
−3.5
−3.67
−4
−5
−4
−4
−4
−6
Hydrogen PEMD “n” value=27. Using Table 8-1, General Expression for Equivalent Binary Domain and Binary Range, and using H2 Radius Value as an Example Target (T) Value, Bohr's H2 infinitesimal Radius Value is estimated using PEM Algorithm to to demonstrate and set-up pi estimating math scheme for atomic, Subatomic and beyond. Fractional PEMD uses the following PEM Math Process for effecting a PEM Computer Control Unit (See
Lower Boundary (DL) of H2's Binary Domain (D), n=27, is:
Upper Boundary (DU) of H2's Binary Domain (D), n=27, is:
Lower Boundary (RL) of H2's Binary Range (R) is =“0”. Value is zero owing to PEMD being ‘leveled or plumb’ for starting displacements. Hence equivalents to Prototype PEMD Domain ‘Key’ for “1 to 2” or (1-2 equiv.) are values omitted for finding Target Displacements.
R
L=0.0.
Upper Boundary (RU) of H2's Binary Range (R) from Table 8-1, n=27, is:
“Full” Range versus “Full” Domain Upper Values: RU are one half DU in all “Binary” PEM Key Schemes:
Knowing Target Domain and Range ‘Boundary’ Values of Hydrogen (H2), and in a sense, working in reverse, in that, a PEMD's binary displacements used for atomic displacements are not governed by physical dimensions dictated by user packaging constraints, Average Displacement per Crank (C) becomes Average Displacement per Circumference (C) or 2 pi, without loss of meaning for fractional Crank (Key Scheme used with Full-Size PEMD).
A Table 8-4 is ‘set-up’ for working in reverse, using Binary H2, n=27 (PEM Math Equivalence), to estimate fractional displacement, and using Table 8-1 for finding DL, DU, RL, and RU Values above. By Prototype Key Scheme, PEM Calculations for “Average Precision per Circumference (C)” are made for H2's Avg. ppc Table. The result is Table 8-5, Page 96. H2 Domain and Range Values are congruent with Key pi Intervals and Divisions for simulated ‘Full-Size’ pi estimated equivalency (outlined on Table 8-4 set-up).
From above upper range value (RU) repeated below, find Mid- and Qtr.-Range Values that fall in Prototype ‘KEY’ Domain Intervals: 2-3, 3-4, 4-5, 5-6, 6-7 or 7-8.
R
U=0.148810(10)−7, n=27.
Mid-range for RU=(RU−0)/2 locates pi angle 78.69 degrees, shown below. And RU/2=Mid-Range=0.074405(10)−7 or 0.74405(10)−8 (PEM Form, ref. Table 8-3). A PEM n=27 Mid-Range Value is near and >T. A PEM Mid-Range is at Key 4-5 and 5-6 boundary or at I3 and I4 Boundary, respectively. Hence, H2 Range Target (T) Value is <n=27 Mid-Range Value at Interval 3's (I3's) Upper Boundary, using upper boundary Range Reference and observing that T is Not in Domain Key 5-6.
Mid-Range of n=27 RU must be further divided to determine if T is less than or greater than another pi boundary. Mid-Range/2=¼ RU and recognizing proportionality of pi's Full-Size PEMD Equivalency (Yb), Mid-Range PEM Intervals are I1+I2+I3=I4+I5+I6. Obeying and following PEM Full-Size Scheme: I1+I2 and I3 (by itself) are ¼ RU—see Table 8-4 below. So that PEM Intervals divide according to arc length measurements using pi, ¼ RU is located at Pi Interval=82.87 degrees and is I3 lower boundary.
Therefore, relative to 6 pi intervals and RU, PEM Quarter-Range n=27 (relative to upper boundary value) is I3 (4-5 equiv.) in order to be equivalent to Pi Intervals and Boundary Pi Angles, that obey PEM. At 82.87 Degrees, find I3 lower ‘Domain’ boundary and at 78.69 Degrees, find I3 upper ‘Domain’ Boundary, discussed further in next paragraph.
Domain Interval that corresponds to the above Range Interval (I3) occurs between Pi Boundaries: 82.87 degrees and 78.69 degrees and shown below:
Domain Increments will correspond to the pi range increments. Divisions will be equal for all intervals and by example, are equal to 101 or 10. Therefore, each Xb change is [0.371654(10)−8]/10 or 0.037166(10)−8.
The nice part of Computer Simulation allows selection of divisions within Pi Intervals that do not have to obey threads per inch or TPI. Hence, for Math convenience, select power of 10 and initially select 101 or 10 divisions within Pi Intervals for Math ease. Therefore, Xb=0.371654(10)−8 will be divided 10 times or each increment=0.037165(10)−8. It should be noticed that unlimited 10n subdivisions are available for infinite increments of Xb used in Equation 2-1 calculations for pi estimated (PEM) displacements and are only limited by how close ‘estimate’ values are intended to approximate ‘target’ values.
Find the H2 Domain Values which identify fractional Pi (expressed in degrees) Increments (Inc.) used for calculating displacement (Yb), using Equation 2-1:
Range Interval that corresponds to the above Domain Increments occur between Equivalent Pi Boundaries: 82.87 degrees and 78.69 degrees. Domain Degree Intervals must be mathematically congruent with the same Increments used in Domain Intervals. For math ease, power of 10 was chosen, exponent=to 1, or 10 divisions. Therefore:
I3 Range Increments (Crank/Rev. equivalents) and corresponding pi increments are:
20/82.870
30/78.690
With Interval Xb Values and corresponding Interval Pi Values above, using Equation 2-1, Avg. ppc are calculated and listed on Table 8-5, Page 95, for PEM H2 Values. It should be realized that Avg. ppc Tables for all Key Interval Schemes could have been computed instead of the above method which locates the specific Avg. ppc Table for H2. By computing all Avg. ppc Tables for PEM (10)−8 and then searching for nearest value (less than) of H2 identifies which Key Interval contains Bohr's Value−Target (T) Value. The above method allows one to go directly to the Crank Number (Number of Circumferences) or Number of Revolutions to find a math equivalent displacement for further evaluation by PEM Algorithm's value approximation. On Table 8-5 Sample Calculations Page 96, using PEM Algorithm, Bohr's Radius is estimated.
Notice that T−E is 10 one-millionths accurate. By doubling pi truncation to 12 digits and expanding domain interval divisions for 102 increments, and expanding the methods of PEM Algorithm—for example: 7th & 8th digit Accuracy, 9th & 10th Digit Accuracy, and 11th & 12th Digit Accuracy using Partials ‘D’ for Fourth, ‘E’ for Fifth and ‘F’ for Sixth Partial pi Estimate Scheme (See PEM Algorithm, Page 33), respectively, to achieve 12 digit truncations, improves T−E error estimate. For even greater accuracy, more increments within Intervals are necessary. It should be noticed that a continuous set of real numbers can be used for 10n increments within Domain Intervals. As ‘n’ approaches a very large number (say toward ∞), and recognizing pi's irrational property of never ending (say pi truncations approaching ∞, and never repeating values), Equation 2, using PEM Key Scheme and pi estimating Methods, in general, can produce accurate, repeatable, approximations for displacement values that go beyond atomic, beyond subatomic, beyond quantum and beyond—beyond (e.g.: to the depths of the darkest black hole in space, and possibly, without ending). Exactness of Target Results become only limited by the computational capacity of super-computer use, and of course, cost.
Rough estimates above are used to verify that PEM approximations will simulate Full-Size PEM device magnitudes in relative proportions to micro-miniature Fractional PEM and equally obey Full Size displacement proportionality. Rough Estimates are compared to Binary Yb calculated using PEM of Equation 2-1 and Key Scheme, Ref. Table 8-4.
For example: 6/16 times 4″ is 24/16 or 1.5″ Displacement for Full-Size PEMD. The fractional PEM ( 6/16) times the upper boundary—Full Range—of H2's RU, n=27, is compared to Yb calculation at Increment 40, Interval 4, Key Scheme Equivalent (5-6) for PEMD proportionality using pi estimating with PEM Key Scheme and simulated for equivalent results of math values compared to base values established by Prototype Device obeying PEM. Both rough and PEM Eq. 2-1 methods provide agreement. Scheme behavior in atomic space holds.
1.489569
0.186329
1.861219
0.372246
Average Precision per Crank:
0.018592
0.004648
0.002324
0.001549
0.000516
0.000052
0.
00
63
62
0.
00
61
96
0.
00
00
52
0.
00
01
56
0.
20
86
51
To avoid Specification Fragmentation, it is recommended that the ‘entire’ Specification (Pages 1 to 98) be read for complete Detailed Descriptions, in that, essential detail are intermingled throughout and further supplements methods used in PEM Algorithm of this utility application. Only when repetition occurs, emphasis or clarity are intended.