Appendix 2: REPRESENTING PHYSICAL MODELS AS ABSTRACT EQUATIONS: PROCEDURES INFERRED FROM EXPERIMENTAL MATHEMATICS

Procedures for representing physical models in equation form cannot be determined from our axioms because our axioms are limited to abstract domains. But representation procedures can be examined by means of experimental mathematics. Valid representation procedures must be consistent with computational consistency tests. Current techniques for calculating the interaction of several natural laws over a spatial increment fail tests that valid representation requires, and are ruled out. A consistent technique is proposed. According to the proposed technique, terms in some equations that have been thought to be infinitesimal are finite. Implications in neural medicine and other fields that deal with the brain appear to be large.

Some seem to feel that mathematics is axiomatic construction and nothing else, but that sometimes, nevertheless, that axiomatic construction can be mapped to some useful work. The jump from the abstract to the concrete is held to occur by some discontinuous and unexplained process. A smoother, better explained transition between the abstract and concrete seems desirable. Mathematics already interfaces with experimental usages, and has long been pushed toward experimental approaches by the computer(1).

G.C. Chaitin has shown that many things in pure math are "true for no (axiomatically provable) reason at all(2)." Chaitin suggests that where existing axioms don't apply, new organizing assumptions may be considered, and may be useful. K. Godel advocated experimental approaches in mathematics on similar grounds(3). Even the interior of mathematics has experimental aspects. Some degree of experimental math seems justified and useful even in number theory.

The interface between abstract mathematics and the representation of physical circumstances can be investigated experimentally, as well.

There may be many reasons to investigate this interface between abstraction and concrete representation. My main one is concern about the correct form of the neural transmission equation. Medically important differences in neural line inductance, that can be 1018:1 or larger, hinge on a question that is beyond the jurisdiction of the axioms of pure mathematics. That question can be clarified, and perhaps entirely resolved, with experimental mathematics.

Conclusions based on mathematical experiments always lack the certainty of an axiomatic basis. Even so, some much-tested conclusions may be useful, and using them as new assumptions can permit useful logical work that would not be possible otherwise. Experiment-based inferences (assumptions) are now widely used in cryptography and other computer-based fields.

Results of mathematical experiments cannot prove with axiomatic certainty, but can disprove. When mathematical experiments show counterexamples to an assumption, that assumption has been ruled out.

Even within pure math, where axioms reign, there are good reasons to use experimental approaches to test and organize ideas that we may wish to use, where our axioms cannot be brought to bear. This supplements axiomatic usages without violating them.

In mathematical representation of PHYSICAL circumstances, set out in terms of experimentally derived physical laws, we are using mathematical techniques beyond where the axioms of pure math apply.  If we are to proceed at all, we must use experimental mathematics.

Here is the logic that experimental work has:

E1. In experimental work, candidate assumptions are somehow recognized or guessed. (No testing can happen before we        focus on something to test.)

E2. Candidate assumptions are tested against evidence. So long as an assumption survives all tests, it is used (with some        wariness) as a provisional assumption.

E3. Assumptions that evidence contradicts are rejected, or the assumptions are modified so that they do fit evidence.

If we use these experimental approaches we may sometimes usefully organize, extend, and focus our knowledge beyond the realm of our axioms. If we do not use these approaches, we cannot go beyond our axioms at all.

When we mathematically represent a physical circumstance, we are beyond our axioms. Let's call that representation process "p-m representation" for "representation from physical model to mathematical model."

(We'll assume that a workable p-m representation can be reversed in a m-p representation so that we can start with a physical model, convert it into a statement in abstract mathematics,  operate on the abstract mathematical statement, and then relate that statement in abstract  mathematics back to the physical model without misinterpreting or losing information of  interest to us.)

We have NO axioms for p-m representation or m-p representation.    We must determine the representation procedures of valid p-m representation and m-p representation on EXPERIMENTAL grounds.

Here is the p-m representation problem in more detail. When we derive an equation representing a physical model, reasoning from a sketch and other physical information, we write down symbols and terms representing physical effects. We may write down several stages of symbolic representation before we settle on our "finished" abstract equation. As we write our symbols, we implicitly face the following question:

Question:   WHEN can we logically forget that the symbols we write                   represent  a physical model?    WHEN can we treat the equation we've                   derived from a physical model as a context-free abstract entity, subject only                   to the exact rules of pure mathematics?

We can never do so on the basis of rigorous, certain, clearly applicable axioms. There are no such axioms. We cannot avoid making an implicit assumption that says

"THIS equation can be treated as a valid abstract equation, without further                  concern about its context or origin, because it seems right to do so, or                  because it is traditional to do so.    We have made the jump from concrete                  representation to valid abstraction HERE."

This assumption may happen to be right in the case at hand. But the assumption about p-m representation is not provably true from the axioms and procedures of pure mathematics. People go ahead and make these sorts of assumptions as they work. They cannot avoid doing so. Right or wrong, they are making "experimentally based" assumptions in their representation-derivations. People have made these implicit assumptions without recognizing the essentially experimental nature of their proceedings. It is better that this experimental nature be recognized, so that consistency checks can be applied to the unprovable steps. Any inconsistencies involved with these implicit steps may then be identified.

For any particular case of p-m representation, decisions are being made in a context of EXPERIMENTAL MATH at the interface between abstract math and physical circumstances. If a counterexample or inconsistency pertaining to a p-m representation usage is found, that is an extra-axiomatic circumstance. The extra-axiomatic usages that are failing as p-m representative tools should be modified so that they pass the consistency tests right p-m representation takes. Such modifications may disturb habits, but they need not, and commonly cannot, disturb the axioms of pure mathematics.

The Kelvin-Rall neural transmission equation derivation is based on an implicit, unprovable assumption about p-m representation:.

USUAL P-M REPRESENTATION ASSUMPTION: Abstract mathematical usages and          p-m representative usages are the SAME. When we are representing a physical          circumstance with mathematical symbols, those symbols are NUMBERS, and nothing more,          the instant they are written down.    All our rules of abstract mathematics apply immediately          to our symbolic constructions.

On the basis of this USUAL P-M REPRESENTATION ASSUMPTION, all of the crossterms in equations 7, 8, and 9 are ill defined. Here is equation 7, derived in detail in Appendix 1 . At a finite scale deltax each of these crossterms (terms below the first line) must correspond to finite physical effects. We have NO axiomatic guidance for computing these compound expressions.

We are referring to products of p-m representation procedures, not to axiom-based entities. We must judge the procedures we use to compute these compound expressions by experimental standards. Do these representations map the territories we expect when we check them? We may if necessary modify those procedures for consistency without violation of any axiom.

We must know what these representations mean numerically. If our computation is valid, the magnitude of a term at a set value of delatx and a set value of independent variable must be unique. After all, our limiting argument is an argument that deals with a decreasing sequence of finite terms. Before we can validly take the limit of equation 7, and derive a differential equation from it, we must know the magnitude of the crossterms for any finite deltax we choose. If we proceed according to the USUAL P-M REPRESENTATION ASSUMPTION, we find that our crossterms are not well defined.   The indeterminacy of these crossterms according to the USUAL P-M REPRESENTATION ASSUMPTION can be shown in the following ways. The difficulties set out below also apply to other crossterms that represent the combination of physical laws over an increment of length, area, volume, or time.

Numerical indeterminacy under "permitted" algebraic manipulations:

We assume that the crosseffect-containing terms such as the curly bracketed terms in (7) consist of  symbols that are "just numbers." We should be able to algebraically simplify each of these crossterms in  many different sequences that involve dimensional unit changes, so long as the end of each of the  sequences is in the same dimensional units. The numerical values of all such paths should be the same.   They are not. See Fig 1. An algebraically unsimplified dimensional group that includes products or ratios of dimensional numbers, such as one of those in curly brackets in (7), is set out in cm length units at A.

This quantity is algebraically simplified directly in cm units to produce "expression 1."     The same physical  quantity may be translated from A into a "per meter" basis at C. The translated quantity at C can then be algebraically simplified to D.   The expression at D, expressed in meter length units, is converted to a "per cm" basis to produce "expression 2."   Expression 1 and Expression 2 must be the same, but they are not.    The calculation is not consistent with itself. By repeating different "valid" computational loops in this way, any of the crossterms in curly brackets in (7) can be changed to any value at all, large or small. This is not the valid arithmetical behavior that we conventionally and thoughtlessly expect!   The loop test of Fig. 1 shows that these crossterms are meaningless as usually calculated, and the reason is as follows:

Before algebraic simplification, going from one unit system to another adjusts not just the numerical value of dimensional properties in the different unit systems, but numerical values corresponding to the spatial variable, as well.

After algebraic simplification, adjusting it to a new unit system corresponds to adjusting numerical values       that correspond to the unit change for the dimensional properties only, with no corresponding adjustment for the absorbed spatial variable.

The result is an irreversible, numerically absurd, but now standard mathematical operation.

THIS IS AN EXTRA-AXIOMATIC CONCERN:   WE HAVE A REPRESENTATION PROCEDURE THAT NEEDS MODIFICATION, BUT NO CHALLENGE TO VALID AXIOMS.

Contradiction between differential equations and the models they came from.

Suppose we assume that the symbols in the crossterms are all "just numbers." When we take the limit as deltax goes to zero on that assumption, these crossterms are all infinitesimal. So the differential equation we derive on this basis lacks these crossterms.

We take our differential equation, and integrate it back up to a specific scale deltax. We get an equation that lacks the crossterms that we know existed at scale deltax in the first place. The values at the same point, derived by two "correct calculations" are inconsistent, and can be very different.

THIS IS AN EXTRA-AXIOMATIC CONCERN:     WE HAVE A REPRESENTATION PROCEDURE THAT NEEDS MODIFICATION, BUT NO CHALLENGE TO VALID AXIOMS.

Crossterms fail a standard test map-representations should pass - the test that the whole should equal the sum of its parts:

In physical representations, wholes should equal the sums of which they consist. Consider any of the terms below the first line of 7. Suppose any term, evaluated at interval deltax, is instead set out as the sum of a number of intervals adding up to interval deltax. If deltax is divided into n pieces, and those n subintervals are computed and summed, that sum will be is only 1/nth (or 1/n2) the value for the same expression computed over interval deltax, taken in one step. We can make the value of the term on the interval deltax vary widely, depending on how many subintervals we choose to divide deltax into. This cannot represent PHYSICAL behavior. These terms are supposed to represent physical behavior.

AGAIN,   THIS IS AN EXTRA-AXIOMATIC CONCERN: WE HAVE A REPRESENTATION PROCEDURE THAT NEEDS MODIFICATION, BUT NO CHALLENGE TO VALID AXIOMS.

The USUAL P-M REPRESENTATION ASSUMPTION is that the symbols we write down are "just numbers" the instant we write them down. In the case of these crossterms that represent multiple physical effects over the same spatial increment, the usual assumption fails. So we need to look more closely at the details of what we are representing, the symbols we use to do that representing, and the procedures that apply to those symbols. We need representative procedures, that interface with our physical model on the one side, and interface with abstract mathematical usages on the other side, that avoid the representative contradictions shown above.

When we look at how physical models are represented by mathematics, we have NO axioms to rely on, and we have NO valid intuition to guide us. We must rely on the ordinary patterns of experimental investigation.

According to E-3, we are seeking a modification of current p-m representation procedure that maps these crossterms validly into axiomatic, abstract mathematics without changing other p-m representation procedures, now currently established, that we have no reason to doubt.

We are violating no valid axiomatic principles when we use experimental approaches to find a p-m representation that passes all operational tests needed to validly map to abstract equations. If a valid p-m representation procedure is found, that empowers axiomatic mathematics, and in no way diminishes it.

If we use the patterns of experimental logic and investigation with the same care that other people have applied to many other technical problems, the operationally valid experimental rules for representation can be found. Here again are the experimental patterns: E1. In experimental work, candidate assumptions are somehow recognized or guessed. (No testing can happen before we focus on something to test.) E2. Candidate assumptions are tested against evidence. So long as an assumption survives all tests, it is used (with some wariness) as a provisional assumption. E3. Assumptions that evidence contradicts are rejected, or the assumptions are modified so that they do fit evidence.

Operational definition of representative entities and inference of arithmetical rules that apply to them in p-m representation.

The jump between a physical system model, defined in terms of drawings, measurement procedures and other detail, and the abstract mathematical representation of it is taken for granted, but not usually set out clearly. S.J. Kline and I have tried to understand at a defined, procedural level how measurable circumstances are mapped to mathematical equations. Kline had written a respected book tightly connected with the subject(4). A first task was to identify the natural law operators, sometimes called dimensional parameters, in procedural detail.

The natural law operators are the entities that interface between our experimental measurements and the formalities of abstract, symbolic mathematics. Here are some directly measurable natural law operators (often referred to as properties):

mass, density, viscosity, bulk modulus, thermal conductivity, thermal diffusivity, resistance (lumped),  resistance (per unit        length), inductance (lumped), inductance (per unit length), membrane current leakage  (per length), capacitance (lumped),        capacitance (per unit length), magnetic susceptibility, emittance,  ionization potential, reluctance, resistivity, coefficient of        restitution, . . . .

There are many, many more.

All are defined according to the same pattern:

DEFINITION: A natural law operator is a "dimensional transform ratio number" that relates two measurable functions numerically and dimensionally. The natural law operator is defined by measurements (or "hypothetical measurements") of two related measurable functions A and B. The natural law operator is the algebraically simplified expression of {A/B} as defined in A = {{A/B}} B. The natural law operator is a transform relation from one dimensional system to another. The natural law operator is also a numerical constant of proportionality between A and B (a parameter of the system.) The natural law operator is valid within specific domains of definition of A and B that are operationally defined by measurement procedures.

Example: A resistance per unit length determined for a specific wire for ONE specific length increment and ONE specific current works for an INFINITE SET of other length increments and currents on that wire (holding temperature the same.)

The natural law operators are not axiomatic constructs. They are context-based linear constructs that encode experimental information.

We are concerned with the arithmetical properties of the natural law operators because of the inconsistencies related to crossproducts including spatial entities that have been discussed above.

Let's review the arithmetical properties relating to the natural law operators that we have no reason to doubt, and much reason to be sure of:

Natural law operators work just like dimensional numbers when they are used in exact correspondence with the equation that defines them.

For example, resistance per unit length is the numerical and dimensional transform that expresses Ohm's        law, and acts "just like a number" in expressions of Ohm's law.: Natural law operators may form compound natural law operators

DEFINITION: A compound natural law operator is a "dimensional transform ratio number" that relates two measurable functions numerically and dimensionally. The compound natural law operator is a transform relation from one dimensional system to another. The compound natural law operator is also a numerical constant of proportionality between one measurable value and another. The compound natural law operator is the product or ratio of two natural law operators, sometimes in association with a spatial increment. The compound natural law operator is valid within specific domains of definition of the natural law operators that define it.

Natural law operators act "just like numbers" when they multiply or divide to form a compound natural law operator that does not include an increment of space (length, area, volume, or time.) The conductance equations that apply to a line conductor, such as a wire, the Heaviside equations, offer examples. Here is the Heaviside equation for voltage, and the constructed natural law operators that apply to it, operationally defined. The products LC, RC, and LG are compound natural law operators that relate the derivatives and variables shown. They are calculated, numerically and dimensionally, just like other products of dimensional numbers: The terms on the right hand side contain products of natural law operators that act as compound natural law operators as follows: Mathematical and engineering practice has long depended on our ability to multiply and divide natural law operators in this (scale independent) way.   There is NO axiomatic reason why we can treat natural law operators as ordinary dimensional numbers when we calculate compound natural law operators that do not include spatial increments.  But we have solid experimental support for the fact that we can do so.    That evidence goes back to celestial mechanics calculations now nearly three hundred years old, and has been essential all through the history of mathematical physics.

We have practically no experience with compound natural law operators that contain spatial increments, however.   J.C. Maxwell and other worked with such constructs, and were often frustrated in calculational sequences.   Indeed, for reasons reviewed above, we have solid calculational experimental support for the fact that we CANNOT treat compound natural law operators including spatial increments, such as those in the curly brackets below, as "just numbers."   However one may wish to describe or think about our difficulties with these constructs, what is numerically essential is that we infer a rule that is a valid p-m representation.   In physical representations, wholes should equal the sums of which they consist. This is an essential test in cartography, the literal mapping of physical spaces that is the type case of our representations.   If the sum of a term over an interval is to be independent of the number of (evenly divided) subintervals into which that interval is divided, that term must be proportional to the following relation: Every term on the right side of 7b is already linearly related to length (m=1) externally to the compound natural law operator expressions. The compound natural law operator terms cannot have any length dependence at all. Otherwise, the terms cannot describe physical behavior. The argument for other compound natural law operator terms (with area or volume increments) will be the same.

For numerical consistency, compound natural law operator terms such as those shown in 7b must be numerically independent of increment scale, just as other natural law operators are independent of increment scale.

Even so, for DIMENSIONAL consistency, the dimensional exponents of the increments in the compound natural law terms must be ADDED.   We know that in a valid equation, every term must have the same net dimensions. (Suppose not: with an algebraic rearrangement, one side of the equation would have different dimensions from the other.)   In   appendix 1 , equation 7a-b is derived by valid dimensional number algebra - every term is dimensionally correct.    In every term where an increment occurs, its dimensionality is added in computation of the dimensionality of the term.    We have found reason to change the numerics of some of these terms, but that cannot change the calculation of dimensionality, which is correct.

We infer the following P-M REPRESENTATION RULE:

ASSUMPTION:   When the symbols that represent natural laws are combined to form a new natural law,      there are special rules for putting them together.   Only AFTER combination according to these rules can a      symbolic construction be formed that can be dealt with according to ordinary rules of algebra.

Specifically:   Constructed natural law operators in combined effect terms will include constructed natural law operators comprising several natural law operators and (perhaps) increments of space or time variables.      Constructed natural law operators are computed as follows: would be algebraically simplified as follows:

numerical part:   Numerical parts of the natural law operators making up         the constructed natural  law operator would be multiplied (divided).         (Numerical parts of any increments in the constructed natural law         operator are not part of the multiplication - the value is therefore         numerically independent of the increment scale at which it is evaluated.)

dimensional part:   dimensional exponents of all natural law operators and          any associated increments in the constructed natural law operator would          be added (subtracted).

This rule produces constructed natural law operators that are increment scale insensitive.   This rule is exactly the procedure used for centuries for compound natural law operators without increments.

According to this rule, crossterms are numerically determinant under permitted algebraic manipulation. There is no longer any contradiction between differential equations and the models they came from.    Wholes equal sums of parts.

The rule may be rephrased, and was expressed as follows in the main paper:

"the expressions within the curly brackets are physical interpretations of natural laws that          happen to have been "effectively measured" at scale x. To compute a natural law coefficient          that  fits the term, we convert x to

(1 length unit)

and algebraically simplify on that basis."

The S-K equation follows from application of this rule to constructed natural law operators that include spatial increments.

We can represent combined physical effects that act over spatial increments as finite terms in differential equations.

Summary: Experimental Math at the edge of axiomatics:

This appendix has treated calculations at the INTERFACE between abstract mathematics and the measurable world. In mathematical representation of PHYSICAL circumstances, set out in terms of experimentally derived physical laws, we are using mathematical techniques beyond where the axioms of pure math apply. If we are to proceed at all, we must use experimental mathematics. This paper has done so.

The results are not so sure as axiomatic results can be, and the negative results are more sure than the positive ones. We can rule out current interpretations of crossterms that call them infinitesimal in the limit. That is a strong result. We can suggest a P-M REPRESENTATION RULE that is a simple change to a currently accepted rule. The P-M REPRESENTATION RULE is consistent with all physical and mathematical issues that have been considered. The P-M REPRESENTATION RULE is a suggestion, that we can hold to be probable, and that we can compare to further calculations and to physical data. The rule assumes that the natural law operators that multiply numerically or divide numerically in compound natural law operators with increments interact arithmetically in the same way that natural law operators in compound natural law operators without increments interact arithmetically. That seems reasonable, and arguments for the arithmetic seem strong. Still, this arithmetic is an unprovable assumption. We have gone beyond the range where axioms determine results.

However, the results so far are useful. The Kelvin-Rall neural conduction equation, which lacks inductance, is strongly ruled out.   The Showalter-Kline neural conduction equation follows from a consistent, reasonable procedure that can be tested further.   It is reasonable that we should be left with a conclusion of experimental math that must be subject to further experimental verification or disproof.

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Dedication: Professor Stephen J. Kline, of Stanford University, author of SIMILITUDE AND APPROXIMATION THEORY4 and one of the great mathematical and experimental fluid mechanicians of this century, was my partner in the work leading up to this paper. We worked together on this for almost ten years, up to his death in November of 1997. Steve's contributions were many and indispensible. Steve thought hard about the problems of physical representation, and was completely clear about the need to find and fix an error at the interface between the representation of coupled physical models at the level of a sketch, and representation by a differential equation.

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NOTES:

1. G. C. Chaitin "Randomness in arithmetic and the decline and fall of reductionism in pure mathematics" p. 25 in G.C. Chaitin THE LIMITS OF MATHEMATICS Springer-Verlag, Singapore 1998.

2. G.C. Chaitin "An Invitation to Algorithmic Information Theory" in Chaitin, op. cit. p. 80

3. K. Godel, COLLECTED WORKS, V.3 manuscript "*1951" cited in Chaitin, op. cit. p.85

4. S.J. Kline SIMILITUDE AND APPROXIMATION THEORY McGraw-Hill, 1967, Springer-Verlag, 1984.