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Chapter 3:
Formal Science and Natural Science

3.1 - The Quine-Putnam Theses
3.2 - Quantum Logic
3.3 - Refutation of the First Quine-Putnam Thesis
    3.3.1 - About the Problem of Quantum Logic
    3.3.2 - General Theory of Relativity and Non-Euclidean Geometry
    3.3.3 - Chaos Theory and Mathematics
    3.3.4 - The Paradox of Revisability
3.4 - Reply to the Second Quine-Putnam Thesis

    Having established natural science as dealing with the physical world, and formal science as dealing with ideal categorial forms and their relationships between them, we proceed to explore how any theory of natural science can imply a revision in the formal science.

3.1 — The Quine-Putnam Theses

    One of the most controversial subjects in philosophy of science has to do with the underdetermination of natural science. Most people refer to the Duhem-Quine Thesis as one of its foundations. It should be mentioned here that there is no such thing as the Duhem-Quine Thesis. As famous as this “thesis” may be, Pierre Duhem and W. V. O. Quine held different points of view concerning natural science and how its theories affect other branches of knowledge.

    This should be corrected because this term has been widely used in the fields of epistemology and philosophy of science. Donald Gillies made an excellent exposition about the similarities and differences regarding Duhem's thesis and Quine's thesis. Pierre Duhem said that in the case of physics an experiment can never condemn a hypothesis but a whole theoretical group. That what is really put to the test is not merely a hypothesis, but a whole bunch of hypotheses, laws and theories that the tested hypothesis supposes.125 This aspect of physics does not extend to other branches of science such as medicine and physiology, and definitely does not extend to formal science.126 Evidence of this is the fact that he refused to think that the general theory of relativity was legitimate, because its use of non-euclidean geometry goes against our intuition that space is euclidean.127

    Quine holds a very different point of view in “Two Dogmas of Empiricism”. He denied the distinction between analytic and synthetic propositions, and, as a result, he concluded that there is no actual distinction between formal science and natural science except in degrees of abstraction. Since there is no distinction among both sciences, all of the formal and natural posits are nothing more than convenient fictions. Quine says the following in “Two Dogmas”:

    If this view is right, it is misleading to speak of the empirical content of an individual statement—especially if it is a statement at all remote from the experiential periphery of the field. Furthermore it becomes folly to seek a boundary between synthetic statements, which holds contingently on experience, and analytic statements, which hold come what may. Any statement can be held true come what may, if we make drastic enough adjustments elsewhere in the system. Even a statement very close to the periphery can be held true in the face of recalcitrant experience by pleading hallucination or by amending certain statements of the kind called logical laws. Conversely, by the same token, no statement is immune to revision. Revision even of the logical law of the excluded middle has been proposed as a means of simplifying quantum mechanics; and what difference is there in principle between such a shift and the shift whereby Kepler superseded Ptolemy, or Einstein Newton, or Darwin Aristotle? [. . .]

    As an empiricist I continue to think of the conceptual scheme of science as a tool, ultimately, for predicting future experience in light of past experience. Physical objects are conceptually imported into the situation as convenient intermediaries—not by definition in terms of experience, but simply as irreducible posits comparable, epistemologically, to the gods of Homer. For my part I do, qua lay physicist, believe in physical objects and not Homer's gods; and I consider it a scientific error to believe otherwise. But in point of epistemological footing the physical objects and the gods differ only in degree and not in kind. Both sorts of entities enter our conception only as cultural posits. [. . .]

    The over-all algebra of rational and irrational numbers is underdetermined by the algebra of rational numbers, but is smoother and more convenient; and it includes the algebra of rational numbers as jagged on gerry-mandered part. Total science, mathematical and natural and human, is similarly but more extremely under-determined by experience. The edge of the system must be kept squared with experience; the rest with all its elaborate myths or fictions, has as its objective the simplicity of laws.128

    As we can see, Quine's proposal is much more radical than Duhem's, and it does extend to logic and mathematics, specifically he presents the case of quantum logic.

    Hilary Putnam is a bit more careful than Quine. He says that propositions such as “2 + 2 = 4” without a doubt are true and not subject to revision. However, he holds the belief that there are mathematical propositions that are “quasi-empirical”, which may be revised. Therefore there is no such thing as a priori knowledge.129 He seems to equate revisability with empirical experience, and in his mind empiricism implies revision of supposed a priori knowledge. We have argued in the previous chapter against Kitcher that a prioricity is not incompatible with revisability.130 Also Putnam shows the example of quantum logic as an instance of revisability in classic logic. He says:

[in rejecting] the traditional philosophical distinction between statements necessary in some eternal sense and statements contingent in some eternal sense [. . .] could some of the 'necessary truths' of logic ever turn out to be false for empirical reasons? I shall argue that the answer to this question is affirmative.131

    I am inclined to think that the situation is not substantially different in logic and mathematics. I believe that if I had the time I could describe for you a case in which we could have a choice between accepting a physical theory based upon non-standard logic, on the one hand, and retaining standard logic and postulating hidden variables on the other. In this case, too, the decision to retain the old logic is not merely the decision to keep the meaning of certain words unchanged, for it has physical and perhaps metaphysical consequences. In quantum mechanics, for example, the customary interpretation says that an electron does not have a definite position measurement; the position measurement causes the electron to take on suddenly the property that we call its 'position' (this is the so-called 'quantum jump'). Attempts to work out a theory of quantum jumps and of measurement in quantum mechanics have been notoriously unsuccessful to date. It has been pointed out that it is entirely unnecessary to postulate the absence of sharp values prior to measurement and the occurrence of quantum jumps, if we are willing to regard quantum mechanics as a theory formalized within a certain non-standard logic, the modular logic proposed in 1935 by Birkhoff and von Newmann, for precisely the purpose of formalizing quantum mechanics.132

Therefore, we have here two philosophers who seem to argue that natural science can indeed revise formal science. Their statement can be summarized in two theses, which shall be called here the Quine-Putnam Theses:133
  1. First Quine-Putnam Thesis: Mathematics and logic can be revised in light of recalcitrant experience as well as changes in scientific theories.

  2. Second Quine-Putnam Thesis: Mathematics exists because it is indispensable to science. This is the so-called indispensability argument.
Here I shall discuss both of these theses in light of the case they present and the refutation of such claims.

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3.2 — Quantum Logic

    One of the most cited cases we see in Quine's and Putnam's arguments about the possibility of revising classic logic is the famous quantum logic which has as its basis the empirical data on quantum behavior. According to classic logic, this well-formed-formula, one distributive law, is a tautology:

(α∧(β∨γ))↔((α∧β)∨(α∧γ))

If this is a tautology, then it is always true, regardless of the truth value assigned to the propositional variables. However, this logical truth would not seem to hold in quantum physics. Martin Curd and  J. A. Cover give us an example of how this is so. Let us look at Illustration 4:

Light Interference Pattern
Illustration 4

It presents us the famous double-slit experiment. If we have a light source on one side of a panel with two slits, we will be able to see an interference pattern in a screen at the other end. If we conceive light as a wave, we will be able to account for the interference pattern in the screen. If we conceive light as made up of photons (light particles), we are not unable to explain that phenomenon. At least according to our experience with particles, the interference pattern should not appear, we should see instead a set of two light bands corresponding to the two slits in the panel. If we cover one of the slits, the interference pattern is not shown anymore; if the two slits are open, then it appears once again. How does the photon “know” that the other is going to pass through the other slit to then form an interference pattern? It might seem that the same photon can pass through both slits to show the interference pattern.

    Now, let us suppose that p is the proposition “The photon is in region R of the screen”, q1 is the proposition “The photon went through slit 1”, and q2 stands for the proposition “The photon went through slit 2”. If the photon goes through slit 1 or slit 2, we do not see the interference pattern formed in the screen. However, if they go through both slits simultaneously, then we can see the pattern. Therefore, this means that:

p ∧ (q1q2)

should not interderive with:

(pq1) ∨ (pq2)

This is true in the quantum world, because a photon is assumed to pass through both slits, not one.134 Is this a refutation of classic logic on empirical grounds, just as the Quine-Putnam Theses suggest?

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3.3 — Refutation of the First Quine-Putnam Thesis

3.3.1 — About the Problem of Quantum Logic

    One of the ironies of philosophy is that one of the philosophers who proposed the First Quine-Putnam Thesis was precisely the one who refuted it: W. V. O. Quine. In his Philosophy of Logic, he discusses many cases of the so-called “deviant logics”, one of them being quantum logic.135  Many of those who favor and those who oppose Quine pay no attention to this very important retraction from statements he made in “Two Dogmas”.

    For Quine, to deny a law of logic or redefine logical connectives according to quantum phenomena would be “changing the subject”. In classic logic, the meaning of logical connectives is defined by their truth values. Quantum logic is not truth functional and we cannot determine through truth tables whether conjunction, disjunction, implication mean the same as in classic logic. Therefore, quantum logic can hardly be considered a refutation of classic logic. At most, it is an alternative logic, but not a refutation of the older one.136  He further says from his pragmatic view:

[. . .] I would cite again the maxim of minimum mutilation as a deterring consideration. [. . .] let us not underestimate the price of a deviant logic. There is a serious loss of simplicity, especially when the new [quantum] logic is not even a many-valued truth-functional logic. And there is a loss, still more serious, on the score of familiarity. Consider again the case [. . .] of begging the question in an attempt to defend classical negation. This only begins to illustrate the handicap of having to think within a deviant logic. The price is perhaps not quite prohibitive, but returns had better be good.

[. . .] Now the present objection from quantum mechanics is in a way reminiscent of this, though without the confusion. [. . .] Certainly a scientist admits as significant many sentences that are not linked in a distinctive way to any possible observations. He admits them so as to round out the theory and make it simpler, just as the arithmetician admits the irrational numbers so as to round out arithmetic and simplify computation; just, also as the grammarian admits such sentences as Carnap's 'This stone is thinking about Vienna' and Russell's 'Quadruplicity drinks procrastination' so as to round out and simplify the grammar. Other things being equal, the less such fat the better; but when one begins to consider complicating logic to cut fat from quantum physics, I can believe that other things are far from equal. The fat must have been admirably serving its purpose of rounding out a smooth theory, and it is rather to be excused than excited.137

    To add to this quinean rejection, many other philosophers and scientists have objected to quantum logic for not helping us understand what happens in the quantum world. For many of them, such a logic only shifts the mystery from quantum physics to logic.138 It is for this reason that many philosophers of science as well as many scientists themselves have completely rejected the Copenhagen interpretation.

    Also, from an epistemological standpoint, this is one attempt to translate quantum phenomena given in experience (a posteriori), and turn it into some sort of a priori logical laws of quanta. The problem relies in the fact that, ideally speaking, there can be numerous possible explanations for that phenomenon, some which may not have been formulated yet. Those who favor quantum logic only rely on one particular interpretation of quantum phenomena, and turn what apparently is a contradiction in light of classic logic into a new kind of logic. The fallacy of this procedure can be seen clearly once we realize that this logic is only valid within a particular a posteriori natural-scientific theory. If in the future such a theory is refuted or abandoned, this new logic will cease to be valid. However, historically, classic logical laws remain true regardless of which a posteriori natural-scientific theories are adopted.

    Finally, we must not forget that the disjunction in the distributive laws is an inclusive disjunction: or one, or the other, or both.

    The norm in science is never to change or revise the axioms and theorems of formal sciences on empirical grounds, but to change the natural-scientific theory so it is consistent with logico-mathematical laws and truths. There is a very simple but good example given by Carl G. Hempel about this:

[. . .] consider now a simple “hypothesis” from arithmetic 3+2=5. If this is actually an empirical generalization of the past experiences, then it must be possible to state what kind of evidence would oblige us to concede the hypothesis was not generally true after all. If any disconfirming evidence for the given proposition can be thought of, the following illustration might well be typical of it: We place some microbes on a slide, putting down first three of them and then another two. Afterward we count all the microbes to test whether in this instance 3 and 2 actually added up to 5. Suppose now what we counted 6 microbes altogether. Would we consider this an empirical disconfirmation of the given proposition, or at least as a proof that it does not apply to microbes? Clearly not; rather, we would assume we had made a mistake in counting or that one of the microbes had split in two between the first and second count. But under no circumstances could the phenomenon just described invalidate the arithmetical proposition in question.139

This illustrates very well the relation between formal sciences and natural sciences. Some events in natural sciences seem to revise mathematics, when in reality they do not. Let us see two more cases where this only seems to happen.

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3.3.2 — General Theory of Relativity and Non-Euclidean Geometry

    One of the most cited arguments in favor of revision of mathematics is the general theory of relativity and its adoption of non-euclidean geometry. It can be said, for instance, that Einstein's discovery of physical space-time being non-euclidean refuted euclidean geometry.140  However, we must look carefully at these claims to understand well what Einstein really did in the case of non-euclidean geometry and his theories of relativity.

    To be able to understand well what happens in the relationship between geometry in general and the general theory of relativity, we should examine the reason why non-euclidean geometry was developed. One of the most significant axioms in euclidean geometry was the so-called “axiom of the parallels” which states that given a line and a non-collinear point, there is one and only one line that goes through that point which is parallel to the given line. For many mathematicians, this axiom was self-evident, but for others it was not. The same assumptions were necessary for the proof of the theorem that stated that the sum of the angles of a triangle is 180°. The more mathematics became an abstract and rigorous discipline, the more the supposed self-evidence of the axiom and the validity of the theorem were questioned. In the eighteenth and nineteenth centuries, there was a conviction among some mathematicians that to deny such an “axiom” would not lead to any contradictions.

    The Jesuit priest Gerolamo Saccheri (1667-1733), after trying to prove the axiom of the parallels, discovered accidentally that consistent non-euclidean geometry is possible. He could not show through the method of Reductio ad Absurdum that the negation of the axiom of the parallels was false. So, without knowing it, he showed that non-euclidean geometry could be consistent and that it could be perfectly possible to conceive the angles of a triangle being less than 180°. He rejected this conclusion on intuitive grounds, but later Carl Friedrich Gauss (1777-1855) realized that non-euclidean geometries are as valid as the euclidean one.

    It was not until János Bolyai (1802-1860) and Nikolai Lobachevsky (1793-1856) that a variant of non-euclidean geometry called “hyperbolic geometry” was developed, which was ignored and rejected by most of the other mathematicians at the time for being counterintuitive. This hyperbolic geometry denied the axiom of the parallels and assumed, not a flat kind of space, but pseudo-spherical. In it, the sum of the angles of the triangle is less than 180°, it was possible to “draw” more lines going through non-collinear points parallel to a given line.

    Another mathematician, Bernard Riemann (1826-1866), developed another kind of non-euclidean geometry called “elliptic geometry”, where the sum of the angles of a triangle is greater than 180°, and where the shortest distance between two points lies in a great circle (the line which divides the sphere in two halves). It also makes possible for more than one line to pass through two points.

    As we can see, these non-euclidean geometries were not grasped by experience in any way, they came out as a direct result of centuries of reflections by mathematicians, especially those in the eighteenth and nineteenth centuries. Such theories did revise mathematics but did not refute euclidean geometry. In fact, euclidean space, under this conception, became one of an infinity of possible mathematical spaces. It did not refute at all that in euclidean space the sum of the angles of the triangle is 180°, or that the Pythagorean Theorem is true. What it did refute was the conception that the only valid geometry is euclidean geometry. Natural science had nothing to do with this revision.

Then what did Einstein do? He was acquainted with the philosophy of the famous mathematician Henri Poincaré, who is considered today one of the fathers of the general theory of relativity. Poincaré accepted the mathematical validity of non-euclidean geometry.141 For him, a non-euclidean world is perfectly possible and is very different from euclidean space,142 but he further states the following:

It is seen that experiment plays a considerable rôle in the genesis of geometry; but it would be a mistake to conclude from that geometry, is, even part, an experimental science [. . .] [Geometry] is not concerned with natural solids: its object is certain ideal solids, absolutely invariable, which are put a greatly simplified and very remote image of them. The concept of these ideal bodies is entirely mental, and experiment is but the opportunity which enables us to reach the idea. The object of geometry is the study of a particular “group”; but the general concept of group pre-exists in our minds, at least potentially. It is imposed on us not as a form of our sensitiveness, but as a form of our understanding; only, from among all possible groups, we must choose one that will be the standard, so to speak, to which we shall refer natural phenomena.

    Experiment guides us in this choice, which it does not impose on us. It tells us not what is the truest, but what is the most convenient geometry. It will be noticed that my description of these [non-euclidean] worlds has required no language other than that of ordinary geometry. Then, were we transported to those worlds, there would be no need to change that language. Beings educated there would no doubt find it more convenient to create a geometry different from ours, and better adapted to their impressions; but as for us, in the presence of the same impressions, it is certain that we should not find it more convenient to make a change.143

    Poincaré's statement regarding non-euclidean geometry is that it is as valid as euclidean geometry, but it would not serve well at all to adopt non-euclidean geometry as a convention in this world. It is perfectly conceivable that it would make sense to adopt non-euclidean geometry as a way to make the theories about the world simpler, even if non-euclidean geometry itself is not as simple as euclidean geometry. But due to the fact that our world seems to be in euclidean space, he rejects the possibility of the eventual adoption of non-euclidean geometry to make scientific theories simpler.

    This is where Einstein comes in. One of the mathematical consequences of the Lorentz Transformations and the adoption of the independence of the constancy of light’s speed with respect to all inertial reference frames is that nothing can travel faster than the speed of light. This left a significant problem: according to newtonian mechanics, the effect of gravity among massive objects is instantaneous, and there is no account for Lorentz's spatial contraction. Poincaré influenced Einstein by letting him see that it was possible to adopt a more complicated mathematical model in order to simplify a scientific theory. Due to the special theory of relativity we cannot talk about rigid bodies, i.e. bodies in which the relative length, time frame, and mass are not affected due to its speed with respect to other inertial reference frames. Euclidean geometry would be an inappropriate model to build a theory using special relativity. So, he had two options:
  1. To retain euclidean geometry as the mathematical model for simplicity, which would mean sacrificing the simplicity of the scientific theory about space-time behavior.

  2. To adopt a more complicated non-euclidean geometry as a mathematical model, but having the benefit of a simpler scientific theory.144
By choosing the latter, Einstein not only formulated a very consistent general theory of relativity, but also was able to predict and include a series of phenomena which were not accounted for in classic newtonian mechanics: the Second Twin Paradox, the way light deviates near massive objects, the motion of Mercury's Perihelion, and the Doppler Effect.145

    So, what we see here in the case of general theory of relativity is not that it refuted euclidean geometry. Euclidean geometry itself does not contradict non-euclidean geometry, because an euclidean space is one of an infinity of possible spaces. Non-euclidean geometry came to be because of internal problem solving processes within mathematics itself, and its historical origin has nothing to do with its adoption or rejection within natural science.

    Therefore, the general theory of relativity did not revise mathematics at all. Quite the contrary. Einstein chose another mathematical model of space which was available thanks to mathematicians' development of non-euclidean geometry the previous century. He formulated the simplest theory when he considered the mathematical implications of the special theory of relativity as well as other phenomena. Instead of natural science revising mathematics, it was mathematics the field that revised natural science.

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3.3.3 — Chaos Theory and Mathematics

Recently there has been an enthusiasm about chaos theory, even to the point of the absurd, mostly as a result of propaganda within the academy.146  Some have presented chaos theory as a refutation of mathematical method in general. What is chaos theory? Alan Sokal and Jean Bricmont explain this very well:

What is chaos theory about? There are many physical phenomena governed by deterministic laws, and therefore, predictable in principle, which are nevertheless unpredictable in practice because of their “sensitivity to initial conditions”. This means that two systems obeying the same laws may, at some moment in time, be in very similar (but not identical) states and yet, after a brief lapse of time, find themselves in very different states. This phenomenon is expressed figuratively by saying that a butterfly flapping its wings today in Madagascar could provoke a hurricane three weeks from now in Florida. Of course, the butterfly by itself doesn't do much. But if one compares the two systems constituted by Earth's atmosphere with and without the flap of the butterfly's wings, the result three weeks from now may be very different (a hurricane or not). One consequence of this is that we do not expect to be able to predict the weather more than a few weeks ahead. Indeed, one would have to take into account such a vast quantity of data, and with such precision, that even the largest conceivable computers could not begin to cope.147

    This is illustrated best with what occurred to one of the fathers of chaos theory, Edward Lorenz. He discovered what would later be known as the “butterfly effect”, especially in relation to the weather. He used attractors in order to describe the behavior of certain systems. Chaotic behavior, in chaos theory, does not mean just pure disorder or pure randomness. A system is chaotic if it depends greatly in the sensitivity of initial conditions. Lorenz, studying the weather and picking up data, eventually showed with an attractor, the behavior of a chaotic system. Illustration 5 is a display of what has come to be known as the Lorenz attractor.

Lorenz Attractor
Illustration 5

    The attractor shows that even in what appears to be disorderly behavior, there is an inherent structure within the stream of data, even when the trajectories never intersect, and the system never repeats itself. Such a view of chaotic patterns has been very useful in explaining, for instance, Jupiter's Red Spot, which is essentially a self-organizing system within a chaotic system. This seems to apply, not only to nature, but also to economy, population growth, and so on.148

    Chaos theory also includes the idea of the fractal aspect of such behavior. Among many scientists and mathematicians, it was Benoit Mandelbrot who discovered accidentally that a diagram of income distribution can be correlated with the diagram of eight years of cotton prices. Gleick tells more of this story:

[. . .] when Mandelbrot sifted the cotton-price data through IBM's computers, he found the astonishing results he was seeking. The numbers that produced aberrations from the point of view of normal distribution produced symmetry from the point of view of scaling. Each particular price change was random and unpredictable. But the sequence of changes was independent of scale: curves for daily price changes and monthly price changes matched perfectly. Incredibly, analyzed Mandelbrot's way, the degree of variation had remained constant over a tumultuous sixty-year period that saw two World Wars and a depression.149

    So, we see not only that there is an order within the pattern as discovered by Lorenz, but also, in a sense, there was a correlation between the whole and the parts of a chaotic system. Mandelbrot could calculate the fractional dimensions of real objects according to shape or any other irregular patterns. And it does not matter which dimensional fraction we reduce it to, we are able to see that irregular pattern again and again. He created the word “fractal” to refer to these fractional dimensions and “fractal geometry”, to create the discipline which has fractals as its objects of study.

    This non-conventional way of looking at the world and the creation of such a mathematical discipline was a very important step in understanding the behavior of the physical world. Up to now we have seen chaotic systems and fractals and their relationship with the physical world. What about the mathematical realm? Many of these views apparently also apply to pure mathematical objects, such as the very well known Mandelbrot Set. Gullberg explains in full detail what the Mandelbrot Set is:

The fractal behavior in the complex number plane is demonstrated by iterating a nonlinear function whose variables include its own result. If a set of an infinite sequence f(z), f(f(z)), f(f(f(z)))..., where z is a complex number, is plotted on a graph, the sequence of iterates may
  1. be unbounded; or
  2. jump around within a bounded region
If (2) holds, we say that z lies in the “filled-in Julia set for f” [. . .]

    The Mandelbrot set is related to the Julia set, but for it the defining variable is the c in f(z)=z²+c, where z and c are complex numbers. Starting with z=0+0i, we look for the complex numbers c, such that 0, f(0), f[f(0)], ... remain bounded.

    If we let z=0+0i in f(z)=z²+c, then

f(z) = f(0+0i) = (0+0i)2 + c = c

f(f(z)) = f(c) = c2 + c

f(f(f(z))) = f(c2 + c) = (c2 + c)2 + c

and the process may be iterated ad infinitum. [. . .]

    We are now in a position to define the Mandelbrot set as the set of complex numbers c for which the iterated f(z)=z²+c remains bounded. The initial value of z is 0+0i and each subsequent value of z is used to find the next one.150

A more formal definition of the Mandelbrot set is the following:

Definition. The Mandelbrot Set M is the set of complex numbers c such that the sequence Sequence does not approach ∞ as n gets larger.

    Through the process of iteration in a computer program, we can actually produce Illustration 6, which is the graphical representation of the Mandelbrot Set.

Mandelbrot Set
Illustration 6

The image, as complex and irregular as it may appear, has also in it an intrinsic pattern. Using a certain sequence of finding fractions on the Mandelbrot Set, we are able to find again a fraction that contains once more its original image. In Illustration 7, the white rectangles show how we can “zoom in” the Mandelbrot Set, and find gradually the same image pattern of the Mandelbrot Set. If we repeat that process, we will find another image of the Mandelbrot Set, and so on.

Mandelbrot  Set - Fractal 1
1
Mandelbrot Set - Fractal 2
2
Mandelbrot Set - Fractal 3
3
Mandelbrot Set - Fractal 4
4
Mandelbrot Set - Fractal 5
5
Mandelbrot Set - Fractal 6
6
Illustration 7

[Top]

    So, it seems that once again we are apparently faced with a possibility that empirical sciences have revised mathematics. The reasoning we apply in empirical experience is the same we apply to mathematical objects, because fractal reasoning applies to objects of sensible experience and also to certain mathematical objects. This reasoning itself is based on experience. Therefore, on the basis of sensible experience, mathematical reasoning has been revised.

    To be able to understand this well, we have to distinguish two very important sides of chaos theory, one that has to do with natural and empirical sciences, and another solely having to do with pure mathematics. Some people have alleged that chaos theory adds uncertainty to mathematics, especially on the basis of experience. First, I wish to ask: if mathematics is uncertain on the basis of experience, then what guarantees the certainty of chaos theory in the first place? If chaos theory in a sense refutes mathematical certainty, then why does it use mathematically certain rules to be able to understand this with certainty?

    Alan Sokal and Jean Bricmont have pointed out the confusion of those who argue this way. They confuse determinism with predictability, but this aspect applies only to empirical sciences, not to pure mathematics. Chaos theory does not refute determinism at all, all chaotic systems in the world are determined according to physical laws. They just have the peculiar aspect of its determination depending on the sensitivity of initial conditions. However, due to the fact that we are not able to account for each and every single variable that intervenes in a chaotic system, we are not able to predict with 100% accuracy certain phenomena. That is why Edward Lorenz discovered that we are able to predict the weather only in short term within a statistical model, and such a prediction loses its certainty as time goes by.151

    But none of this revises mathematics at all, on the contrary, as I will show, the application of certain mathematical chaotic notions such as strange attractors or fractals, is no different from the application of non-euclidean geometry to physics. So, for this discussion we will have to look at the part of chaos theory that deals with mathematics.

    In general, there are some misuses of the notion of fractals that should be mentioned here. Notice that many of the advocates for fractal geometry say that fractals are a more accurate representation of reality. As Gleick said about Mandelbrot:

Clouds are not spheres, Mandelbrot is fond of saying. Mountains are not cones. Lightning does not travel in a straight line. The new [fractal] geometry mirrors a universe that is rough, not rounded, scabrous, not smooth. It is a geometry of the pitted, pocked, and broken up, the twisted, tangled, intertwined.152

The classic way in which Mandelbrot confronts a certain problem concerning the usual way we do geometry, is to ask: “How long is the Coast of Britain?” Mandelbrot found out that Lewis F. Richardson saw discrepancies about 20% in the estimated lengths of the coasts of Spain, Portugal, Belgium, and the Netherlands. Mandelbrot wanted to take another approach: the fractal approach. He arrived to the conclusion that a coastline is infinitely long. In theory, if we continue “zooming in” the coastline, not only will everyone discover how long it is, but also at one point, we will see the same irregular shapes as the original (as the famous fractal shore illustrates).153 But is this true?

    Gullberg comments about this:

The universe is replete with shapes that repeat themselves on different scales within the same object. In Mandelbrot's terminology, such objects are said to be self-similar.

    In the idealized world of mathematics, there are several well defined figures that are self-similar and an infinite number of such figures may be generated through iteration of functions [. . .] The word fractal — coined by Mandelbrot — was intended to describe a dimension that could not be expressed as an integer, today, “fractal” is generally understood to mean a set that is self-similar under magnification.

    Unlike mathematical fractals, no object in nature can be magnified an infinite number of times and still present the same shape of every detail in successive magnifications – one reason being the finite size of molecules and atoms. Yet fractal models may provide useful approximations of reality over a finite range of scales.

    Mandelbrot and others have applied fractals as explanatory models of natural phenomena involving irregularities on different size scales. This technique is used in graphical analysis in such diverse fields as fluid mechanics, economics, and linguistics and the study of crystal formation, vascular networks in biological tissue, and population growth.154

The word “models” here is key to understand exactly what is going on. As we can see, fractal geometry is as much an approximation to reality as euclidean and non-euclidean geometries are. What chaos theorists do essentially is use fractal geometry and many other mathematical notions and apply them to experience, the very same way non-euclidean geometry was applied to simplify scientific theory and explain the physical world more accurately. In this way, fractal geometry helps us to understand better the chaotic systems in the world. None of this refutes the validity of euclidean geometry at all nor any other mathematical axiom or theorem. The choice of the mathematical models depend greatly on which kind of natural-scientific theory we choose, how that model is pertinent to it, and if it really simplifies the theory in such a way that actually makes a better understanding of the world possible.

    So, attempts to make chaos theory a way to revise formal science basing ourselves on empirical experience is also doomed to failure.

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3.3.4 — The Paradox of Revisability

    As we said in Chapter 2, we cannot forget the paradox of revisability pointed out by Jerrold Katz. This is a big headache to all of those who believe in the First Quine-Putnam Thesis, because this paradox discovers two facts: the absolute necessity of some basic logical truths such as the principle of no-contradiction, and it also discovers the inviability of the potential revision of all formal science.

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3.4 — Reply to Second Quine-Putnam Thesis

    The Second Quine-Putnam Thesis has been known as the “indispensability argument”, which states that mathematics is meaningful because of the fact that it is indispensable to science. This is related to the First Quine-Putnam Thesis, that somehow formal sciences are revised in light of recalcitrant experience. I wish to point out the indispensability argument as a strange claim.

    Rosado Haddock says that if mathematics is subordinated to physics, it is strange that mathematics does not refer at all to physical entities or theories of any kind. In fact, it seems that contrary, to physical theories, many mathematical truths are self-evident and true in every possible world.

Now, although applicable to the physical (and other) sciences, mathematical theorems seem to be true even if all actually accepted physical theories were false and, thus, the claim that only after the advent of modern physical science can we argue that mathematical theorems are true seems really amazing, to say the least. It is also extremely unreasonable to think that before the advent of modern physical science there was no way to establish the existence of mathematical entities, thus, e.g., that there exists an immediate successor of 3 in the natural number series. Moreover, it is perfectly conceivable that there exists a world in which all mathematical theorems known to present-day mathematicians are true (supposing that current mathematics is consistent), and that mathematicians know as much mathematics as they actually know, but in which none of the physical laws accepted as true nowadays were known to humanity. What is not possible is a world in which physical science were as developed as it actually is, but in which our present mathematical theories (especially those applicable to present-day physical science) were not valid, or, at least, were not considered to be valid.155

    Katz also made his criticism along this line, stating that we can establish the existence of these mathematical entities even without empirical science.156 So, can we remain with a straight face when we state that the validity of mathematics depends on the validity of scientific theories? It seems the other way around. We admit that these replies to the Second Quine-Putnam Thesis are not a refutation per-se of the claims, but they show how unlikely this thesis seems to be.

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Footnotes:

125Duhem, 1991, pp. 183-188; Gillies, 1993, pp. 98-99.  [Return to Text]

126Duhem, 1991, pp. 180-183.  [Return to Text]

127Curd & Cover, 1998, p. 377; Gillies, 1993, p. 105.  [Return to Text]

128Quine, 1953, pp. 43-45.  [Return to Text]

129Putnam, 1975, pp. 124-126.  [Return to Text]

130See Hale's (1987) comments on Putnam's view on revisability of a priori disciplines (p. 143).  [Return to Text]

131Putnam, 1975, p. 174.  [Return to Text]

132Putnam, 1975, p. 248.  [Return to Text]

133This is a phrase used by Katz (1998) to refer to Quine's and Putnam's statement on the revisability of formal sciences in light of experience (p. 50).  [Return to Text]

134Curd & Cover, 1998, p. 380.  [Return to Text]

135The other “deviant logics” Quine (1970) mentions are intuitionistic logic (which rejects the principle of excluded middle) and various multi-valued logics.  [Return to Text]

136Quine, 1970, pp. 83-86.  [Return to Text]

137Quine, 1970, p. 86.  [Return to Text]

138Curd & Cover, 1998, p. 380.  [Return to Text]

139Hempel, 2001, p. 4, my italics.  [Return to Text]

140Putnam, 1975, pp. xv-xvi.  [Return to Text]

141Poincaré, 1952, p. 50.  [Return to Text]

142Poincaré, 1952, pp. 64-68.  [Return to Text]

143Poincaré, 1952, pp. 70-71, my italics.  [Return to Text]

144Einstein, 1983, pp. 33-35, 39.  [Return to Text]

145See also Carnap's comments in Reichenbach, 1958, p. v.  [Return to Text]

146I need not emphasize the huge problems of certain “thinkers” who use chaos theory to support the latest nonsense that comes to their mind. Alan Sokal and Jean Bricmont illustrate very well the overwhelming confusions concerning so-called “thinkers” like Jean-François Lyotard, Jean Baudrillard, Gilles Deleuze, and Félix Guattari (Sokal & Bricmont, 1999, pp. 147-168). For a very sober research on chaos theory, Sokal and Bricmont have suggested the following readings: Kadanoff, 1986; Matheson & Kirchoff, 1997; Ruelle, 1991; and Van Peer, 1998.  [Return to Text]

147Sokal & Bricmont, 1998, p. 138.  [Return to Text]

148Gleick, 1987, p. 55.  [Return to Text]

149Gleick, 1987, p. 86.  [Return to Text]

150Gullberg, 1997, p. 633.  [Return to Text]

151Sokal & Bricmont, 1998, pp. 140-146.  [Return to Text]

152Gleick, 1987, p. 94.  [Return to Text]

153Gleick, 1987, pp. 94-96.  [Return to Text]

154Gullberg, 1997, p. 626, my italics.  [Return to Text]

155Hill & Rosado, 2000, p. 269.  [Return to Text]

156Katz, 1998, pp. 50-51.  [Return to Text]



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