Reference CoffaIt would be hard to find a more crucial epistemological problem than that of the character of a priori knowledge.—
Coffa 1991Our “empirical propositions” do not form a homogeneous mass.—
Wittgenstein 19691. Introduction
One way to organize much of twentieth-century philosophy of science is to read it as a series of debates over what had been considered a priori knowledge. Although synthetic a priori knowledge was officially rejected by the Vienna Circle with their adoption of empiricism in the 1929 pamphlet “Wissenschaftliche Weltauffassung: Der Wiener Kreis” (Neurath Reference Neurath, Neurath and Cohen[1929] 1974), parts of knowledge that had been considered a priori by Kant, such as geometry, space and time, causality, and the basic principles of physics, were widely discussed throughout the twentieth century and statements about them have often been given a special role, either as conventions, or as the hard core of scientific theories. One would think that Quine's critique of the analytic-synthetic distinction (Reference Quine1953) would have put the final nail in the coffin of a priori knowledge and that a holism in which all scientific statements are justified empirically has replaced the notion of any special status for what was formerly considered to be a priori. However, several recent discussions have questioned to what extent a priori knowledge has been refuted (Creath Reference Creath1991; Friedman Reference Friedman2001; Hanson and Hunter Reference Hanson and Hunter1992; Stein Reference Stein1992; Richardson Reference Richardson1997). While it is possible to defend Carnap or even Kant from Quinean holistic empiricism, I will take a new approach to the question and argue that the former a priori should be treated as empirical in a very abstract sense but also as conventional. By conventionalism, I mean the idea that some elements of physical theory have a unique epistemological status—one must adopt these elements in order to begin empirical inquiry. They therefore function as an a priori part of our physical theory that is chosen for conceptual or pragmatic reasons, prior to any empirical testing. Though I am willing to concede to Quine that these conventions are ultimately empirical, the picture of knowledge developed here is very different from that developed in Quinean holism in that categories of knowledge can be differentiated. While Quine admits that some elements of empirical theory are much less likely to be revised than others, he underestimates the asymmetric relation between the “hard core” and the “periphery.” It is not just that the periphery is more likely to be revised than the hard core, but rather that the statements of the periphery cannot even be stated, let alone tested, without the hard core functioning as an a priori in the Kantian sense as a necessary precondition.
The literature on conventions in science begins with Mach and Poincaré (who hold that we choose Euclidean geometry to describe space, regardless of what experiment says) and continues with the Vienna Circle, especially Schlick, Carnap, and Reichenbach (in his trilogy of books on space-time). A different interpretation of conventionalism was later developed by C. I. Lewis, Victor Lenzen, Arthur Pap, who is responsible for the term “functional a priori,” and by Russell Norwood Hanson. Kuhn eventually (and tentatively) picked up the idea of a conventional treatment of synthetic a priori knowledge as an explication of his own views (Kuhn Reference Kuhn1990), and Ian Hacking has advocated something similar to conventionalism with his notion of “styles of reasoning” (Hacking Reference Hacking1992). Many of these treatments of a priori knowledge share the idea that what Kant took to be necessary can and indeed has changed through the development of scientific theories.Footnote 1
The development of non-Euclidean geometries, and especially of the General Theory of Relativity (GTR), made a profound impact on philosophy of science in the early twentieth century by showing philosophers that fundamental aspects of physical theory could be changed. Conceptual change of this sort is what many postpositivist philosophers of science, such as Kuhn, Toulmin, Laudan, and Shapere, saw as a fundamentally important aspect of science. Thus, the idea that there are conventions at the heart of science was already well developed prior to the Vienna Circle, continued in the work of the Vienna Circle and in Logical Empiricism, and was maintained even in postpositivist philosophy of science. My aim here is to present a coherent picture of conventionalism.
2. Standard Critiques of Conventionalism
Schlick's Reference Schlick, Feigl and Brodbeck1938 interpretation of conventionalism seems to have been extremely influential, in part because of the influence he had on Reichenbach, but also because it was translated by Herbert Feigl and May Brodbeck and reprinted in their influential collection, Readings in the Philosophy of Science (Schlick Reference Schlick, Feigl and Brodbeck[1938] 1953). Schlick interpreted Poincaré's conventionalism as a version of holism (i.e., the Duhem-Quine thesis), an epistemological interpretation that has been standard ever since, especially in Popper's critique of conventionalism. Since all empirical theories—not just physical geometry—are underdetermined in the Duhemian sense, the major interpretive problem for those who hold the epistemological interpretation of Poincaré's conventionalism is to explain why he holds that only geometry is conventional. Poincaré's conventionalism is limited, so it cannot be equivalent to the Duhem-Quine thesis (or holism).Footnote 2
Schlick's critique of what he calls conventionalism was also very influential, but unfortunately it seems to have muddied the discussion of conventionalism while leaving holism unscathed. Schlick argues that conventionalists are caught in a dilemma (Schlick Reference Schlick, Feigl and Brodbeck[1938] 1953, 187): If conventionalism involves only the choice of symbols or of explicitly defined terms, then conventions are analytic. Conventions, taken as changes in explicit definitions, can only result in trivial notational variation, not genuine change of physical theory. If conventions are synthetic, they are testable empirically and Poincaré's metric conventionalism is empirically false. Schlick argues that natural laws must be treated either as genuine claims, in which case they have truth values, are synthetic, and are to be justified or rejected empirically, or they must be treated as explicitly stipulated definitions, in which case they are analytic, lack truth values, and turn out to be irrelevant to science.
Schlick assumes a position here that is clearly equivalent to a strict form of empiricism and therefore begs the question against Kantian or other idealists. Why should a Kantian accept Schlick's view that all synthetic scientific claims must be justified empirically? Even if we accept the view that a priori justifications of knowledge (e.g., by intuition) are problematic and should be ruled out, it does not follow that all knowledge should be justified in the same way. Rather than defend Kant, the point to emphasize here is that Schlick mistakenly treats all empirical statements as having an equal role in the structure of knowledge. What Schlick misses is the element of scientific theories that function as a priori knowledge.
Michael Friedman has detailed how Schlick's influence changed Reichenbach's views on conventionalism after an exchange of letters between the two. As Friedman points out, Reichenbach's important early critique of conventionalism is lost in his later work where he adopts Schlick's interpretation of conventionalism. Reichenbach's early point is that the GTR has shown that metric conventionalism is false:
[M]athematicians asserted that a geometrical system was established according to conventions and represented an empty schema that did not contain any statements about the physical world. It was chosen on purely formal grounds and might equally well be replaced by a non-Euclidean schema. In the face of these criticisms the objection of the general theory of relativity embodies a completely new idea. This theory asserts simply and clearly that the theorems of Euclidean geometry do not apply to our physical space. (Reichenbach as cited in Friedman Reference Friedman, Salmon and Wolters1994, 26, and in Friedman Reference Friedman1999, 66–67)
Although the underlying mathematical structure of GTR does not have a determinate metric, metric is determined empirically in GTR by the distribution of mass and energy. According to the GTR, we do not conventionally choose a metric geometry—Euclidean geometry is not adequate for the GTR. However, this was not widely understood until the 1970s and 80s, that is, until the relatively contemporary discussion of spacetime theories (Friedman Reference Friedman, Salmon and Wolters1994, 27, 67).Footnote 3
When Reichenbach adopts Schlick's holistic version of conventionalism in The Philosophy of Space and Time (1958), he argues for conventionalism epistemologically, as can be seen especially clearly in his introduction of his theorem (Reference Reichenbach1958, 33). An empirically testable theory is a combination of geometry and physics, so geometries can be conventionally chosen as long as adjustments are made in physics. Mach makes a similar Duhemian argument against absolute theories of space when he incorporates universal forces in his defense of relationalism. Mach argues that we cannot know whether it is absolute space or distant objects plus a universal force that account for inertial effects (Sklar Reference Sklar1974, 201; Reference FriedmanFriedman 1983, 296–301).
It will be useful to compare Schlick and Reichenbach's views with more recent literature on spacetime conventionalism, for we will see a parallel debate developed in the critique of Grünbaum's conventionalism. Grünbaum, to his credit, never accepted Schlick's interpretation of Poincaré's conventionalism. He thought that conventionalism follows not from holism but rather solely from the continuity of space. Friedman objected to Grünbaum's argument in Foundations of Space-Time Theories as follows:
If we are to draw any conclusions about “metrical amorphousness” from the continuity of physical space, we need an additional premise: namely, that the only spatio-temporal relations that objectively exist are topological relations and order relations. It follows from this claim that properties and relations not definable in terms of topological properties and order relations do not objectively exist and, consequently, that a continuous space objectively lacks metrical properties. (Friedman Reference Friedman1983, 304)
To shorten a long story considerably, it is now widely acknowledged that metric conventionalism requires a fully relational theory of space, yet none of the historically accepted space or spacetime theories—Newtonian, STR or GTR—have been fully relational in the required sense. Friedman's point here is essentially the same as Reichenbach's point in 1920, that GTR shows metric conventionalism to be untrue. Thus, the major critique of geometric conventionalism that was developed within the recent literature on space and time argued that physical theory does not support the conventionalist thesis. Sklar would seem to agree with this point when he argues that the only possible way to defend metric conventionalism now is with holism (Sklar Reference Sklar1986). While Schlick and Popper's critique of conventionalism was philosophical, the recent critique was based on natural science.
The recent discussion has shown that with the proper background theory, Poincaré's conventionalism would have been possible. It is a merely contingent fact (and rather surprising too) that uniform acceleration is detectable and unrelativizable, while uniform velocity is not detectable and is relativisable. The most important point for this discussion, however, is that the epistemological status of the metric of space or spacetime changed as we changed background theories. In this case, Newtonian theory and GTR each set the epistemological status of space (or spacetime). In Newtonian theory we know a priori that space is Euclidean, but in GTR, the metric is determined empirically. Thus, background theory and context determine what is a priori and what is empirical, that is, which parts of the theory function as a priori knowledge. For example, the Newtonian theories of space and of motion are empirical theories, but the metric of space is Euclidean and functions as a priori knowledge within Newtonian theory. It is true that an empirical theory determines the metric of space, but only in a very indirect and abstract sense. The metric of space is not testable within any of the historical spacetime theories. Perhaps our current theory of the metric of spacetime received an empirical confirmation, along with the rest of the GTR, but this metric was neither conceived of nor justified by empirical considerations in anything like the way that ordinary empirical claims are.
This viewpoint is, of course, close to Carnap's in that the background commitments of a scientific theory determine what is a priori and what is empirical. However, Carnap makes a mistake in considering the background commitments as a language. He sees a priori truths as analytic, leaving himself vulnerable to Schlick's critique of conventions as trivial, as well as to further critiques by Quine. The process of determining what is a priori and what is empirical is embedded within a physical, empirical theory. It is necessary to develop a considerable amount of theory before empirical tests are possible at all, and even then, it may seem that empirical tests have very little to do with, for example, the truth of Euclidean geometry. Nevertheless, Newtonian theory is ultimately empirical, that is, our change from Newtonian theory to STR and to GTR has an empirical basis.
3. Geometric Conventionalism and the Constitution of Knowledge
Reichenbach introduces his famous distinction between two meanings of ‘a priori’ in the following passage from The Theory Relativity and A Priori Knowledge:
Kant's concept of a priori has two different meanings. First, it means “necessarily true” or “true for all times” and secondly, “constituting the concept of object.” The second meaning must be clarified. According to Kant, the object of knowledge, the thing of appearance, is not immediately given. Perceptions do not give the object, only the material of which it is constructed. Such constructions are achieved by an act of judgment. The judgment is the synthesis constructing the object from the manifold of the perception. (Reichenbach Reference Reichenbach1965, 48)
Constitution needs to be clarified because it could seem to lead immediately to idealism—the construction of physical objects by perception. For example, we might consider that when Kuhn introduces his “changes of world view” language in The Structure of Scientific Revolutions, he says, “I have so far argued only that paradigms are constitutive of science. Now I wish to display a sense in which they are constitutive of nature as well” (Kuhn Reference Kuhn[1962] 1997, 110). Here conventionalists seem to be caught in a further dilemma. If there are synthetic a priori principles, then it seems that one is committed to idealism, since the a priori element in knowledge constitutes the object of knowledge. If, on the other hand, all synthetic statements are a posteriori, then one is committed to empiricism and Schlick's dilemma appears. However, Quine's critique of the analytic-synthetic distinction should give one pause when considering Schlick's dilemma. It may be true that conventionalism is difficult to formulate without the analytic-synthetic distinction, but Schlick's critique is difficult to formulate as well. While the empiricist version of conventionalism seems problematic, I believe that it can be defended and is preferable to idealism.Footnote 4
Fortunately, idealism is not required to defend conventions as functionally a priori; all that is necessary is to recognize the different epistemological status of various parts of a physical theory. All of these parts can be ultimately empirical, but they are not all empirical in the same way, since some are more embedded and less directly testable than others are. C. I. Lewis emphasizes this crucial point in his discussion of how his view differs from that of the Vienna Circle (Lewis Reference Lewis, Goheen and Mothershead[1941] 1970, 106). Even more significantly, some elements of a theory are required before others can be tested or indeed even formulated. By paying attention to what is required for testing, the theory itself tells us what is functionally a priori and what is empirical. Friedman has recently elaborated several examples of a priori elements in physical science (Reference Friedman2001, esp. ch. 2) and there is a long-standing literature on the status of Newton's laws that shows that they cannot all be empirical at the same time (e.g., Pap Reference Pap1946). Although their intent is anticonventionalist, Forster and Sober's defense of the evidential significance of simplicity as a criterion is congenial with the position that I adopt here (Reference Forster and Sober1994). By analyzing Akaike's statistical methods that are widely employed in science, they discover that
the data tell you more than you may have thought…. At least in the context of the curve-fitting problem, Akaike's technical result provides a benchmark that identifies the degree to which simplicity has evidential significance. (Forster and Sober Reference Forster and Sober1994, 27)
However, Forster and Sober do not deny that application of Akaike's theorem requires the use of both physical and (pure) mathematical assumptions. In this sense, a functional a priori remains, and will always remain, even if we discover that we have more of an empirical basis than most had thought when we choose a simpler theory. The ultimate status of some of the fundamental assumptions required to apply Akaike's theorem is ambiguous in a way that supports my claim that classification of scientific principles as a priori or empirical is a pragmatic decision, not a permanent grounding of science:
[T]he assumption that measurement errors are normally distributed around a mean value is so widespread in science that it is often referred to as the law of errors. On the theoretical side, the central limit theorem affords a theoretical explanation of these empirical facts. In a somewhat humorous tone, Cramér (Reference Cramér1946, 232) sums up by quoting Lippman as saying: ‘everyone believes in the law of errors, the experimenters because they think it is a mathematical theorem, the mathematicians because they think it is an experimental fact,’ and adds that ‘both parties are perfectly right, provided that their belief is not too absolute.’ (Forster and Sober Reference Forster and Sober1994, 30)
What we have here is a set of regularity assumptions that come in stronger and weaker mathematical forms. Although the assumptions are consistent with experimental statistical work, they cannot be claimed to have been tested. They are rather assumptions that are required for purely mathematical reasons.
The issue between idealist and empiricist versions of conventionalism seems to come down to whether a priori principles are taken to be analytic or synthetic. Carnap's work represents the fullest working out of the view that a priori principles are analytic, which leaves him open to the criticisms that Quine makes in “Two Dogmas of Empiricism” (Reference Quine1953) and in “Truth by Convention” (Reference Quine1935). Idealist leaning arguments seem to use the notion of constitution in order to distinguish the functionally a priori from the rest of knowledge. For example, according to Reichenbach, it is the constitutive function that gives principles of physics and parts of mathematics their distinctive epistemological status, one that is not captured by strict empiricism and that is masked by holism:
[T]his view is distinct from an empiricist philosophy that believes it can characterize all scientific statements indifferently by the notion “derived from experience.” Such an empiricist philosophy has not noticed the great difference existing between specific physical laws and the principles of coordination and is not aware of the fact that the latter have a completely different status from the former for the logical construction of knowledge. The doctrine of the a priori has been transformed into the theory that the logical construction of knowledge is determined by a special class of principles, and that this logical function singles out this class, the significance of which has nothing to do with the manner of its discovery and the duration of its validity. (Reichenbach Reference Reichenbach1965 as cited in Friedman Reference Friedman, Salmon and Wolters1994, 23, and in Friedman Reference Friedman1999, 62)
Empiricists can explain how it is possible to “harden” any empirical statement, that is, to hold it fixed as a postulate, but this may not be enough of a distinction to overcome holism. Quine is comfortable admitting that in practice, some statements are easy to harden and difficult to test, while others are easy to test and difficult to harden. However, for the functional account of the a priori to be compelling, it is not clear that the division between the a priori and empirical parts of knowledge has to be as hard and fast as the distinction between analytic and synthetic sentences, or as the distinction between constitutive and nonconstitutive elements of knowledge.
First, how the distinction is to be drawn seems less important than showing that there must be some functionally a priori element in order to proceed. If there is always an a priori element of knowledge at least in a functional sense, then there is no need to know in advance what counts as a priori and what does not. When theories are tested or even formulated, many explicit and implicit assumptions are made. It is possible to go back over an experiment and challenge any of these assumptions as long as one is willing to develop an alternative. The functional account of the a priori does not require some aspects of knowledge to be permanently untestable, rather, only that some aspects of theory be accepted conditionally. Second, emphasizing the functional a priori aspect of parts of scientific theories and ignoring the distinction between analytic and synthetic statements avoids the necessity of developing a theory of language or of meaning. Empirical theory determines what is a priori and what is not. Since no theory of meaning and language will be needed, Quine's arguments against Carnap will not apply. Furthermore, Quine's main argument in “Two Dogmas of Empiricism,” that there is no way to explain or justify the analytic-synthetic distinction without begging the question, is simply irrelevant because we are not trying to ground or to justify science. Beyond the usual pragmatic and conceptual arguments, there is no need to justify conventional choices with a philosophical theory—something Quine, as a pragmatist, should know well! As Wittgenstein said, “The difficulty is to realize the groundlessness of our believing” (Reference Wittgenstein1969, 24).
4. Positioning
By embracing empiricism, we can put to rest the epistemological debate between rationalism and empiricism. However, if we wish to understand the nature of science, rather than continue the pretension that we are putting it on a firm foundation, Quinean holism gives us practically no answers, while conventionalism provides a framework for significant contributions to our understanding of scientific knowledge. Since I adopt naturalism, fallibilism, and empiricism, it may seem that I have simply landed with both feet in Quine's camp, and in a sense that is true. The naturalism that I can accept I define negatively as the view that there is no “first philosophy” that is prior to and independent of science. By fallibilism I mean that there are no unrevisable beliefs and no certainty, and by empiricism I mean that all truths, save explicitly stipulated definitions, are empirically justified, though the functionally a priori parts of physical theory are only empirical in the extremely tenuous sense that the general theory that classified them as a priori is an empirical theory.
An interesting extension of Quine's view can be found in Michael Resnik's work on the philosophy of mathematics (Resnik Reference Resnik1997).Footnote 5 Presenting a defense of empiricism and a reduced and subtle kind of realism in mathematics, Resnik defends the indispensability thesis and promotes Quinean holism, arguing that mathematics is not separable from the rest of science and that justification of mathematics, once we move away from local justifications within various branches of mathematics, ultimately involves the role that mathematics plays in science as a whole. Resnik defends epistemic holism by arguing that the objects of physics are not so different from those in mathematics and by accounting for the stability of mathematics pragmatically. Mathematics will be tinkered with less frequently than experimental hypotheses and becomes relatively a priori, that is, more likely to be taken for granted. However, Resnik admits that mathematics is never falsified (Reference Resnik1997, 133), leading one to wonder whether this is not in itself prima facie evidence for a fundamental epistemic difference between mathematics and the rest of science. This difference may not be apparent when one's only concern is the ultimate justification of mathematics, but it is immediately apparent when one considers the very different roles that mathematics and physical theory play in the web of knowledge (to use Quine's term). Thus, in a sense, the difference between Quinean holism and a theory of the functional a priori is a matter of emphasis. Quineans emphasize the (ultimately) empirical nature of mathematical knowledge, while functional a priorists emphasize the conventional basis of scientific knowledge. This does not mean, however, that the ultimate grounding of science is a priori. Science as a whole remains empirical, but saying so tells us very little about science. By simply granting that such grounding is empirical, we can set aside the issue of the ultimate justification of mathematics and other fundamental principles of science and focus attention instead on how these elements of scientific theories function as a priori knowledge and as conventions, which is a much more significant result concerning the structure of science.