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Mancosu - Philosophy of Mathematical Practice (Oxford, 2008).pdf

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408 alasdair urquhartfrom the observational terms. A description and extended critical discussion<strong>of</strong> this picture, known as the ‘Received View on Theories’ can be foundin Suppe (1977). Although only small parts <strong>of</strong> classical physics were in factgiven an axiomatic form by the philosophers <strong>of</strong> science <strong>of</strong> the day, there wasconsiderable optimism that larger and larger parts <strong>of</strong> science, or at least themore formal parts, could be formulated as sets <strong>of</strong> logical postulates and rules.This approach to the philosophy <strong>of</strong> science, one that is associated with thenames <strong>of</strong> neo-positivist philosophers such as Carnap, Reichenbach, Hempel,Feigl, and others, is now almost totally out <strong>of</strong> style. There are good reasons forthis. The actual formulation <strong>of</strong> non-trivial scientific theories as logical edificesis a difficult task, demanding very good knowledge <strong>of</strong> both the scientificliterature and the mathematical concepts needed to make the methods <strong>of</strong> agiven area precise, and it is not surprising that philosophers and logicians neveraccomplished more than a very small fraction <strong>of</strong> what they had set out to do.In any case, the relationship between theory and applications is surelymore complicated than the schematic ideas propounded in the philosophicalliterature <strong>of</strong> the immediate post-war period. The ‘theory and interpretation’view is that the application <strong>of</strong> a theory can be reduced to the ‘theory andmodel’ paradigm beloved <strong>of</strong> model theorists. So, for example, we can formulatethe abstract theory <strong>of</strong> groups as a first-order theory with a single operationrepresenting group composition. An applied version <strong>of</strong> this theory would begiven by an interpretation in terms <strong>of</strong> a particular group, say, for example, thegroup <strong>of</strong> rigid motions in Euclidean 3-space.This view is attractive and elegant. However, it is hard to square with theactual practice <strong>of</strong> scientists. The world is so complex that physicists who areattempting to provide mathematical models <strong>of</strong> physical reality do not in generalbegin by a direct attempt to formulate theories in which the primitive termscan be given an immediate empirical interpretation. Rather, they very <strong>of</strong>tenconstruct idealized mathematical models in which the behaviour <strong>of</strong> certainvariables bears at least a qualitative resemblance to the real world—if theresemblance can be quantified, so much the better.¹As an example <strong>of</strong> such a model, let us look at a well-known model<strong>of</strong> ferromagnetism, the so-called Curie–Weiss model, described in mostelementary textbooks <strong>of</strong> statistical physics (Thompson, 1972, pp. 95–105),(Yeomans, 1992, pp. 50–54). The empirical phenomenon to be explained isthe spontaneous magnetization <strong>of</strong> ferromagnetic materials. If we cool a sample<strong>of</strong> such a material, while subjecting it to a magnetic field, then there is a sharply¹ Recent work on the role <strong>of</strong> models and idealization can be found in the two collections Morganand Morrison (1999) and Jones and Cartwright (2005).

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