Then in the second half of the nineteenth century the work of a new generation of theoretical physicists (including Maxwell in Scotland, Ludwig Boltzmann in Germany, and Josiah Willard Gibbs in America) showed that the principles of thermodynamics could in fact be deduced mathematically, by an analysis of the probabilities of different configurations of certain kinds of system, those systems whose energy is shared among a very large number of subsystems, as for instance a gas whose energy is shared among the molecules of which it is composed. (Ernest Nagel gave this as a paradigmatic example
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