Mechanical Proof of the Second Law of Thermodynamics Based on Volume Entropy

Details Mechanical Proof of the Second Law of Thermodynamics Based on Volume Entropy Mechanical Proof of the Second Law of Thermodynamics Based on Volume Entropy

2007-04-19

arxiv.org/abs/0704.2567v1

Studies In History and Philosophy of Modern Physics, Volume 39, Issue 1, January 2008, Pages 181-194

Physics

Condensed Matter

Statistical Mechanics

17 pages, 1 figure

Scientific paper

10.1016/j.shpsb.2007.09.002

In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mechanical foundations of equilibrium thermodynamics on the basis of the Generalized Helmholtz Theorem. It was found that the volume entropy provides a good mechanical analogue of thermodynamic entropy because it satisfies the heat theorem and it is an adiabatic invariant. This property explains the ``equal'' sign in Clausius principle ($S_f \geq S_i$) in a purely mechanical way and suggests that the volume entropy might explain the ``larger than'' sign (i.e. the Law of Entropy Increase) if non adiabatic transformations were considered. Based on the principles of microscopic (quantum or classical) mechanics here we prove that, provided the initial equilibrium satisfy the natural condition of decreasing ordering of probabilities, the expectation value of the volume entropy cannot decrease for arbitrary transformations performed by some external sources of work on a insulated system. This can be regarded as a rigorous quantum mechanical proof of the Second Law. We discuss how this result relates to the Minimal Work Principle and improves over previous attempts. The natural evolution of entropy is towards larger values because the natural state of matter is at positive temperature. Actually the Law of Entropy Decrease holds in artificially prepared negative temperature systems.

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