Gibbs, Boltzmann, and negative temperatures

Abstract

In a recent paper, Dunkel and Hilbert [Nature Physics 10, 67-72 (2014)] use an entropy definition due to Gibbs to provide a 'consistent thermostatistics' which forbids negative absolute temperatures. Here we argue that the Gibbs entropy fails to satisfy a basic requirement of thermodynamics, namely that when two bodies are in thermal equilibrium, they should be at the same temperature. The entropy definition due to Boltzmann does meet this test, and moreover in the thermodynamic limit can be shown to satisfy Dunkel and Hilbert's consistency criterion. Thus, far from being forbidden, negative temperatures are inevitable, in systems with bounded energy spectra.

9 pages, 3 figures, RevTeX 4.1 -- conditionally accepted Am J Phys, with minor changes from previous version

References in corpus (4)

• Negative Absolute Temperature for Motional Degrees of Freedom
• Equilibration rates and negative absolute temperatures for ultracold atoms in optical lattices
• Atomic Gases at Negative Kinetic Temperature
• System-size scaling of Boltzmann and alternate Gibbs entropies

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