Abstract
The status of the Gibbs and Boltzmann expressions for entropy has been a matter of some confusion in the literature. We show that: (1) the Gibbs H function yields the correct entropy as defined in phenomenological thermodynamics; (2) the Boltzmann H yields an “entropy” that is in error by a nonnegligible amount whenever interparticle forces affect thermodynamic properties; (3) Boltzmann's other interpretation of entropy, S = k log W, is consistent with the Gibbs H, and derivable from it; (4) the Boltzmann H theorem does not constitute a demonstration of the second law for dilute gases; (5) the dynamical invariance of the Gibbs H gives a simple proof of the second law for arbitrary interparticle forces; (6) the second law is a special case of a general requirement for any macroscopic process to be experimentally reproducible. Finally, the “anthropomorphic” nature of entropy, on both the statistical and phenomenological levels, is stressed.
Dates
Type | When |
---|---|
Created | 20 years ago (Aug. 22, 2005, 3:01 p.m.) |
Deposited | 2 years, 1 month ago (July 13, 2023, 1:49 a.m.) |
Indexed | 3 days, 8 hours ago (Aug. 31, 2025, 6:30 a.m.) |
Issued | 60 years, 4 months ago (May 1, 1965) |
Published | 60 years, 4 months ago (May 1, 1965) |
Published Online | 20 years, 1 month ago (July 8, 2005) |
Published Print | 60 years, 4 months ago (May 1, 1965) |
@article{Jaynes_1965, title={Gibbs vs Boltzmann Entropies}, volume={33}, ISSN={1943-2909}, url={http://dx.doi.org/10.1119/1.1971557}, DOI={10.1119/1.1971557}, number={5}, journal={American Journal of Physics}, publisher={American Association of Physics Teachers (AAPT)}, author={Jaynes, E. T.}, year={1965}, month=may, pages={391–398} }