English

Thermodynamic fluctuation relation for temperature and energy

Statistical Mechanics 2009-10-15 v2

Abstract

The present work extends the well-known thermodynamic relation C=β2<δE2>C=\beta ^{2}< \delta {E^{2}}> for the canonical ensemble. We start from the general situation of the thermodynamic equilibrium between a large but finite system of interest and a generalized thermostat, which we define in the course of the paper. The resulting identity <δβδE>=1+<δE2< \delta \beta \delta {E}> =1+< \delta {E^{2}}% > \partial ^{2}S(E) /\partial {E^{2}} can account for thermodynamic states with a negative heat capacity C<0C<0; at the same time, it represents a thermodynamic fluctuation relation that imposes some restrictions on the determination of the microcanonical caloric curve β(E)=S(E)/E\beta (E) =\partial S(E) /\partial E. Finally, we comment briefly on the implications of the present result for the development of new Monte Carlo methods and an apparent analogy with quantum mechanics.

Keywords

Cite

@article{arxiv.cond-mat/0702031,
  title  = {Thermodynamic fluctuation relation for temperature and energy},
  author = {L. Velazquez and S. Curilef},
  journal= {arXiv preprint arXiv:cond-mat/0702031},
  year   = {2009}
}

Comments

Version accepted for publication in J. Phys. A: Math and Theo

R2 v1 2026-07-22T11:42:48.040Z