Local Detailed Balance : A Microscopic Derivation

TL;DR

This paper derives a microscopic basis for local detailed balance in non-equilibrium systems, connecting microscopic dynamics with mesoscopic transition rates and fluctuation relations, especially in thermal contact scenarios.

Contribution

It provides a microscopic derivation of local detailed balance and fluctuation relations for systems with finite configurations exchanging conserved quantities.

Findings

Transition rates obey local detailed balance under certain assumptions.

Derived fluctuation relation for heat exchange in finite-time evolution.

Generalized framework for systems exchanging energy, volume, and matter with reservoirs.

Abstract

Thermal contact is the archetype of non-equilibrium processes driven by constant non-equilibrium constraints when the latter are enforced by reservoirs exchanging conserved microscopic quantities. At a mesoscopic scale only the energies of the macroscopic bodies are accessible together with the configurations of the contact system. We consider a class of models where the contact system, as well as macroscopic bodies, have a finite number of possible configurations. The global system with only discrete degrees of freedom has no microscopic Hamiltonian dynamics, but it is shown that, if the microscopic dynamics is assumed to be deterministic and ergodic and to conserve energy according to some specific pattern, and if the mesoscopic evolution of the global system is approximated by a Markov process as closely as possible, then the mesoscopic transition rates obey three constraints. In the limit where macroscopic bodies can be considered as reservoirs at thermodynamic equilibrium (but with different intensive parameters) the mesoscopic transition rates turn into transition rates for the contact system and the third constraint becomes local detailed balance ; the latter is generically expressed in terms of the microscopic exchange entropy variation, namely the opposite of the variation of the thermodynamic entropy of the reservoir involved in a given microscopic jump of the contact system configuration. For a finite-time evolution after contact has been switched on we derive a fluctuation relation for the joint probability of the heat amounts received from the various reservoirs. The generalization to systems exchanging energy, volume and matter with several reservoirs, with a possible conservative external force acting on the contact system, is given explicitly.