Volume 97, Number 3, February 2012
|Number of page(s)||6|
|Published online||31 January 2012|
Nonequilibrium thermodynamics as a gauge theory
Dipartimento di Fisica, Università di Bologna - via Irnerio 46, 40126 Bologna, Italy, EU and INFN, Sezione di Bologna - via Irnerio 46, 40126 Bologna, Italy, EU
Accepted: 13 December 2011
We assume that Markovian dynamics on a finite graph enjoys a gauge symmetry under local scalings of the probability density, derive the transformation law for the transition rates and interpret the thermodynamic force as a gauge potential. A widely accepted expression for the total entropy production of a system arises as the simplest gauge-invariant completion of the time derivative of Gibbs's entropy. We show that transition rates can be given a simple physical characterization in terms of locally detailed balanced heat reservoirs. It follows that Clausius's measure of irreversibility along a cyclic transformation is a geometric phase. In this picture, the gauge symmetry arises as the arbitrariness in the choice of a prior probability. Thermostatics depends on the information that is disposable to an observer; thermodynamics does not.
PACS: 05.70.Ln – Nonequilibrium and irreversible thermodynamics / 02.50.Ga – Markov processes / 11.15.Ha – Lattice gauge theory
© EPLA, 2012
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