Fluctuation dynamics, thermodynamic analogies and ergodic behavior for nonequilibrium-independent rate processes with dynamical disorder

Marcel Ovidiu Vlad, John Ross and Michael C. Mackey

Physica A: Statistical Mechanics and its Applications, 1997, vol. 243, issue 3, 340-361

Abstract: The stochastic properties of the sojourn times attached to a Markov process in continuous time and with a finite number of states are described by using a statistical ensemble approach. This approach is applied for investigating the large time behavior of independent rate processes with dynamical disorder. The large time behavior of the system is described in terms of an effective transport operator which can be expressed as a static average with respect to the stochastic properties of the sojourn times. The method is illustrated by the generalization of the Van den Broeck approach to the generalized Taylor diffusion. Explicit formulas for the effective transport coefficients and for the fluctuations of the concentration fields are derived. The results are used for extending the non-equilibrium generalized thermodynamic formalisms suggested by Keizer and by Ross, Hunt and Hunt to systems with dynamical disorder. It is shown that the logarithm of the probability density functional of concentration fluctuations is a Lyapunov functional of the effective transport equation. This Lyapunov functional plays the role of a generalized nonequilibrium thermodynamic potential which may serve as a basis for a thermodynamics description of the average behavior of the system. The existence and stability of a steady state can be expressed as an extremum condition for the Lyapunov functional. For Taylor diffusion in an external electric field different from zero the generalized potential has a structure similar to the Helmholtz free energy rather than to the entropy. A generalized chemical potential is derived as the functional derivative of the Lyapunov functional with respect to the concentration field; the gradient of this generalized chemical potential is the driving force which determines the structure of the effective transport equation.

Date: 1997
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Persistent link: https://EconPapers.repec.org/RePEc:eee:phsmap:v:243:y:1997:i:3:p:340-361

DOI: 10.1016/S0378-4371(97)00263-X

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