On the derivation of the Onsager relations from the Master equation
β Scribed by M. Moreau
- Publisher
- Springer
- Year
- 1975
- Tongue
- English
- Weight
- 337 KB
- Volume
- 1
- Category
- Article
- ISSN
- 0377-9017
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β¦ Synopsis
The asymptotical properties of a Markov system with discrete states are derived from the Master equation by using the quadratic approximate form of entropy.
In particular, symmetry relations equivalent to the Onsager reciprocal relations are established for time reversal invariant systems.
i.
The Onsager relations may be derived from the hypotheses of the detailed balance, or more generally from time reversal invariance, either by using the Einstein theory of fluctuations [I], or alternatively the Boltzmann equation [2,3]. In fact, it will be shown in this paper that similar relations follow directly from the Master equation for a time reversal invariant Markov system.
Taking the case of a Markov system with a finite number of states, we discuss the symmetry properties of the transition probabilities at first. Then, using the quadratic approximate form of entropy, we study the tendency towards equilibrium, and we derive the Onsager relations by expressing the time-varying probabilities in terms of the average values of convenient constant physical quantities.
π SIMILAR VOLUMES
Instituut voor theoretische fysica, Rijksuniversiteit te Utrecht, Nederland ## Synopsis The 'master equation' describes the behaviour of a macroscopic system in terms of a time dependent probability distribution. It is here shown that, if the initial distribution is concentrated in a small region
The present work consist of two parts: In the first part we apply the method of quasilinearization to the differential equation describing the time development of the quantum-mechanical probability density. In this way we derive the master equation without resorting to perturbation theory. In the se
The Onsager linear relations between macroscopic ows and thermodynamics forces are derived from the point of view of large deviation theory. For a given set of macroscopic variables, we consider the short-time evolution of near-equilibrium uctuations, represented as the limit of ΓΏnite-size condition