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- W1973123089 abstract "The description of the steady state by means of a minimum principle is given. Previous attempts to use the entropy production were successful only if the deviations from equilibrium were small. We show how entropy production can be defined so that the principle will hold for arbitrary deviations. The choice is further corroborated by a physical picture: That part of the entropy production which is due to the heat flow to the bath should be divided, not by the temperature of the bath, but by a different temperature. This temperature is determined as a function of the occupation probabilities. Unfortunately, this temperature cannot be defined in an invariant way. The definition is microscopic and holds only for systems that can be described by a linearized master equation. A proof is given that the generalized temperature used in the new entropy-production definition is higher than the equilibrium temperature, but less than or equal to the steady-state temperature. This proof is limited to a two-level system, for which a steady-state temperature can be defined, interacting with a heat reservoir and external radiation, as discussed in the text." @default.
- W1973123089 created "2016-06-24" @default.
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- W1973123089 date "1970-05-01" @default.
- W1973123089 modified "2023-10-18" @default.
- W1973123089 title "Modification of the Minimum-Entropy-Production Principle" @default.
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- W1973123089 doi "https://doi.org/10.1103/physreva.1.1527" @default.
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