Fluctuation relations and strong inequalities for thermally isolated systems

被引:6
作者
Jarzynski, Christopher [1 ]
机构
[1] Univ Maryland, College Pk, MD 20742 USA
基金
美国国家科学基金会;
关键词
Fluctuation theorems; Adiabatic processes; Second law of thermodynamics; FREE-ENERGY DIFFERENCES; DIFFERENTIAL EQUATIONS; HAMILTONIAN SYSTEM; ADIABATIC THEOREM; NONEQUILIBRIUM MEASUREMENTS; JARZYNSKI EQUALITY; THERMODYNAMICS; FOUNDATIONS; PRINCIPLES; BOLTZMANN;
D O I
10.1016/j.physa.2019.122077
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
For processes during which a macroscopic system exchanges no heat with its surroundings, the second law of thermodynamics places two lower bounds on the amount of work performed on the system: a weak bound, expressed in terms of a fixed-temperature free energy difference, W >= Delta F-T, and a strong bound, given by a fixed-entropy internal energy difference, W >= Delta E-S. It is known that statistical inequalities related to the weak bound can be obtained from the nonequilibrium work relation, < e(-beta W)> = e(-beta Delta FT). Here we derive an integral fluctuation relation < e(-beta x)> = 1 that is constructed specifically for adiabatic processes, and we use this result to obtain inequalities related to the strong bound, W >= Delta E-S. We provide both classical and quantum derivations of these results. (C) 2019 Elsevier B.V. All rights reserved.
引用
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页数:12
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