Similarities and differences between non-equilibrium steady states and time-periodic driving in diffusive systems

被引:22
作者
Busiello, D. M. [1 ,2 ]
Jarzynski, C. [2 ,3 ,4 ]
Raz, O. [3 ,5 ]
机构
[1] Univ Padua, Dipartimento Fis G Galilei, Via Marzolo 8, I-35131 Padua, Italy
[2] Univ Maryland, Inst Phys Sci & Technol, College Pk, MD 20742 USA
[3] Univ Maryland, Dept Chem & Biochem, College Pk, MD 20742 USA
[4] Univ Maryland, Dept Phys, College Pk, MD 20742 USA
[5] Weizmann Inst Sci, Dept Phys Complex Syst, IL-76100 Rehovot, Israel
关键词
periodic driving; non-equilibrium steady state; Fokker-Planck equation; MOLECULAR MOTOR; THERMODYNAMICS; F-1-ATPASE; RATCHETS;
D O I
10.1088/1367-2630/aade61
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
A system that violates detailed balance evolves asymptotically into a non-equilibrium steady state (NESS) with non-vanishing currents. Analogously, when detailed balance holds at any instant of time but the system is driven through time-periodic variations of external parameters, it evolves toward a time-periodic state, which can also support non-vanishing currents. In both cases the maintenance of currents throughout the system incurs a cost in terms of entropy production. Here we compare these two scenarios for one dimensional diffusive systems with periodic boundary condition, a framework commonly used to model biological and artificial molecular machines. We first show that the entropy production rate in a periodically driven system is necessarily greater than that in a stationary system without detailed balance, when both are described by the same (time-averaged) current and probability distribution. Next, we show how to construct both a NESS and a periodic driving that support a given time averaged probability distribution and current. Lastly, we show that although the entropy production rate of a periodically driven system is higher than that of an equivalent steady state, the difference between the two entropy production rates can be tuned to be arbitrarily small.
引用
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页数:11
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