Department of Chemistry, Colorado State University, Fort Collins, Colorado 80523, USA.
Phys Rev E. 2019 Nov;100(5-1):050603. doi: 10.1103/PhysRevE.100.050603.
We propose a generalization of stochastic thermodynamics to systems of active particles, which move under the combined influence of stochastic internal self-propulsions (activity) and a heat bath. The main idea is to consider joint trajectories of particles' positions and self-propulsions. It is then possible to exploit formal similarity of an active system and a system consisting of two subsystems interacting with different heat reservoirs and coupled by a nonsymmetric interaction. The resulting thermodynamic description closely follows the standard stochastic thermodynamics. In particular, total entropy production, Δs_{tot}, can be decomposed into housekeeping, Δs_{hk}, and excess, Δs_{ex}, parts. Both Δs_{tot} and Δs_{hk} satisfy fluctuation theorems. The average rate of the steady-state housekeeping entropy production can be related to the violation of the fluctuation-dissipation theorem via a Harada-Sasa relation. The excess entropy production enters into a Hatano-Sasa-like relation, which leads to a generalized Clausius inequality involving the change of the system's entropy and the excess entropy production. Interestingly, although the evolution of particles' self-propulsions is free and uncoupled from that of their positions, nontrivial steady-state correlations between these variables lead to the nonzero excess dissipation in the reservoir coupled to the self-propulsions.
我们提出了一种将随机热力学推广到活性粒子系统的方法,这些粒子在随机内部自推进(活性)和热浴的共同影响下运动。主要思想是考虑粒子位置和自推进的联合轨迹。然后,可以利用活性系统和由与不同热库相互作用并通过非对称相互作用耦合的两个子系统组成的系统之间的形式相似性。由此产生的热力学描述与标准随机热力学非常相似。特别是,总熵产生Δs_{tot}可以分解为维持性部分Δs_{hk}和过剩部分Δs_{ex}。Δs_{tot}和Δs_{hk}都满足涨落耗散定理。稳态维持性熵产生的平均速率可以通过 Harada-Sasa 关系与波动耗散定理的违反联系起来。过剩熵产生进入 Hatano-Sasa 类似关系,这导致了一个广义的克劳修斯不等式,涉及系统熵的变化和过剩熵产生。有趣的是,尽管粒子自推进的演化是自由的,并且与它们的位置没有耦合,但这些变量之间的非平凡稳态相关性导致与自推进耦合的储层中存在非零的过剩耗散。