宏观热力学系统的非静态响应系数和耗散可用性

IF 1.1 Q3 PHYSICS, MULTIDISCIPLINARY Journal of Physics Communications Pub Date : 2023-12-27 DOI:10.1088/2399-6528/ad1597
Yuki Izumida
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引用次数: 0

摘要

有限时间热力学过程的表征对于将平衡热力学扩展到非平衡热力学至关重要。核心问题是量化热力学变量的响应以及与施加于系统的热动力的非定量变化相关的不可逆耗散。在这项研究中,我们推导出一个简单的公式,将非定量响应系数与昂萨格动力学系数结合起来,其中昂萨格系数表征了半显微系统广泛热力学变量波动的弛豫动力学。此外,热力学长度和耗散的可用性可量化不可逆热力学过程的效率,它们是根据推导出的非等静态响应系数计算得出的。本结果通过使用理想气体模型进行验证。本结果原则上可通过实验验证,因此有望为宏观热力学系统的非平衡控制提供指导原则。
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Non-quasistatic response coefficients and dissipated availability for macroscopic thermodynamic systems
The characterization of finite-time thermodynamic processes is of crucial importance for extending equilibrium thermodynamics to nonequilibrium thermodynamics. The central issue is to quantify responses of thermodynamic variables and irreversible dissipation associated with non-quasistatic changes of thermodynamic forces applied to the system. In this study, we derive a simple formula that incorporates the non-quasistatic response coefficients with Onsager’s kinetic coefficients, where the Onsager coefficients characterize the relaxation dynamics of fluctuation of extensive thermodynamic variables of semi-macroscopic systems. Moreover, the thermodynamic length and the dissipated availability that quantifies the efficiency of irreversible thermodynamic processes are formulated in terms of the derived non-quasistatic response coefficients. The present results are demonstrated by using an ideal gas model. The present results are, in principle, verifiable through experiments and are thus expected to provide a guiding principle for the nonequilibrium control of macroscopic thermodynamic systems.
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来源期刊
Journal of Physics Communications
Journal of Physics Communications PHYSICS, MULTIDISCIPLINARY-
CiteScore
2.60
自引率
0.00%
发文量
114
审稿时长
10 weeks
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