论文标题
非克劳西乌斯传热:非平稳朗格文方程的方法
Non-Clausius heat transfer: The method of the nonstationary Langevin equation
论文作者
论文摘要
与热力学第二定律的其他制剂相比,克劳西乌斯的陈述表明,热量不会自发地流向冷热,这涉及非平衡状态的系统,在这方面,系统更雄心勃勃,但更含糊。当Clausius声明以其简单的形式不存在时,我们讨论了两种情况。首先,对于厄贡系统,能量传输可能与粗粒度时间尺度上的陈述一致,但在时间间隔中的定向比热时间短。特别是,当最初更冷的系统与热浴接触时,前者的内部能量长期会随着时间的推移而增加,但不是单调的。其次,由于局部振动模式的形成,传热可能不尊重非恋爱系统中任何时间尺度的Clausius声明。我们用熟悉的同位素原子附着在半无限谐波原子链上的同位素原子的模型来说明这两种情况。从技术上讲,讨论是基于同位素的langevin方程,当同位素和链条最初以不相关的规范状态制备时,使用初始条件,这是在最初固定和随后释放的同位素和链之间的边界原子之间的约束。在这种情况下,Langevin方程中的噪声是非平稳的,并且波动散文关系具有非标准形式。
Compared to other formulations of the second law of thermodynamics, the Clausius statement that heat does not spontaneously flow from cold to hot concerns a system in non-equilibrium states, and in that respect is more ambitious but also more ambiguous. We discuss two scenarios when the Clausius statement in its plain form does not hold. First, for ergodic systems, the energy transfer may be consistent with the statement on a coarse-grained time scale, but be anomalously directed during time intervals shorter than the thermalization time. In particular, when an initially colder system is brought in contact to a hotter bath, the internal energy of the former increases with time in a long run but not monotonically. Second, the heat transfer may not respect the Clausius statement on any time-scale in non-ergodic systems due to the formation of localized vibrational modes. We illustrate the two scenarios with a familiar model of an isotope atom attached to a semi-infinite harmonic atomic chain. Technically, the discussion is based on a Langevin equation for the isotope, using the initial condition when the isotope and chain are initially prepared in uncorrelated canonical states under the constraint that the boundary atom between the isotope and chain is initially fixed and later released. In such setting, the noise in the Langevin equation is non-stationary, and the fluctuation-dissipation relation has a non-standard form.