Thermodynamics II

Mandeep Dalal
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Abstract

CHAPTER 6 Thermodynamics – II  Clausius-Clapeyron Equation The Clausius-Clapeyron equation was initially proposed by a German physics Rudolf Clausius in 1834 and then further developed by French physicist Benoît Clapeyron in 1850. This equation is extremely useful in characterizing a discontinuous phase transition between two phases of a single constituent.  Derivation of Clausius-Clapeyron Equation In order to derive the Clausius-Clapeyron equation, consider a system at equilibrium i.e. the free energy change for the ongoing process is zero (ΔG = 0). However, we know from the principles of thermodynamics that the variation of free energy with temperature and pressure can be formulated by the following differential equation.
Clausius-Clapeyron方程Clausius-Clapeyron方程最初是由德国物理学家Rudolf Clausius在1834年提出的,然后由法国物理学家beno t Clapeyron在1850年进一步发展。这个方程在描述单一组分的两相之间的不连续相变时非常有用。为了推导Clausius-Clapeyron方程,考虑一个处于平衡状态的系统,即正在进行的过程的自由能变化为零(ΔG = 0)。然而,我们从热力学原理知道,自由能随温度和压力的变化可以用以下微分方程表示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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