{"title":"Thermodynamics II","authors":"Mandeep Dalal","doi":"10.2307/j.ctvmd85m7.27","DOIUrl":null,"url":null,"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.","PeriodicalId":255617,"journal":{"name":"Fundamentals of Physics I","volume":"70 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Fundamentals of Physics I","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2307/j.ctvmd85m7.27","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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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.