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Fundamentals of Physics I最新文献

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Waves I 波我
Fundamentals of Physics I Pub Date : 1991-11-01 DOI: 10.2307/j.ctvmd85m7.22
Jeff Duntemann
{"title":"Waves I","authors":"Jeff Duntemann","doi":"10.2307/j.ctvmd85m7.22","DOIUrl":"https://doi.org/10.2307/j.ctvmd85m7.22","url":null,"abstract":"Page 1 of 3 http://edugen.wileyplus.com/edugen/courses/crs7165/halliday9781118230...Xk5NzgxMTE4MjMwNzI1YzE2LXNlYy0wMDQ0Lnhmb3Jt.enc?course=crs7165&id=ref Print this page Review & Summary Transverse and Longitudinal Waves Mechanical waves can exist only in material media and are governed by Newton's laws. Transverse mechanical waves, like those on a stretched string, are waves in which the particles of the medium oscillate perpendicular to the wave's direction of travel. Waves in which the particles of the medium oscillate parallel to the wave's direction of travel are longitudinal waves.","PeriodicalId":255617,"journal":{"name":"Fundamentals of Physics I","volume":"99 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1991-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"121907162","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 12
Thermodynamics II
Fundamentals of Physics I Pub Date : 1900-01-01 DOI: 10.2307/j.ctvmd85m7.27
Mandeep Dalal
{"title":"Thermodynamics II","authors":"Mandeep Dalal","doi":"10.2307/j.ctvmd85m7.27","DOIUrl":"https://doi.org/10.2307/j.ctvmd85m7.27","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":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116279347","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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