{"title":"热库热化过程中熵产生的直观证明","authors":"Ramandeep S. Johal","doi":"arxiv-2409.03581","DOIUrl":null,"url":null,"abstract":"In this note, the equilibrium curve of a thermodynamic system is used to\ndepict entropy production in the process of thermalization with a reservoir.\nFor the given initial and final equilibrium states of the system, the entropy\nproduction is reduced when work is also extracted during thermalization. The\ncase of maximum work extraction corresponds to a reversible process. For less\nthan optimal work extraction, the lost available work is shown to be directly\nproportional to the entropy produced.","PeriodicalId":501482,"journal":{"name":"arXiv - PHYS - Classical Physics","volume":"62 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A visual proof of entropy production during thermalization with a heat reservoir\",\"authors\":\"Ramandeep S. Johal\",\"doi\":\"arxiv-2409.03581\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this note, the equilibrium curve of a thermodynamic system is used to\\ndepict entropy production in the process of thermalization with a reservoir.\\nFor the given initial and final equilibrium states of the system, the entropy\\nproduction is reduced when work is also extracted during thermalization. The\\ncase of maximum work extraction corresponds to a reversible process. For less\\nthan optimal work extraction, the lost available work is shown to be directly\\nproportional to the entropy produced.\",\"PeriodicalId\":501482,\"journal\":{\"name\":\"arXiv - PHYS - Classical Physics\",\"volume\":\"62 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Classical Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.03581\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Classical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03581","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A visual proof of entropy production during thermalization with a heat reservoir
In this note, the equilibrium curve of a thermodynamic system is used to
depict entropy production in the process of thermalization with a reservoir.
For the given initial and final equilibrium states of the system, the entropy
production is reduced when work is also extracted during thermalization. The
case of maximum work extraction corresponds to a reversible process. For less
than optimal work extraction, the lost available work is shown to be directly
proportional to the entropy produced.