{"title":"束散射的CH4-Ar势","authors":"J.R. Brooks, A.E. Grosser","doi":"10.1016/0031-8914(74)90076-7","DOIUrl":null,"url":null,"abstract":"<div><p>Lennard-Jones (<em>n</em>,6) potentials fitted to differential cross-section measurements for CH<sub>4</sub>-Ar, in conjunction with those from bulk-proeprty studies, confirm that the optimum value of the repulsive exponent <em>n</em> is 18–21.</p></div>","PeriodicalId":55605,"journal":{"name":"Physica","volume":"78 2","pages":"Pages 340-342"},"PeriodicalIF":0.0000,"publicationDate":"1974-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0031-8914(74)90076-7","citationCount":"9","resultStr":"{\"title\":\"CH4-Ar potential from beam scattering\",\"authors\":\"J.R. Brooks, A.E. Grosser\",\"doi\":\"10.1016/0031-8914(74)90076-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Lennard-Jones (<em>n</em>,6) potentials fitted to differential cross-section measurements for CH<sub>4</sub>-Ar, in conjunction with those from bulk-proeprty studies, confirm that the optimum value of the repulsive exponent <em>n</em> is 18–21.</p></div>\",\"PeriodicalId\":55605,\"journal\":{\"name\":\"Physica\",\"volume\":\"78 2\",\"pages\":\"Pages 340-342\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1974-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0031-8914(74)90076-7\",\"citationCount\":\"9\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physica\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0031891474900767\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physica","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0031891474900767","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Lennard-Jones (n,6) potentials fitted to differential cross-section measurements for CH4-Ar, in conjunction with those from bulk-proeprty studies, confirm that the optimum value of the repulsive exponent n is 18–21.
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