{"title":"分布温度系统中的热爆炸、临界和临界消失IV.严格界限及其实际意义","authors":"G. Wake, T. Boddington, P. Gray","doi":"10.1098/rspa.1989.0107","DOIUrl":null,"url":null,"abstract":"In thermal explosion theory it is usually impossible analytically, and sometimes a substantial task numerically, to locate the ambient temperature at which transition from discontinuous to continuous behaviour occurs. It is possible to establish analytically a lower bound that is remarkably close to the numerically computed value.","PeriodicalId":20605,"journal":{"name":"Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences","volume":"26 1","pages":"285 - 289"},"PeriodicalIF":0.0000,"publicationDate":"1989-10-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":"{\"title\":\"Thermal explosions, criticality and the disappearance of criticality in systems with distributed temperatures IV. Rigorous bounds and their practical relevance\",\"authors\":\"G. Wake, T. Boddington, P. Gray\",\"doi\":\"10.1098/rspa.1989.0107\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In thermal explosion theory it is usually impossible analytically, and sometimes a substantial task numerically, to locate the ambient temperature at which transition from discontinuous to continuous behaviour occurs. It is possible to establish analytically a lower bound that is remarkably close to the numerically computed value.\",\"PeriodicalId\":20605,\"journal\":{\"name\":\"Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences\",\"volume\":\"26 1\",\"pages\":\"285 - 289\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1989-10-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"5\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1098/rspa.1989.0107\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1098/rspa.1989.0107","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Thermal explosions, criticality and the disappearance of criticality in systems with distributed temperatures IV. Rigorous bounds and their practical relevance
In thermal explosion theory it is usually impossible analytically, and sometimes a substantial task numerically, to locate the ambient temperature at which transition from discontinuous to continuous behaviour occurs. It is possible to establish analytically a lower bound that is remarkably close to the numerically computed value.