{"title":"紊流爆发现象的模型:紊流普朗特数的预测","authors":"L.C. Thomas, M.B. Ibrahim","doi":"10.1016/0094-4548(81)90024-2","DOIUrl":null,"url":null,"abstract":"<div><p>A preliminary analysis is developed coupling surface-renewal and classical ideas which accounts for the fundamental difference between the transport process within the wall region and the turbulent core. It shows that Pr<sub>t</sub> increases with Pr very near the wall, but decreases with Pr at greater distances from the wall.</p></div>","PeriodicalId":100875,"journal":{"name":"Letters in Heat and Mass Transfer","volume":"8 5","pages":"Pages 357-369"},"PeriodicalIF":0.0000,"publicationDate":"1981-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0094-4548(81)90024-2","citationCount":"1","resultStr":"{\"title\":\"A model of the turbulent burst phenomenon: Predictions for turbulent prandtl number\",\"authors\":\"L.C. Thomas, M.B. Ibrahim\",\"doi\":\"10.1016/0094-4548(81)90024-2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>A preliminary analysis is developed coupling surface-renewal and classical ideas which accounts for the fundamental difference between the transport process within the wall region and the turbulent core. It shows that Pr<sub>t</sub> increases with Pr very near the wall, but decreases with Pr at greater distances from the wall.</p></div>\",\"PeriodicalId\":100875,\"journal\":{\"name\":\"Letters in Heat and Mass Transfer\",\"volume\":\"8 5\",\"pages\":\"Pages 357-369\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1981-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0094-4548(81)90024-2\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Letters in Heat and Mass Transfer\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0094454881900242\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Letters in Heat and Mass Transfer","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0094454881900242","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A model of the turbulent burst phenomenon: Predictions for turbulent prandtl number
A preliminary analysis is developed coupling surface-renewal and classical ideas which accounts for the fundamental difference between the transport process within the wall region and the turbulent core. It shows that Prt increases with Pr very near the wall, but decreases with Pr at greater distances from the wall.