{"title":"水撞击时地表压力的预测","authors":"A. Wardlaw, P. M. Aronson","doi":"10.2514/3.63076","DOIUrl":null,"url":null,"abstract":"Nomenclature CD(X = drag coefficient assuming a constant entry velocity CP = pressure coefficient Cw = wetting factor, h/h' en = unit vector normal to the body surface h = model depth below effective planar surface h' — model depth below original surface A/z = increment in depth below the effective planar surface in successive steps t = time t*m — VEt/D, where t is time measured from initial model impact t* = VEt/d, where t is the length of time the element centroid has been submerged VE = entry velocity Bc = cone half angle 6 = entry angle (measured from the horizontal) = velocity potential","PeriodicalId":157493,"journal":{"name":"Journal of Hydronautics","volume":"34 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1977-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Prediction of Surface Pressures during Water Impact\",\"authors\":\"A. Wardlaw, P. M. Aronson\",\"doi\":\"10.2514/3.63076\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Nomenclature CD(X = drag coefficient assuming a constant entry velocity CP = pressure coefficient Cw = wetting factor, h/h' en = unit vector normal to the body surface h = model depth below effective planar surface h' — model depth below original surface A/z = increment in depth below the effective planar surface in successive steps t = time t*m — VEt/D, where t is time measured from initial model impact t* = VEt/d, where t is the length of time the element centroid has been submerged VE = entry velocity Bc = cone half angle 6 = entry angle (measured from the horizontal) = velocity potential\",\"PeriodicalId\":157493,\"journal\":{\"name\":\"Journal of Hydronautics\",\"volume\":\"34 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1977-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Hydronautics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.2514/3.63076\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Hydronautics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2514/3.63076","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Prediction of Surface Pressures during Water Impact
Nomenclature CD(X = drag coefficient assuming a constant entry velocity CP = pressure coefficient Cw = wetting factor, h/h' en = unit vector normal to the body surface h = model depth below effective planar surface h' — model depth below original surface A/z = increment in depth below the effective planar surface in successive steps t = time t*m — VEt/D, where t is time measured from initial model impact t* = VEt/d, where t is the length of time the element centroid has been submerged VE = entry velocity Bc = cone half angle 6 = entry angle (measured from the horizontal) = velocity potential