{"title":"放射气象学研究(第三部分)一种新的湍流参数","authors":"B. Bean, E. Dutton, J. Lane, W. B. Sweezy","doi":"10.6028/JRES.067D.065","DOIUrl":null,"url":null,"abstract":"The co ncep t of t he rm al stabili ty is utili zed to d eri ve expressions for t he radio refractivity of an a ir p a rcel und ergoing adiabatic compression or expansion. These expression s a re of exponen t ia l form witll scale heights of 12.5 km for t he dry adiabatic process and 7.0 km for the wet adiabatic process . The adiabatic curves for N are determined solely from conditions at the earth's surface. A new tu rb ulence p arameter, II , is d eri ved as t he di ffe rence of the en vironmen tal r efractive index struc t ure a nd t he adiabatic curves for a n a ir parcel li fted from t he s urface to 3 km. This parameter yields co rrelations wi t h three hou rl y median fi eld strength data t hat a rc not statistically differen t f rolTI those obtain ed with the much simpler para meter , toN. The co rrelations obtained wi th the eq ui valen t g radient are not statistically differen t from zero.","PeriodicalId":398550,"journal":{"name":"Journal of Research of the National Bureau of Standards, Section D: Radio Propagation","volume":"29 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1963-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Radiometeorological Study, Part III. A New Turbulence Parameter\",\"authors\":\"B. Bean, E. Dutton, J. Lane, W. B. Sweezy\",\"doi\":\"10.6028/JRES.067D.065\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The co ncep t of t he rm al stabili ty is utili zed to d eri ve expressions for t he radio refractivity of an a ir p a rcel und ergoing adiabatic compression or expansion. These expression s a re of exponen t ia l form witll scale heights of 12.5 km for t he dry adiabatic process and 7.0 km for the wet adiabatic process . The adiabatic curves for N are determined solely from conditions at the earth's surface. A new tu rb ulence p arameter, II , is d eri ved as t he di ffe rence of the en vironmen tal r efractive index struc t ure a nd t he adiabatic curves for a n a ir parcel li fted from t he s urface to 3 km. This parameter yields co rrelations wi t h three hou rl y median fi eld strength data t hat a rc not statistically differen t f rolTI those obtain ed with the much simpler para meter , toN. The co rrelations obtained wi th the eq ui valen t g radient are not statistically differen t from zero.\",\"PeriodicalId\":398550,\"journal\":{\"name\":\"Journal of Research of the National Bureau of Standards, Section D: Radio Propagation\",\"volume\":\"29 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1963-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Research of the National Bureau of Standards, Section D: Radio Propagation\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.6028/JRES.067D.065\",\"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 Research of the National Bureau of Standards, Section D: Radio Propagation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.6028/JRES.067D.065","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A Radiometeorological Study, Part III. A New Turbulence Parameter
The co ncep t of t he rm al stabili ty is utili zed to d eri ve expressions for t he radio refractivity of an a ir p a rcel und ergoing adiabatic compression or expansion. These expression s a re of exponen t ia l form witll scale heights of 12.5 km for t he dry adiabatic process and 7.0 km for the wet adiabatic process . The adiabatic curves for N are determined solely from conditions at the earth's surface. A new tu rb ulence p arameter, II , is d eri ved as t he di ffe rence of the en vironmen tal r efractive index struc t ure a nd t he adiabatic curves for a n a ir parcel li fted from t he s urface to 3 km. This parameter yields co rrelations wi t h three hou rl y median fi eld strength data t hat a rc not statistically differen t f rolTI those obtain ed with the much simpler para meter , toN. The co rrelations obtained wi th the eq ui valen t g radient are not statistically differen t from zero.