{"title":"关于随机介质中波的抛物方程模型的评述","authors":"S. Mudaliar","doi":"10.23919/USNC-URSINRSM51531.2021.9336446","DOIUrl":null,"url":null,"abstract":"One of the most important contributions of V.I. Tatarskii is the introduction and development of the parabolic equation model (PEM) for waves in random media (WRM). Most of the theories for WRM are based on perturbation methods that place stringent constraints on the magnitude of refractive index fluctuations. The PEM was hence introduced as a strong fluctuation theory. An important merit of the theory is that one can obtain closed equations for moments of wave functions of any order. This model is based on the following three assumptions: (a) wave propagation is predominant in one direction (negligible backscatter), (b) the refractive index fluctuations obey Gaussian statistics, and (c) the random medium is delta correlated along the direction of propagation. In spite of the restrictions imposed by these assumptions, PEM has been quite successful in numerous applications since 1970.","PeriodicalId":180982,"journal":{"name":"2021 United States National Committee of URSI National Radio Science Meeting (USNC-URSI NRSM)","volume":"40 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-01-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Remarks on the Parabolic Equation Model for Waves in Random Media\",\"authors\":\"S. Mudaliar\",\"doi\":\"10.23919/USNC-URSINRSM51531.2021.9336446\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"One of the most important contributions of V.I. Tatarskii is the introduction and development of the parabolic equation model (PEM) for waves in random media (WRM). Most of the theories for WRM are based on perturbation methods that place stringent constraints on the magnitude of refractive index fluctuations. The PEM was hence introduced as a strong fluctuation theory. An important merit of the theory is that one can obtain closed equations for moments of wave functions of any order. This model is based on the following three assumptions: (a) wave propagation is predominant in one direction (negligible backscatter), (b) the refractive index fluctuations obey Gaussian statistics, and (c) the random medium is delta correlated along the direction of propagation. In spite of the restrictions imposed by these assumptions, PEM has been quite successful in numerous applications since 1970.\",\"PeriodicalId\":180982,\"journal\":{\"name\":\"2021 United States National Committee of URSI National Radio Science Meeting (USNC-URSI NRSM)\",\"volume\":\"40 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2021-01-04\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2021 United States National Committee of URSI National Radio Science Meeting (USNC-URSI NRSM)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.23919/USNC-URSINRSM51531.2021.9336446\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2021 United States National Committee of URSI National Radio Science Meeting (USNC-URSI NRSM)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.23919/USNC-URSINRSM51531.2021.9336446","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Remarks on the Parabolic Equation Model for Waves in Random Media
One of the most important contributions of V.I. Tatarskii is the introduction and development of the parabolic equation model (PEM) for waves in random media (WRM). Most of the theories for WRM are based on perturbation methods that place stringent constraints on the magnitude of refractive index fluctuations. The PEM was hence introduced as a strong fluctuation theory. An important merit of the theory is that one can obtain closed equations for moments of wave functions of any order. This model is based on the following three assumptions: (a) wave propagation is predominant in one direction (negligible backscatter), (b) the refractive index fluctuations obey Gaussian statistics, and (c) the random medium is delta correlated along the direction of propagation. In spite of the restrictions imposed by these assumptions, PEM has been quite successful in numerous applications since 1970.