{"title":"非均匀物体波散射的等效表面表示","authors":"D. Swatek, I. Ciric","doi":"10.1109/ANTEM.1998.7861778","DOIUrl":null,"url":null,"abstract":"The inhomogeneous structure of an object is accounted for by a pair of surface integral operators that provide the components of the electric and magnetic fields tangent to the object's outer surface only in terms of a single unknown density of electric current distributed on that same outer surface. This equivalent surface representation is invariant under rotation and translation, and independent of external material and illumination. The computational advantage of such a transformation is shown by a numerical example.","PeriodicalId":334204,"journal":{"name":"1998 Symposium on Antenna Technology and Applied Electromagnetics","volume":"52 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"An equivalent surface representation for wave scattering by inhomogeneous objects\",\"authors\":\"D. Swatek, I. Ciric\",\"doi\":\"10.1109/ANTEM.1998.7861778\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The inhomogeneous structure of an object is accounted for by a pair of surface integral operators that provide the components of the electric and magnetic fields tangent to the object's outer surface only in terms of a single unknown density of electric current distributed on that same outer surface. This equivalent surface representation is invariant under rotation and translation, and independent of external material and illumination. The computational advantage of such a transformation is shown by a numerical example.\",\"PeriodicalId\":334204,\"journal\":{\"name\":\"1998 Symposium on Antenna Technology and Applied Electromagnetics\",\"volume\":\"52 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1998 Symposium on Antenna Technology and Applied Electromagnetics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ANTEM.1998.7861778\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1998 Symposium on Antenna Technology and Applied Electromagnetics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ANTEM.1998.7861778","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
An equivalent surface representation for wave scattering by inhomogeneous objects
The inhomogeneous structure of an object is accounted for by a pair of surface integral operators that provide the components of the electric and magnetic fields tangent to the object's outer surface only in terms of a single unknown density of electric current distributed on that same outer surface. This equivalent surface representation is invariant under rotation and translation, and independent of external material and illumination. The computational advantage of such a transformation is shown by a numerical example.