General Solution of EM Wave Propagation in Anisotropic Media

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dc.contributor.authorLee J.ko
dc.contributor.authorLee S.ko
dc.date.accessioned2013-03-08T17:55:36Z-
dc.date.available2013-03-08T17:55:36Z-
dc.date.created2012-02-06-
dc.date.created2012-02-06-
dc.date.issued2010-
dc.identifier.citationJOURNAL OF THE KOREAN PHYSICAL SOCIETY, v.57, no.1, pp.55 - 60-
dc.identifier.issn0374-4884-
dc.identifier.urihttp://hdl.handle.net/10203/93817-
dc.description.abstractWhen anisotropy is involved, the wave equation becomes simultaneous partial differential equations that are not easily solved. Moreover, when the anisotropy occurs clue to both permittivity and permeability, these equations are insolvable without a numerical or an approximate method. The problem is essentially due to the fact neither epsilon nor mu can be extracted from the curl term, when they are in it. The turns del x E (or H) and del x epsilon E (or mu H) are practically independent variables, and E and H are coupled to each other. However, if Maxwell's equations are manipulated in a different way, new wave equations are obtained. The obtained equations can be applied in anisotropic, as well as isotropic, cases. In addition, E and H are decoupled in the new equations, so the equations can be solved at by using tensor Green's functions.-
dc.languageEnglish-
dc.publisherKOREAN PHYSICAL SOC-
dc.subjectGREENS-FUNCTIONS-
dc.titleGeneral Solution of EM Wave Propagation in Anisotropic Media-
dc.typeArticle-
dc.identifier.wosid000280009100010-
dc.identifier.scopusid2-s2.0-77956209032-
dc.type.rimsART-
dc.citation.volume57-
dc.citation.issue1-
dc.citation.beginningpage55-
dc.citation.endingpage60-
dc.citation.publicationnameJOURNAL OF THE KOREAN PHYSICAL SOCIETY-
dc.identifier.doi10.3938/jkps.57.55-
dc.contributor.localauthorLee J.-
dc.contributor.nonIdAuthorLee S.-
dc.type.journalArticleArticle-
dc.subject.keywordAuthorAnisotropy-
dc.subject.keywordAuthorDyadic Green&apos-
dc.subject.keywordAuthors functions-
dc.subject.keywordPlusGREENS-FUNCTIONS-
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