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Electromagnetic eigenfrequencies in a spheroidal cavity

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dc.contributor.author Kokkorakis, GC en
dc.contributor.author Roumeliotis, JA en
dc.date.accessioned 2014-03-01T01:12:51Z
dc.date.available 2014-03-01T01:12:51Z
dc.date.issued 1997 en
dc.identifier.issn 0920-5071 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/12262
dc.relation.uri http://www.scopus.com/inward/record.url?eid=2-s2.0-0030643780&partnerID=40&md5=0c06de0a3a81593db99c742856a89535 en
dc.subject.classification Engineering, Electrical & Electronic en
dc.subject.classification Physics, Applied en
dc.subject.classification Physics, Mathematical en
dc.subject.other Boundary conditions en
dc.subject.other Boundary value problems en
dc.subject.other Conductive materials en
dc.subject.other Eigenvalues and eigenfunctions en
dc.subject.other Mathematical models en
dc.subject.other Perturbation techniques en
dc.subject.other Closed form expressions en
dc.subject.other Electromagnetic eigenfrequencies en
dc.subject.other Expansion coefficients en
dc.subject.other Shape perturbation method en
dc.subject.other Spheroidal cavity en
dc.subject.other Electromagnetic field theory en
dc.title Electromagnetic eigenfrequencies in a spheroidal cavity en
heal.type journalArticle en
heal.language English en
heal.publicationDate 1997 en
heal.abstract The electromagnetic eigenfrequencies f(nsm) in a perfectly conducting spheroidal cavity are determined analytically, by a shape perturbation method. The analytical determination is possible in the case of small values of the quantity v = 1 - a(2)/b(2), (\v\ <much less than 1), where 2a and 2b are the lengths of the rotation axis and the other axis of the spheroidal cavity, respectively. In this case, exact, closed-form expressions are obtained for the expansion coefficients ((1)(gnsm)) and ((2)(gnsm)) in the resulting relation f(nsm)(v) = f(ns)(0)[1 + vg(nsm)((1)) + v(gnsm)(2)((2)) + O(v(3))]. There is no need for using any spheroidal eigenvectors in our solution. The electromagnetic field is expressed in a series of spherical eigenvectors, while the equation of the spheroidal boundary is given in terms of the spherical coordinates. Numerical results are given for the eigenfrequencies of the lower-order magnetic and electric modes. en
heal.publisher VSP BV en
heal.journalName Journal of Electromagnetic Waves and Applications en
dc.identifier.isi ISI:A1997WP95300001 en
dc.identifier.volume 11 en
dc.identifier.issue 3 en
dc.identifier.spage 279 en
dc.identifier.epage 292 en


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