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Acoustic scattering by an impenetrable spheroid

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dc.contributor.author Roumeliotis, JA en
dc.contributor.author Kotsis, AD en
dc.contributor.author Kolezas, G en
dc.date.accessioned 2014-03-01T01:25:52Z
dc.date.available 2014-03-01T01:25:52Z
dc.date.issued 2007 en
dc.identifier.issn 1063-7710 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/17780
dc.subject Acoustic Scattering en
dc.subject Acoustic Waves en
dc.subject Cross Section en
dc.subject Perturbation Method en
dc.subject.classification Acoustics en
dc.subject.other Boundary conditions en
dc.subject.other Numerical methods en
dc.subject.other Perturbation techniques en
dc.subject.other Wave functions en
dc.subject.other Scattered pressure fields en
dc.subject.other Shape perturbation method en
dc.subject.other Spheroidal boundary en
dc.subject.other Spheroidal wave functions en
dc.subject.other Acoustic wave scattering en
dc.title Acoustic scattering by an impenetrable spheroid en
heal.type journalArticle en
heal.identifier.primary 10.1134/S1063771007040033 en
heal.identifier.secondary http://dx.doi.org/10.1134/S1063771007040033 en
heal.language English en
heal.publicationDate 2007 en
heal.abstract The scattering of a plane acoustic wave from an impenetrable, soft or hard, prolate or oblate spheroid is considered. Two different methods are used for the evaluation. In the first, the pressure field is expressed in terms of spheroidal wave functions. In the second, a shape perturbation method, the field is expressed in terms of spherical wave functions only, while the equation of the spheroidal boundary is given in spherical coordinates. Analytical expressions are obtained for the scattered pressure field and the various scattering cross-sections, when the solution is specialized to small values of the eccentricity h = d/(2a) [Figure not available: see fulltext.], where d is the interfocal distance of the spheroid and 2a is the length of its rotation axis. In this case, exact, closed-form expressions are obtained for the expansion coefficients g (2) and g (4) in the relation S(h) = S(0)[1 + g (2) h 2 + g (4) h 4 + O(h 6)] expressing the scattered field and the scattering cross-sections. Numerical results are given for various values of the parameters. © 2007 Pleiades Publishing, Ltd. en
heal.publisher MAIK NAUKA/INTERPERIODICA/SPRINGER en
heal.journalName Acoustical Physics en
dc.identifier.doi 10.1134/S1063771007040033 en
dc.identifier.isi ISI:000248046600003 en
dc.identifier.volume 53 en
dc.identifier.issue 4 en
dc.identifier.spage 436 en
dc.identifier.epage 447 en


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