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dc.contributor.authorMorgan, M.A.
dc.contributor.authorChen, C.H.
dc.contributor.authorHill, S.C.
dc.contributor.authorBarber, P.W.
dc.date.accessioned2015-10-14T21:51:13Z
dc.date.available2015-10-14T21:51:13Z
dc.date.issued1984-10
dc.identifier.citationWave Motion, Vol. 6 1984, pp. 91-103en_US
dc.identifier.urihttp://hdl.handle.net/10945/47013
dc.descriptionThis paper was presented at the Workshop/ Symposium on Research Techniques in Wave Propagation and Scattering, organized by V.K. Varadan and V.V. Varadan, October 18-2 1. 1982. The Ohio State University. Columbus. Ohio.en_US
dc.description.abstractA new formulation is described which combines the most robust attributes of the volume finite element and surface integral equation approaches to electromagnetic boundary value solutions. The result is a numerical technique which may be applied to scatte ring problems involving configurations having metallic surfaces and inhomogeneous penetrable mate rial situated in open spatial regions. This is accomplished by way of coupling internal region finite element modal field solutions to equivalent currents on the surrounding boundary surface through an appropriate surface integral equation. The method is demonstrated for the special case of scattering by axisymmetric inhomogeneous penetrable objects. Example numerical calculations are presented for validation of the procedure and potential problem areas are discussed.en_US
dc.rightsThis publication is a work of the U.S. Government as defined in Title 17, United States Code, Section 101. As such, it is in the public domain, and under the provisions of Title 17, United States Code, Section 105, may not be copyrighted.en_US
dc.titleFinite Element-Boundary Integral Formulation for Electromagnetic Scatteringen_US
dc.typeArticleen_US
dc.contributor.departmentElectrical Engineeringen_US
dc.description.funderThis work was partially supported by funding from the U.S. Army Research Office and employed the facilities of the University of Utah and the Naval Postgraduate School.en_US


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