2011
DOI: 10.1364/josaa.28.002510
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Electromagnetic scattering from cylindrical objects above a conductive surface using a hybrid finite-element–surface integral equation method

Abstract: This work presents a novel finite-element solution to the problem of scattering from a finite and an infinite array of cylindrical objects with arbitrary shapes and materials over perfectly conducting ground planes. The formulation is based on using the surface integral equation with Green's function of the first or second kind as a boundary constraint. The solution region is divided into interior regions containing the cylindrical objects and the region exterior to all the objects. The finite-element formulat… Show more

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Cited by 12 publications
(9 citation statements)
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“…3(b) gives the field distribution along the boundary. With the results compared with those of the traditional FEM-BIM [20], it can be seen that the results of the multiregion FEM-BIM show good agreement with those of the traditional FEM-BIM. The relative error of the multiregion Fig.…”
Section: A Validation Of the Hybrid Methodsmentioning
confidence: 83%
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“…3(b) gives the field distribution along the boundary. With the results compared with those of the traditional FEM-BIM [20], it can be seen that the results of the multiregion FEM-BIM show good agreement with those of the traditional FEM-BIM. The relative error of the multiregion Fig.…”
Section: A Validation Of the Hybrid Methodsmentioning
confidence: 83%
“…In (20), the interactions from subordinate regions S 1l and S 1r are taken into account as a second incident source. As the secondary incident wave, the total incident field impinged in the dominant regions can be received by substituting (18) and (19) into (21).…”
Section: Theoretical Formulationmentioning
confidence: 99%
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“…(1) with a G , integrating over a Ω , and invoking the second Green's scalar theorem (6) where b k is the wave number of b Ω . The Green's function…”
Section: Theoretical Analysismentioning
confidence: 99%
“…However, the approximate absorbing boundaries often need to be set far enough away from the model surface to keep their precision, and are often invalid to some particular problems. To improve the precision and the versatile of FEM, the boundary integral equation [5,6] is introduce as the artificial truncated boundary. The earlier work based on FEM always used an artificial boundary to enclose the whole scattering model, which consumes largely of computational time and memory.…”
Section: Introductionmentioning
confidence: 99%