2012
DOI: 10.1134/s1064226912090094
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Application of various orthogonal coordinate frames for simulating wave scattering by a group of bodies

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Cited by 7 publications
(8 citation statements)
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“…To verify the correctness of the proposed method, we compared the dependences of the scattering dia gram g(θ, ϕ) (here, (θ, ϕ) are spherical coordinates) of a thin disk with a radius ka = 50 and a highly oblate spheroid with semiaxes ka = 50 and kc = 0.5, where To solve the problem of plane wave diffraction by an oblate spheroid, we used a version of the modified dis crete source method (MDSM) [9,10]. Figure 1 shows the angular dependences of the magnitude of the scat tering diagram for a thin disk (solid curve) and a spher oid (open dots) with the dimensions specified above.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…To verify the correctness of the proposed method, we compared the dependences of the scattering dia gram g(θ, ϕ) (here, (θ, ϕ) are spherical coordinates) of a thin disk with a radius ka = 50 and a highly oblate spheroid with semiaxes ka = 50 and kc = 0.5, where To solve the problem of plane wave diffraction by an oblate spheroid, we used a version of the modified dis crete source method (MDSM) [9,10]. Figure 1 shows the angular dependences of the magnitude of the scat tering diagram for a thin disk (solid curve) and a spher oid (open dots) with the dimensions specified above.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…OF INTEGRAL EQUATIONS We solve the formulated problem using the auxil iary current method that hereinafter is reduced to the MMDS [1][2][3][4][5][6]. To this end, we represent the wave field outside the region of the grating and inside the central elements of the grating as …”
Section: Derivation Of the Systemmentioning
confidence: 99%
“…This problem is rather complicated to be realized numerically because the geometry has no axial symmetry. The problem is solved here using the modified method of discrete sources (MMDS) [1][2][3][4][5][6]. The close problem of diffraction of a plane wave by a plane grating of impedance bodies of revolution was earlier considered in [4].…”
Section: Introductionmentioning
confidence: 99%
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“…The most simple tensors E ν and H ν are defined in cylindrical coordinates. In order to transform these tensors to the corresponding orthogonal coordinates we use the formula [15,16] …”
Section: Introductionmentioning
confidence: 99%