1970
DOI: 10.21236/ad0706111
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Electromagnetic Diffraction by a Perfectly-Conducting Plane Angular Section

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Cited by 22 publications
(20 citation statements)
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“…The canonical problem of this type is the "plane annular sector," which consists of a sector of an infinite conducting plane with its tip at the origin. The problem has been investigated by Kraus, Levine, Satterwhite, and Kouyoumjian [16][17][18] and yields an exact solution. The current density near a 90 degree corner of a conducting sector has the general form…”
Section: Extensions To 3d Problemsmentioning
confidence: 99%
See 1 more Smart Citation
“…The canonical problem of this type is the "plane annular sector," which consists of a sector of an infinite conducting plane with its tip at the origin. The problem has been investigated by Kraus, Levine, Satterwhite, and Kouyoumjian [16][17][18] and yields an exact solution. The current density near a 90 degree corner of a conducting sector has the general form…”
Section: Extensions To 3d Problemsmentioning
confidence: 99%
“…Φ ei (φ) and Φ oi (φ) are even and odd Lame functions [18], j ν (κr) is a spherical Bessel function, and primes denote derivatives. The coefficients a i and b i depend on the source.…”
Section: Extensions To 3d Problemsmentioning
confidence: 99%
“…The vertex diffracted current is then defined as (1) where is the exact current and is the well-known PO current. and are the fringe-wave contributions due to the two edges of the angular sector.…”
Section: Current Density On the Plane Angular Sectormentioning
confidence: 99%
“…An exact solution based on the separation of variables in the sphero-conal coordinate system was first developed by Satterwhite [1]. In his solution, fields and currents are expressed in terms of scalar wave functions that are the solutions of a two-parameter eigenvalue problem of two coupled spherical Lamé differential equations and spherical Bessel functions.…”
Section: Introductionmentioning
confidence: 99%
“…An even more serious impairment is encountered in applying GTD to RCS calculations, due to the fact that the leading edge contributions are restricted to lying on the pertinent diffraction cones. The canonical problem of the plane angular sector was solved by Satterwhite and Kouyoumjian [3,4], but the series expansion of the solution is hard to compute and not well-suited for a practical asymptotic evaluation. Most of the literature on this topic presents formulations based on numerical or hybrid techniques [5][6][7] or on approximate, high-frequency methods [8][9][10][11][12][13].…”
Section: Introductionmentioning
confidence: 99%