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Diffraction by a planar junction between a perfectly conducting half plane and a resistive sheet illuminated by a dipole close to its edge

机译:完美导电的半平面与电阻片之间的平面接合处产生的衍射,该电阻片被靠近其边缘的偶极子照亮

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The problem of evaluating the field diffracted in the far zone by a junction between a perfectly electric conducting (PEC) half-plane and a resistive sheet, illuminated by an arbitrarily oriented dipole, is considered in this paper. The field diffracted by a PEC-resistive sheet junction for plane wave incidence is expressed in terms of an integral along the Sommerfeld contour of a suitable spectral function, which is determined by applying the bisection technique and the Maliuzhinets' (1958) method This integral representation is well suited to analysing the diffracted field far from the edge of the junction, when the saddle point technique is applicable. To describe the field in the vicinity of the junction, the solution has to be expressed as a series of Bessel functions and their derivatives. Finally, a representation of the field diffracted in the far zone by the junction illuminated by an arbitrarily oriented dipole is obtained by reciprocity.
机译:本文考虑了评估由理想导电偶极子照亮的完美导电(PEC)半平面和电阻片之间的结点在远区中衍射的场的问题。由PEC电阻片交界处的平面波入射所衍射的场表示为沿适当光谱函数的Sommerfeld轮廓的积分,该积分是通过应用对分技术和Maliuzhinets(1958)方法确定的。当采用鞍点技术时,它非常适合分析远离结点边缘的衍射场。为了描述交界处附近的场,必须将解决方案表示为一系列贝塞尔函数及其导数。最后,通过互易性获得由任意取向的偶极子照射的结在远区中衍射的场的表示。

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