A Plane Wave Scattering by a LHM Anisotropic Uniaxial-coated Conducting Sphere

Y. Geng, Lewei Li, Jian Wu
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引用次数: 0

Abstract

On the basis of spherical vector wave functions in uniaxial anisotropic left-handed materials (LHMs) and the first, second, third and fourth spherical vector wave functions in uniaxial anisotropic LHMs satisfy the same differential equation, the electromagnetic fields in uniaxial anisotropic LHMs can be expressed as an addition of the first and second spherical vector wave functions in uniaxial anisotropic LHMs. Applying the boundary conditions of electromagnetic fields in the interface between LHMs and free space, in the surface of conducting sphere, the expansion coefficients of electromagnetic field in uniaxial anisotropic LHMs and scattering field in free space can be derived, and then the radar section cross (RCS) of a plane wave scattering by a LHMs anisotropic uniaxial-coated conducting sphere. Some numerical results are given in this paper.
LHM各向异性单轴涂层导电球的平面波散射
基于单轴各向异性左手材料中的球面矢量波函数和单轴各向异性左手材料中的第一、二、三、四球面矢量波函数满足相同的微分方程,可以将单轴各向异性左手材料中的电磁场表示为单轴各向异性左手材料中第一、二球面矢量波函数的相加。利用lhm与自由空间交界面的电磁场边界条件,在导电球表面,可以推导出单轴各向异性lhm中电磁场的膨胀系数和自由空间中的散射场,进而得到lhm各向异性单轴涂层导电球散射平面波的雷达截面截面(RCS)。文中给出了一些数值结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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