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TM scattering by a narrow conducting strip located at the interface between two semi-infinite half-spaces

机译:通过位于两个半无限半空间之间的界面的窄导电带进行TM散射

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The far-zone field scattered by a narrow conducting strip located at the interface between two semi-infinite dielectric half-spaces is determined analytically. The permeabilities of the two half-spaces are equal, and the excitation is restricted to be transverse magnetic to, and invariant along, the axis of the strip. The solution of the approximate integral equation for the current on the strip is constructed as an infinite series of Chebyshev polynomials of the first kind weighted by a function exhibiting the proper edge behavior at the strip edges. Two methods, one depending upon integrals of the known excitation and the other upon its derivatives, are presented. The far-zone scattered field is represented as series involving Bessel functions and coefficients determined from the excitation. In the special case of incident plane wave illumination, explicit expressions for the series coefficients are given.
机译:解析地确定位于两个半无限电介质半空间之间的界面处的狭窄导电带所散射的远区场。两个半空间的磁导率是相等的,并且激励被限制为横向于条带的轴并且沿着条带的轴是不变的。带材上电流的近似积分方程的解构造为第一类Chebyshev多项式的无穷级数,该多项式通过函数在带材边缘处表现出适当的边缘行为进行加权。提出了两种方法,一种取决于已知激励的积分,另一种取决于其导数。远区散射场表示为一系列,涉及贝塞尔函数和由激发确定的系数。在入射平面波照明的特殊情况下,给出了级数系数的明确表达式。

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