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Singular Integral Equations in the Problem of Diffraction of an Electromagnetic Plane Wave by a Perfectly Conducting Finite Hollow Cylinder

机译:理想导体空心圆柱在电磁平面波衍射问题中的奇异积分方程

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The problem of diffraction of a plane electromagnetic wave by a finite metallic cylinder (linear electric vibrator) is one of the key problems in the theory of receiving antennas, and it is most difficult to determine the electric-current distribution over the cylinder. The method of calculating the electric-current distribution in a system of thin linear vibrators excited by a plane wave was developed in [1 ]. In that paper, the diffraction problem (in the thin-vibrator approximation) was reduced to an ill-posed problem [2] that was represented by a set of Fredholm integral equations of the first kind with logarithmic singularities in their kernels and was solved by the self-regularization method [3], Symmetric vibrations (independent of the azimuth coordinate) of a perfectly conducting finite hollow cylinder were considered in [4]. However, Tikhonov and Dmitriev [3] stated that the solution obtained in [4] is incorrect. On the other hand, the two-dimensional problem of diffraction of a plane electromagnetic wave by an infinite perfectly conducting circular cylinder was solved long ago in [5] under the assumption of the absence of field variations along the axial cylindrical coordinate. In [6-8], the theory of singular equations was applied to develop the theory of a thin electric vibrator in the approximation of a perfectly conducting finite hollow circular cylinder by ignoring the azimuthal electric-current component. In the present study, the problem of the diffraction of a plane electromagnetic wave by a perfectly conducting finite hollow circular cylinder is analyzed with allowance for the azimuthal component of the electric current arising on the cylinder surface.
机译:有限金属圆柱体(线性电振子)对平面电磁波的衍射问题是接收天线理论中的关键问题之一,最难确定圆柱体上的电流分布。在[1]中发展了一种计算由平面波激发的薄线性振动器系统中电流分布的方法。在那篇论文中,将衍射问题(在薄振动器近似中)简化为不适定问题[2],该问题由一组第一类Fredholm积分方程表示,它们的核中具有对数奇异性,并通过自调整方法[3],在[4]中考虑了一个完美传导的有限空心圆柱体的对称振动(独立于方位角坐标)。但是,Tikhonov和Dmitriev [3]指出,[4]中获得的解决方案是不正确的。另一方面,早在[5]中就已经解决了无限电磁波传导平面电磁波的二维问题,这种假设是在沿轴向圆柱坐标不存在磁场变化的前提下进行的。在[6-8]中,奇异方程的理论被用来发展薄电振子的理论,它通过忽略方位电流分量来逼近完美传导的有限空心圆柱体。在本研究中,分析了一个完美传导的有限空心圆柱体对平面电磁波的衍射问题,并考虑了在圆柱体表面上产生的电流的方位角分量。

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