首页> 外文会议>Symposium on Antenna Technology and Applied Electromagnetics >Scattering of electromagnetic plane wave by conducting convex plate
【24h】

Scattering of electromagnetic plane wave by conducting convex plate

机译:导电凸板对电磁平面波的散射

获取原文

摘要

Scattering problems of electromagnetic plane wave by conducting plate of arbitrary shape are studied nsing physical theory of diffraction (PTD). PTD solution consists of physical optic (PO) solution and its correction due to nonuniform edge current. Usually PO solution is given by surface integral with integrand which includes the amplitude multiplied by linear phase term. When this amplitude is constant, the PO radiation integral can be transformed into contour integral using Stokes's theorem which has been developed by Gordon [1]. This contour integral may be performed analytically for special cases of triangular, rectangular, circular and elliptic conducting disks, but we have to rely on numerical integration for general disks. For convex plate, an asymptotic solution for the contour integral is derived using the stationary phase method of integration. There are two stationary points in this integrand which correspond to diffraction points and the solution has a simple physical interpretation that diffracted field comes from these two diffraction points [2]. The amplitudes of the diffracted rays are found to be proportional to the square root of the radius of curvature at the diffraction point. Using the similarity of the derived asymptotic solution with that of circular disk which is obtained by applying asymptotic expansion to the Airy pattern, we deduce the caustic corrected solution [3]. The validity of the expression is verified numerically for special shaped convex plate. Next, the expression for the non-unifourm edge correction is derived by applying the equivalent current method (ECM) to Ufimtsev's edge current [4],[5]. For convex plate, the asymptotic expression is derived usiug the stationary phase method of integration. For special case of circular disk the PTD solution agrees completely with that obtained by Ufimtsev [3].
机译:运用衍射的物理理论(PTD)研究了任意形状的导电板对电磁平面波的散射问题。 PTD解决方案包括物理光学(PO)解决方案,以及由于边缘电流不均匀而对其进行的校正。通常,PO解是通过表面与积分的积分给出的,积分包括振幅乘以线性相位项。当该振幅恒定时,可以使用由戈登[1]开发的斯托克斯定理将PO辐射积分转换为轮廓积分。对于三角形,矩形,圆形和椭圆形导电盘的特殊情况,可以通过分析来执行此轮廓积分,但是对于一般的盘,我们必须依靠数值积分。对于凸板,使用平稳相积分方法导出轮廓积分的渐近解。该积分物中有两个固定点,分别对应于衍射点,并且该溶液具有简单的物理解释,即衍射场来自这两个衍射点[2]。发现衍射射线的振幅与在衍射点处的曲率半径的平方根成比例。利用导出的渐近解与通过对Airy模式应用渐近展开获得的圆盘的相似性,我们推导出了苛刻的校正解[3]。对于特殊形状的凸板,通过数值验证了该表达式的有效性。接下来,通过将等效电流方法(ECM)应用于Ufimtsev的边缘电流[4],[5],可以得出非unifourm边缘校正的表达式。对于凸板,采用平稳相积分方法导出了渐近表达式。对于圆盘的特殊情况,PTD解决方案与Ufimtsev [3]完全一致。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号