Abstract

The analysis of the TM electromagnetic scattering from perfectly electrically conducting polygonal cross-section cylinders is successfully carried out by means of an electric field integral equation formulation in the spectral domain and the method of analytical preconditioning which leads to a matrix equation at which Fredholm’s theory can be applied. Hence, the convergence of the discretization scheme is guaranteed. Unfortunately, the matrix coefficients are improper integrals involving oscillating and, in the worst cases, slowly decaying functions. Moreover, the classical analytical asymptotic acceleration technique leads to faster decaying integrands without overcoming the most important problem of their oscillating nature. Thus, the computation time rapidly increases as higher is the accuracy required for the solution. The aim of this paper is to show a new analytical technique for the efficient evaluation of such kind of integrals even when high accuracy is required for the solution.

Highlights

  • Spectral domain formulations are suitable for the analysis of a wide class of electromagnetic problems ranging from the propagation in planar guides and waveguides or the radiation by planar antennas to the scattering from cylindrical structures or planar surfaces involving homogeneous or stratified media, just to give some examples

  • When dealing with polygonal cross-section cylindrical structures or canonical shape planar surfaces, just for examples, a well-posed matrix operator equation can be obtained by means of the method of analytical preconditioning [1]. It consists of the discretization of the integral equation by means of Galerkin’s method with a suitable set of expansion functions leading to a matrix equation at which Fredholm’s or Steinberg’s theorems can be applied [2, 3]

  • The aim of this section is to show the efficiency of the presented technique even by means of comparisons with the classical analytical asymptotic acceleration technique (CAAAT)

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Summary

Introduction

Spectral domain formulations are suitable for the analysis of a wide class of electromagnetic problems ranging from the propagation in planar guides and waveguides or the radiation by planar antennas to the scattering from cylindrical structures or planar surfaces involving homogeneous or stratified media, just to give some examples. When dealing with polygonal cross-section cylindrical structures or canonical shape planar surfaces, just for examples, a well-posed matrix operator equation can be obtained by means of the method of analytical preconditioning [1]. It consists of the discretization of the integral equation by means of Galerkin’s method with a suitable set of expansion functions leading to a matrix equation at which Fredholm’s or Steinberg’s theorems can be applied [2, 3]. Only TM solutions can be obtained; i.e., the induced current is longitudinal and the electromagnetic field is invariant along the z axis

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