AN H ‐FIELD SOLUTION FOR ELECTROMAGNETIC SCATTERING BY A CONDUCTING BODY OF REVOLUTION
ISSN: 0332-1649
Article publication date: 1 March 1982
Abstract
The magnetic field integral equation for electromagnetic scattering from a perfectly conducting body of revolution is solved by the method of moments. A Fourier series in ø is used. The t dependence of the expansion functions is subsectional. Pulses are used for the ø component of the unknown electric current induced on the surface S of the body of revolution. Triangles divided by the cylindrical coordinate radius are used for the t component. Here, t and ø are orthogonal coordinates on S, t being the arc length along the generating curve of S and ø the azimuthal angle.
Citation
MAUTZ, J.R. and HARRINGTON, R.F. (1982), "AN
Publisher
:MCB UP Ltd
Copyright © 1982, MCB UP Limited