AN H‐FIELD SOLUTION FOR ELECTROMAGNETIC SCATTERING BY A CONDUCTING BODY OF REVOLUTION

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 H‐FIELD SOLUTION FOR ELECTROMAGNETIC SCATTERING BY A CONDUCTING BODY OF REVOLUTION", COMPEL - The international journal for computation and mathematics in electrical and electronic engineering, Vol. 1 No. 3, pp. 137-163. https://doi.org/10.1108/eb009969