Author_Institution :
IIT Res. Inst., Annapolis, MD, USA
Abstract :
Summary form only given. While in the case of a smooth perfectly-conducting scatterer, transition-region electromagnetic fields can readily be obtained from tabulated values of familiar integrals, such tabulated values are not, in general, available in the case of an impedance or coated scatterer. A comparison between the solution of Hussar and Albus (1991) with the more familiar UTD shadow-region solution of Pathak, Burnside and Marhefka (1980) for a conducting scatterer, and for impedance and coated cylinders proposed by Kim and Wang (1989) suggests the introduction of a novel function p*(/spl xi/,q,u) with the property that p*(/spl xi/,q) (a Pekeris function) is rapidly approached as u increases past unity. Extension of this function into the lit region is easily achieved, and, for a value of u not greatly in excess of unity, p*(/spl xi/,q,u) provides an accurate approximation for p*(/spl xi/,q) for /spl xi/ as small as -1.5 and at a modest cost in computational terms. A complete solution is obtained by employing heuristically derived criteria to effect a transition between a UTD solution employing p/sup /spl xi/,q,u/ and geometrical optics.
Keywords :
conductors (electric); electric impedance; electromagnetic fields; electromagnetic wave scattering; function approximation; geometrical optics; geometrical theory of diffraction; series (mathematics); Pekeris function; UTD shadow-region solution; UTD solution; approximation; coated cylinders; coated scatterer; conducting scatterer; function; geometrical optics; impedance cylinders; impedance scatterer; lit-region fields; residue-series computation; smooth perfectly-conducting scatterer; transition-region electromagnetic fields; Abstracts; Antennas and propagation; Computational efficiency; Cost function; Electromagnetic fields; Electromagnetic scattering; Geometrical optics; Impedance; Optical scattering;