Electromagnetic Diffraction and Propagation Problems |
Contents
New methods in diffraction theory Fock 1948 | 3 |
The distribution of currents induced by a plane wave on the surface of a con | 10 |
Diffraction of a plane electromagnetic wave by a perfectly conducting parabo | 66 |
Copyright | |
14 other sections not shown
Common terms and phrases
Airy functions amplitude asymptotic expressions attenuation factor body boundary conditions C₁ calculated Chapter coefficient complex considered constant contour coordinates corresponding curvature curve denote derivatives dielectric constant differential equation diffraction dipole earth earth's surface eixt electromagnetic equal expressed in terms field components finite Fock Fresnel formulae geometrical optics H₁ H₂ Hankel function Hertz function illuminated region incident wave infinity integral integrand introduce inversion layer M-curve M-profile magnetic Maxwell equations obtain paraboloid parameter penumbra penumbra region phase plane wave problem quantity radiowave propagation radius real axis reflected wave reflection formula refractive index relation residue roots S₁ satisfies Section shadow sinē singularity solution t₁ tion U₂ V. A. Fock V₁ valid variable vector W₁ w₁(t W₂ waveguide wavelength y₁ ди ду მა