Electromagnetic Wave TheoryThis is a first year graduate text on electromagnetic field theory emphasizing mathematical approaches, problem solving and physical interpretation. Examples deal with guidance, propagation, radiation and scattering of electromagnetic waves, metallic and dielectric wave guides, resonators, antennas and radiating structures, Cerenkov radiation, moving media, plasmas, crystals, integrated optics, lasers and fibers, remote sensing, geophysical probing, dipole antennas and stratified media. |
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Page 389
Jin Au Kong. This is the most popular formula for diffraction used in physical optics . Clearly , when other components of the electric field become important , the formula breaks down . Thus in the case of diffraction of a linearly ...
Jin Au Kong. This is the most popular formula for diffraction used in physical optics . Clearly , when other components of the electric field become important , the formula breaks down . Thus in the case of diffraction of a linearly ...
Page 391
... diffraction patterns with Huygens ' wavelet concept , Fresnel found that the amplitude factor ik ( î · Â + ñ · Ê ̧ ) had to be postulated in order to get accurate results . It was ... Diffraction 391 4 Fresnel and Fraunhofer Diffraction.
... diffraction patterns with Huygens ' wavelet concept , Fresnel found that the amplitude factor ik ( î · Â + ñ · Ê ̧ ) had to be postulated in order to get accurate results . It was ... Diffraction 391 4 Fresnel and Fraunhofer Diffraction.
Page 478
... diffraction coefficient D ( 3 , 3 ) = -BB.D ̧ – Îo ¿ Dh where Bŝix și and B. = - ŝ × as shown in Figure P5.4.8b . The first term corresponds to a TM wave and the second term to a TE wave . If the field points are not close to the shadow ...
... diffraction coefficient D ( 3 , 3 ) = -BB.D ̧ – Îo ¿ Dh where Bŝix și and B. = - ŝ × as shown in Figure P5.4.8b . The first term corresponds to a TM wave and the second term to a TE wave . If the field points are not close to the shadow ...
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Common terms and phrases
amplitudes angle antenna aperture array axis bianisotropic boundary conditions cavity complex conductor Consider constitutive relations coordinate cos² current sheet cylindrical defined denote density derived determined dielectric dipole dispersion relation dyadic Green's function E₁ E₂ eikr electric field electromagnetic waves field components field vectors formula frequency Green's function guidance condition guided waves H₂ Hankel function impedance incident wave integral isotropic medium k₁ kız linearly polarized Lorentz Lorentz transformation magnetic field matrix Maxwell's equations modes obtain optical permittivity perpendicular phase front plane wave Poynting's Poynting's theorem Problem radiation radius reflection coefficient region resonant saddle point scalar scattered Show shown in Figure sin² solution spherical tensor theorem tion TM waves transformation transmission uniaxial velocity wave equation wave propagating wave vector waveguide wavenumber zero