Electromagnetic Wave TheoryA 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. |
From inside the book
Results 1-3 of 85
Page 262
... obtain an infinite system of linear equations of the form on where au = Σ aunon n odd ( 52 ) au , n hn * -00 sin @de ( 1 ) ( kl ) Nuju ( kl ) Joo [ Tucos ) ] [ P ( cos ) ] ( 53 ) Another system of equations governing the coefficients ...
... obtain an infinite system of linear equations of the form on where au = Σ aunon n odd ( 52 ) au , n hn * -00 sin @de ( 1 ) ( kl ) Nuju ( kl ) Joo [ Tucos ) ] [ P ( cos ) ] ( 53 ) Another system of equations governing the coefficients ...
Page 263
... obtained . First , integrating ( 49 ) from 0 to -00 we find nl Yt = Zovo ( 1 ) √6 * ~ * T - 00 de H & ( r = 1 ) ( 60 ) where the characteristic impedance Zo is given by ( 25 ) . Next , substi- tuting ( 51 ) into the above equation we ...
... obtained . First , integrating ( 49 ) from 0 to -00 we find nl Yt = Zovo ( 1 ) √6 * ~ * T - 00 de H & ( r = 1 ) ( 60 ) where the characteristic impedance Zo is given by ( 25 ) . Next , substi- tuting ( 51 ) into the above equation we ...
Page 380
... obtained for the Huygens ' prin- ciple . Making use of ( 3 ) , we obtain from ( 1 ) and ( 2 ) ίωμ + Vg ( F , F ' ) × [ î × E ( F ′ ) ] } k2 iwe . 1 × 2 VVg ( F , F ′ ) · [ ŵ × H ( F ′ ) ] ( 17 ) VVg ( F , F ′ ) · [ ñ × E ( 7 ′ ) ] k2 + ...
... obtained for the Huygens ' prin- ciple . Making use of ( 3 ) , we obtain from ( 1 ) and ( 2 ) ίωμ + Vg ( F , F ' ) × [ î × E ( F ′ ) ] } k2 iwe . 1 × 2 VVg ( F , F ′ ) · [ ŵ × H ( F ′ ) ] ( 17 ) VVg ( F , F ′ ) · [ ñ × E ( 7 ′ ) ] k2 + ...
Other editions - View all
Common terms and phrases
amplitudes angle antenna aperture approximation assume axis bianisotropic boundary conditions cavity complex conductor Consider constitutive relations coordinate cos² current sheet cutoff defined denote density derived determined dielectric direction dispersion relation dyadic Green's function E₁ E₂ eikr electric field electromagnetic waves field vectors frequency Green's function guidance condition guided waves H₁ H₂ impedance incident wave integral isotropic media k₁ kız linearly polarized Lorentz Lorentz transformation magnetic field matrix Maxwell's equations medium modes obtain optical permittivity perpendicular phase front plane wave Poynting's Poynting's theorem Poynting's vector Problem radiation radius reflection coefficient region saddle point scalar scattering Show shown in Figure sin² solution surface current tangential tensor theorem time-average TM waves transformation uniaxial wave equation wave propagating wave vector waveguide wavenumber zero