Classical Electrodynamics |
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Page 24
... equal to 91 , while the second has 92. Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
... equal to 91 , while the second has 92. Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
Page 263
... equal to its free - space value V / c . Immediately below this " cutoff " frequency , the system no longer acts as a guide but as an antenna , with energy being radiated radially . For frequencies well above cutoff , ẞ and k are of the ...
... equal to its free - space value V / c . Immediately below this " cutoff " frequency , the system no longer acts as a guide but as an antenna , with energy being radiated radially . For frequencies well above cutoff , ẞ and k are of the ...
Page 382
... equal to y times its nonrelati- vistic value . In the same limit , however , the duration of appreciable field strengths at the point P is decreased . A measure of the time interval over which the fields are appreciable is evidently b ...
... equal to y times its nonrelati- vistic value . In the same limit , however , the duration of appreciable field strengths at the point P is decreased . A measure of the time interval over which the fields are appreciable is evidently b ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ