Classical Electrodynamics |
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Page 297
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
Page 324
... compared to the radius , the dynamic behavior is characteristic of hydrodynamic shock waves . But for a hot , tenuous plasma the mean free path is comparable to , or larger than , the radius . Then a model with particles moving freely ...
... compared to the radius , the dynamic behavior is characteristic of hydrodynamic shock waves . But for a hot , tenuous plasma the mean free path is comparable to , or larger than , the radius . Then a model with particles moving freely ...
Page 432
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
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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