Classical Electrodynamics |
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Page 340
... wave number kp , kp = Wp 2 ( u2 ) ( 10.106 ) that appreciable departures of the frequency from ∞ , occur . For wave numbers kk , the phase and group velocities of the longitudinal plasma oscillations are : % ~ k 3 ( u2 ) Vg Up ( 10.107 ) ...
... wave number kp , kp = Wp 2 ( u2 ) ( 10.106 ) that appreciable departures of the frequency from ∞ , occur . For wave numbers kk , the phase and group velocities of the longitudinal plasma oscillations are : % ~ k 3 ( u2 ) Vg Up ( 10.107 ) ...
Page 363
... wave is an invariant quantity . Actually , the phase of any plane wave is invariant under a Lorentz transformation , the reason being that the phase can be associated with mere counting which is independent of coordinate frame ...
... wave is an invariant quantity . Actually , the phase of any plane wave is invariant under a Lorentz transformation , the reason being that the phase can be associated with mere counting which is independent of coordinate frame ...
Page 640
... wave solutions , 203 , 212 in wave guide , 244 Uncertainty principle , 209 , 215 use of , to obtain quantum - mechanical modifications , 440 , 442 , 453 , 455 , 511 , 527 , 532 ... Wave packets , spreading in time , 215 Waves , 640 Index.
... wave solutions , 203 , 212 in wave guide , 244 Uncertainty principle , 209 , 215 use of , to obtain quantum - mechanical modifications , 440 , 442 , 453 , 455 , 511 , 527 , 532 ... Wave packets , spreading in time , 215 Waves , 640 Index.
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