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Page 340
... wave number kD KD 2 = 2 “ ო ( u2 ) ( 10.106 ) that appreciable departures of the frequency from ∞ , occur . For wave numbers k « kp , the phase and group velocities of the longitudinal plasma oscillations are : @p Vp k 3 ( u2 ) Vp ...
... wave number kD KD 2 = 2 “ ო ( u2 ) ( 10.106 ) that appreciable departures of the frequency from ∞ , occur . For wave numbers k « kp , the phase and group velocities of the longitudinal plasma oscillations are : @p Vp k 3 ( u2 ) Vp ...
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.
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ