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Page 209
... wave eiko for all x , the orthogonality relation ( 2.52 ) shows that A ( k ) = √2πd ( k − k 。) , corresponding to a monochromatic traveling wave u ( x , t ) = eikox - iw ( ko ) , as required . If , however , at t = 0 , u ( x , 0 ) ...
... wave eiko for all x , the orthogonality relation ( 2.52 ) shows that A ( k ) = √2πd ( k − k 。) , corresponding to a monochromatic traveling wave u ( x , t ) = eikox - iw ( ko ) , as required . If , however , at t = 0 , u ( x , 0 ) ...
Page 340
... wave number kp , 2 KD kp2 = 2 @p ( u2 ) ( 10.106 ) that appreciable departures of the frequency from @ , occur . For wave numbers k « k » , the phase and group velocities of the longitudinal plasma oscillations are : @p UD k 3 ( u2 ) Ug ...
... wave number kp , 2 KD kp2 = 2 @p ( u2 ) ( 10.106 ) that appreciable departures of the frequency from @ , occur . For wave numbers k « k » , the phase and group velocities of the longitudinal plasma oscillations are : @p UD k 3 ( u2 ) Ug ...
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.
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ