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Page 310
... Oscillations occur in the charge density . These high - frequency oscillations are called plasma oscillations and are to be distinguished from lower - frequency oscillations which involve motion of the fluid , but no charge separation ...
... Oscillations occur in the charge density . These high - frequency oscillations are called plasma oscillations and are to be distinguished from lower - frequency oscillations which involve motion of the fluid , but no charge separation ...
Page 341
... oscillations are virtually undamped . But the damping becomes important as soon as k ~ k ( even for k = 0.5kp , Im w ~ -w / 6 ) . For wave numbers larger than the Debye wave number the damping is so great that it is meaningless to speak ...
... oscillations are virtually undamped . But the damping becomes important as soon as k ~ k ( even for k = 0.5kp , Im w ~ -w / 6 ) . For wave numbers larger than the Debye wave number the damping is so great that it is meaningless to speak ...
Page 628
... oscillations , 340 see also Radiative reaction Darwin - Breit interaction , 411 Debye - Hückel screening radius or ... oscillating electric , 271 Oscillating magnetic , 274 Dipole moment , electrostatic , 100 induced , 120 interaction ...
... oscillations , 340 see also Radiative reaction Darwin - Breit interaction , 411 Debye - Hückel screening radius or ... oscillating electric , 271 Oscillating magnetic , 274 Dipole moment , electrostatic , 100 induced , 120 interaction ...
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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