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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 ~ −0.7w ) . 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 ~ −0.7w ) . 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 ог ... 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 ог ... oscillating electric , 271 oscillating magnetic , 274 Dipole moment , electrostatic , 100 induced , 120 interaction ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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