Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 193
... waves ( plasma oscillations ) and plane transverse waves ( electromagnetic waves ) : ( 5.1 ) - * A , = 1 , [ a , exp [ i ( k · x − ∞ , t ) ] + a exp [ — i ( k · x − wpt ) ] + k * + Σe , [ a , exp [ i ( k⋅ x — o , t ) ] + a exp [ — i ...
... waves ( plasma oscillations ) and plane transverse waves ( electromagnetic waves ) : ( 5.1 ) - * A , = 1 , [ a , exp [ i ( k · x − ∞ , t ) ] + a exp [ — i ( k · x − wpt ) ] + k * + Σe , [ a , exp [ i ( k⋅ x — o , t ) ] + a exp [ — i ...
Page 211
... transverse wave . We therefore consider such a group , writing the wave vectors of the longitudinal waves as k11 , k127 and the wave vector of the transverse wave as kr . If there is to be nonzero interaction , frequencies and wave ...
... transverse wave . We therefore consider such a group , writing the wave vectors of the longitudinal waves as k11 , k127 and the wave vector of the transverse wave as kr . If there is to be nonzero interaction , frequencies and wave ...
Common terms and phrases
adiabatic invariant amplitude approximation Boltzmann equation boundary conditions boundary layer calculated cathode coefficient collision components consider constant contraction corresponds courbe critère current density d³k d³v Debye length derived differential equations discharge dispersion relation distribution function eigenvalue electric field electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ k₂ KRUSKAL KULSRUD l'axe magnétique limit lowest order m₁ magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle perturbation Phys plasma oscillations plasma physics Poisson's equation potential problem quantities R₁ radial region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity voisinage waves in plasmas zero zero-order Απ