Advanced Plasma TheoryM. N. Rosenbluth |
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Page 193
... waves ( plasma oscillations ) and plane transverse waves ( electromagnetic waves ) : ( 5.1 ) A , * Σl , [ a , exp [ i ( k x − ∞ , t ) ] + a exp [ — i ( k · x — wpt ) ] + k - − + Σe , [ a , exp [ i ( k⋅ x − ∞1t ) ] + a ‡ exp [ — i ...
... waves ( plasma oscillations ) and plane transverse waves ( electromagnetic waves ) : ( 5.1 ) A , * Σl , [ a , exp [ i ( k x − ∞ , t ) ] + a exp [ — i ( k · x — wpt ) ] + k - − + Σe , [ a , exp [ i ( k⋅ x − ∞1t ) ] + a ‡ exp [ — i ...
Page 194
... wave . This is not unreasonable , for the growth in amplitude of a wave packet should depend upon the source terms ... transverse wave . This is an example of the wave - interaction relations which will be discussed further in Section 6 ...
... wave . This is not unreasonable , for the growth in amplitude of a wave packet should depend upon the source terms ... transverse wave . This is an example of the wave - interaction relations which will be discussed further in Section 6 ...
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 KRUSKAL KULSRUD l'axe magnétique limit lowest order magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle périodique 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