Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 193
... waves ( plasma oscillations ) and plane transverse waves ( electromagnetic waves ) : ( 5.1 ) and Ar McWP Σl , [ a , exp [ i ( k⋅ x − ∞ , t ) ] + a exp [ — i ( k · x — opt ) ] + k - + Σe , [ a , exp [ i ( k⋅ x − ∞1t ) ] + a exp ...
... waves ( plasma oscillations ) and plane transverse waves ( electromagnetic waves ) : ( 5.1 ) and Ar McWP Σl , [ a , exp [ i ( k⋅ x − ∞ , t ) ] + a exp [ — i ( k · x — opt ) ] + k - + Σe , [ a , exp [ i ( k⋅ x − ∞1t ) ] + a exp ...
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 ...
Page 211
... transverse wave . We therefore consider such a group , writing the wave vectors of the longitudinal waves as k11 , k12 , 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 , k12 , and the wave vector of the transverse wave as kr . If there is to be nonzero interaction , frequencies and wave ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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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 electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function 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 region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ