Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 182
... relation ( 1.1 ) into a form which resembles the dispersion relation for a warm plasma [ 5 ] ( 1.3 ) wav2 ) k2 . We shall also show that another effect of this wave interaction is to damp an initial wave , if there is a random ...
... relation ( 1.1 ) into a form which resembles the dispersion relation for a warm plasma [ 5 ] ( 1.3 ) wav2 ) k2 . We shall also show that another effect of this wave interaction is to damp an initial wave , if there is a random ...
Page 190
... relations » [ 8 ] , which will be discus- sed further in Section 6. The terms of ( 4.7 ) for which k1 = k2 and k ̧ = k ̧ ... relation ( 4.15 ) where ( 4.16 ) w = wp + △ Q ( k ) , AQ ( k ) = C ( k , k ' ) a ( k ' ) 2 . k The expression ...
... relations » [ 8 ] , which will be discus- sed further in Section 6. The terms of ( 4.7 ) for which k1 = k2 and k ̧ = k ̧ ... relation ( 4.15 ) where ( 4.16 ) w = wp + △ Q ( k ) , AQ ( k ) = C ( k , k ' ) a ( k ' ) 2 . k The expression ...
Page 191
... relation for a wave in a thermal plasma may be obtained on a one - dimensional model , whereas , according to ( 4.14 ) , the background waves parallel to the test wave make no contribution to ( 4.17 ) . However , in a thermal plasma ...
... relation for a wave in a thermal plasma may be obtained on a one - dimensional model , whereas , according to ( 4.14 ) , the background waves parallel to the test wave make no contribution to ( 4.17 ) . However , in a thermal plasma ...
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