Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 55
... KRUSKAL and OBERMAN [ 2 ] which is slightly more pessimistic ( more unstable ) than the energy principle of the adiabatic theory is definitely more pessimistic than that of the double adiabatic theory . The name double adiabatic theory ...
... KRUSKAL and OBERMAN [ 2 ] which is slightly more pessimistic ( more unstable ) than the energy principle of the adiabatic theory is definitely more pessimistic than that of the double adiabatic theory . The name double adiabatic theory ...
Page 89
... KRUSKAL and OBERMAN and differs from ours due to a difference in definition of ɛ . Their ε is EKо = vp + q2 / 2 with no y . Expression ( 88 ) is identical with that given by KRUSKAL and OBERMAN after one sets f1 = f in their expression ...
... KRUSKAL and OBERMAN and differs from ours due to a difference in definition of ɛ . Their ε is EKо = vp + q2 / 2 with no y . Expression ( 88 ) is identical with that given by KRUSKAL and OBERMAN after one sets f1 = f in their expression ...
Page 96
... Kruskal Oberman theory , = implies . Again the derivation of the comparison theorems follows that given in both references [ 2 ] and [ 5 ] . *** I should like to thank DIETRICH VOSLAMBER for critically reading these notes and making ...
... Kruskal Oberman theory , = implies . Again the derivation of the comparison theorems follows that given in both references [ 2 ] and [ 5 ] . *** I should like to thank DIETRICH VOSLAMBER for critically reading these notes and making ...
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