Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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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 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 ...
Page 259
... KRUSKAL : ( private communication ) . [ 6 ] P. LANGEVIN and M. DE BROGLIE : La Théorie du Rayonnement et les Quanta ( Report on meeting at Institute Solvay , Brussels , 1911 ) ( Paris , 1912 ) , p . 450 . [ 7 ] G. D. BIRKHOFF : Trans ...
... KRUSKAL : ( private communication ) . [ 6 ] P. LANGEVIN and M. DE BROGLIE : La Théorie du Rayonnement et les Quanta ( Report on meeting at Institute Solvay , Brussels , 1911 ) ( Paris , 1912 ) , p . 450 . [ 7 ] G. D. BIRKHOFF : Trans ...
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