Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 150
... wave lengths comparable to the ion - gyro- radius , kR1 ; To .. = 1 ; 0,00 . Moreover we see that since u / the < 1 the argument of the electron W function is very small . Since we are concerned with a wave nearly at resonance with the ...
... wave lengths comparable to the ion - gyro- radius , kR1 ; To .. = 1 ; 0,00 . Moreover we see that since u / the < 1 the argument of the electron W function is very small . Since we are concerned with a wave nearly at resonance with the ...
Page 187
... function . By considering various trapping regions of a wave of arbitrary form suc- cessively , filling a potential well with an appropriate distribution of trapped ions and a potential hump with an appropriate distribution of trapped ...
... function . By considering various trapping regions of a wave of arbitrary form suc- cessively , filling a potential well with an appropriate distribution of trapped ions and a potential hump with an appropriate distribution of trapped ...
Page 209
... function H by eq . ( A - 4.12 ) . However , on noting that we shall need only the zero - frequency part of this ... wave interaction . APPENDIX VI Coupling of electromagnetic and electrostatic waves in plasmas . If it is assumed that the ...
... function H by eq . ( A - 4.12 ) . However , on noting that we shall need only the zero - frequency part of this ... wave interaction . APPENDIX VI Coupling of electromagnetic and electrostatic waves in plasmas . If it is assumed that the ...
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