Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 152
... geometry : magnetic field in the direction , and plasma parameters and field strength varying with . Thus , for the ... 3 γ + d n T ' 8 , T and from charge neutrality , we must have n ' n ' n n We will also assume for simplicity that the ...
... geometry : magnetic field in the direction , and plasma parameters and field strength varying with . Thus , for the ... 3 γ + d n T ' 8 , T and from charge neutrality , we must have n ' n ' n n We will also assume for simplicity that the ...
Page 160
... geometry can be introduced as desired . In Section 2 of this paper we derive the basis equations . In Section 3 we demonstrate some general properties of the unstable modes . In Section 4 we find the solutions in the outer , infinite ...
... geometry can be introduced as desired . In Section 2 of this paper we derive the basis equations . In Section 3 we demonstrate some general properties of the unstable modes . In Section 4 we find the solutions in the outer , infinite ...
Page 211
... geometry of the model and all pairs of values of the polarization vector e ... three . We consider the effect of interactions between two longitudinal waves ... 3 We mow assume that solutions of the eqs . ( A - 6.5 ) and ( A - 6.6 ) may ...
... geometry of the model and all pairs of values of the polarization vector e ... three . We consider the effect of interactions between two longitudinal waves ... 3 We mow assume that solutions of the eqs . ( A - 6.5 ) and ( A - 6.6 ) may ...
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