Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 146
... equations instead of just Poisson's equation so that the dispersion relative is a 3 × 3 deter- minant . However , in the limit of small B , the only possible instabilities are those which do not perturb the magnetic field as any ...
... equations instead of just Poisson's equation so that the dispersion relative is a 3 × 3 deter- minant . However , in the limit of small B , the only possible instabilities are those which do not perturb the magnetic field as any ...
Page 147
... Poisson's equation , we must now perform the time integral indicated above as well as the integral over all velocities . Thus we have to do the integrals fr . dr . fde fde får exp [ pr ] exp [ ik , r , t ] exp [ ik , y ] exp It is ...
... Poisson's equation , we must now perform the time integral indicated above as well as the integral over all velocities . Thus we have to do the integrals fr . dr . fde fde får exp [ pr ] exp [ ik , r , t ] exp [ ik , y ] exp It is ...
Page 241
... equations with nearly periodic solutions , which is closely related to our topic , see KRUSKAL [ 8 ] . 4 ... Poisson's equation in one variable only , the longitudinal distance from the probe z ; it is just this feature that ...
... equations with nearly periodic solutions , which is closely related to our topic , see KRUSKAL [ 8 ] . 4 ... Poisson's equation in one variable only , the longitudinal distance from the probe z ; it is just this feature that ...
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