Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 39
... interaction matters . For temperatures T > 500 keV the entire calculation should be made relativistic a complication I propose to avoid . If the magnetic interaction is omitted ( IV.1.1 ) may be coarse - grained as before , and the last ...
... interaction matters . For temperatures T > 500 keV the entire calculation should be made relativistic a complication I propose to avoid . If the magnetic interaction is omitted ( IV.1.1 ) may be coarse - grained as before , and the last ...
Page 189
... interaction by perturbation methods . The harmonic content can be extracted from these calculations , but will not be discussed here . The more interesting effect is the slow time variation of the amplitudes . It is found that both ...
... interaction by perturbation methods . The harmonic content can be extracted from these calculations , but will not be discussed here . The more interesting effect is the slow time variation of the amplitudes . It is found that both ...
Page 197
... interaction process . The two formulas are not equivalent , and the difference may be traced to differences between the subsidiary condi- tions which appear most appropriate to the Eulerian formulation and the Lagrangian formulation of ...
... interaction process . The two formulas are not equivalent , and the difference may be traced to differences between the subsidiary condi- tions which appear most appropriate to the Eulerian formulation and the Lagrangian formulation of ...
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