Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 37
... approximation . - The integrals required to evaluate the D ; take the form d ( w + k⋅v ) | k2 ɛ ( k , w ) | 2 from ( III.3.10 ) fary fark do k d3k d ( w + k⋅v ) k2ε ( k , w ) 2 from ( III.3.13 ) where gv ' — v . fåoy fd'k do kk = ( k ...
... approximation . - The integrals required to evaluate the D ; take the form d ( w + k⋅v ) | k2 ɛ ( k , w ) | 2 from ( III.3.10 ) fary fark do k d3k d ( w + k⋅v ) k2ε ( k , w ) 2 from ( III.3.13 ) where gv ' — v . fåoy fd'k do kk = ( k ...
Page 97
... approximation procedure , but not by the model . This is different with the lectures on gas discharge theory where not so much a special approximation but rather the extension of the model charac- terizes the course . In a gas discharge ...
... approximation procedure , but not by the model . This is different with the lectures on gas discharge theory where not so much a special approximation but rather the extension of the model charac- terizes the course . In a gas discharge ...
Page 182
... approximation , we may still represent what goes on in a plasma instantaneously in terms of these waves , but we must allow for coupling between them so that the presence of one wave affects the dispersion relation of another , and ...
... approximation , we may still represent what goes on in a plasma instantaneously in terms of these waves , but we must allow for coupling between them so that the presence of one wave affects the dispersion relation of another , and ...
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