Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 9
... relaxation term , i.e. retaining only the tendency for a distribution function f to relax back to the Maxwellian , and representing I ( f ) by − 1 / t ( f - fo ) , whereupon ( I.3.3 ) becomes 1 / τ ( f 。− f ) = Dfo , or f = fo¬tDƒ ...
... relaxation term , i.e. retaining only the tendency for a distribution function f to relax back to the Maxwellian , and representing I ( f ) by − 1 / t ( f - fo ) , whereupon ( I.3.3 ) becomes 1 / τ ( f 。− f ) = Dfo , or f = fo¬tDƒ ...
Page 172
... relaxation of the constraint that fluid must remain attached to magnetic field . For a zero - order field that is not a vacuum field , possibilities of lowering po- tential energy are always present ; the introduction of finite ...
... relaxation of the constraint that fluid must remain attached to magnetic field . For a zero - order field that is not a vacuum field , possibilities of lowering po- tential energy are always present ; the introduction of finite ...
Page 240
... relaxation from Liouville to the Fokker - Planck equation and then to thermal equilibrium constitutes a « contraction » in the description of the fluid from a function of 6N variables to one of 6 ( the particle distri- bution in phase ...
... relaxation from Liouville to the Fokker - Planck equation and then to thermal equilibrium constitutes a « contraction » in the description of the fluid from a function of 6N variables to one of 6 ( the particle distri- bution in phase ...
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