Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 7
... frequency is much greater than any hydrodynamic frequency , i.e. if we introduce a macroscopic time scale , T , length scale , L , and a characteristic velocity , V = LT - 1 , then , if the external forces are small , so that T - 2 < 1 ...
... frequency is much greater than any hydrodynamic frequency , i.e. if we introduce a macroscopic time scale , T , length scale , L , and a characteristic velocity , V = LT - 1 , then , if the external forces are small , so that T - 2 < 1 ...
Page 122
... frequency ( 4.6 ) vi ( ci ) = - cos x ) d2 , ( 2 ) where is the deflection angle in the laboratory system . We see that for the X collision integral simple expressions in terms of the current density occur only if we can neglect the ...
... frequency ( 4.6 ) vi ( ci ) = - cos x ) d2 , ( 2 ) where is the deflection angle in the laboratory system . We see that for the X collision integral simple expressions in terms of the current density occur only if we can neglect the ...
Page 148
... frequency in a tepid C's plasma when the electron drift velocity parallel to the magnetic field exceeds about three times the ion . thermal velocity . Under the conditions of this experiment the ratio of kinetic . to magnetic pressure ...
... frequency in a tepid C's plasma when the electron drift velocity parallel to the magnetic field exceeds about three times the ion . thermal velocity . Under the conditions of this experiment the ratio of kinetic . to magnetic pressure ...
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