Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 54
... limit where collisions are so strong that the pressure always remains a scalar , but however , still so weak that the conductivity may be taken as infinite . The adiabatic theory corresponds to the limit of no collisions and to the limit ...
... limit where collisions are so strong that the pressure always remains a scalar , but however , still so weak that the conductivity may be taken as infinite . The adiabatic theory corresponds to the limit of no collisions and to the limit ...
Page 146
... limit of this instability from the point of view of the generalized entropy discussed earlier . We recall that , consistent with the conservation of momentum , the lowest possible internal energy state for the plasma constituents is ...
... limit of this instability from the point of view of the generalized entropy discussed earlier . We recall that , consistent with the conservation of momentum , the lowest possible internal energy state for the plasma constituents is ...
Page 164
... limit on v corresponds to a growth rate that is of the same order as the rate of resistive diffusion , and is therefore insignificant . The upper limit on v is reached only by modes that exist also in the standard infinite ...
... limit on v corresponds to a growth rate that is of the same order as the rate of resistive diffusion , and is therefore insignificant . The upper limit on v is reached only by modes that exist also in the standard infinite ...
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