Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 54
... theory , the adiabatic theory and the double adiabatic theory or Chew - Goldberger - Low theory . The fluid theory corresponds to the strong - collision limit where collisions are so strong that the pressure always remains a scalar ...
... theory , the adiabatic theory and the double adiabatic theory or Chew - Goldberger - Low theory . The fluid theory corresponds to the strong - collision limit where collisions are so strong that the pressure always remains a scalar ...
Page 55
... theory is designated as adiabatic be- cause the motion of each particle is governed by the magnetic moment being an adiabatic invariant . In the double adiabatic theory a separate equation of state is derived for each of the two ...
... theory is designated as adiabatic be- cause the motion of each particle is governed by the magnetic moment being an adiabatic invariant . In the double adiabatic theory a separate equation of state is derived for each of the two ...
Page 180
... theory after linear theory not because this is the logical order but because it is the expedient one . Nonlinear theory of waves in plasmas , or of any other nontrivial phenomenon , does not consist of a new sweeping treatment of the ...
... theory after linear theory not because this is the logical order but because it is the expedient one . Nonlinear theory of waves in plasmas , or of any other nontrivial phenomenon , does not consist of a new sweeping treatment of the ...
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