Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 54
... fluid 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 ...
... fluid 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 ...
Page 55
... fluid theory . Thus , since these equations arise from an adiabatic assumption ( adiabatic here means no heat flow ) this theory is often called the double adiabatic theory . The two uses of the term adiabatic in adiabatic theory and ...
... fluid theory . Thus , since these equations arise from an adiabatic assumption ( adiabatic here means no heat flow ) this theory is often called the double adiabatic theory . The two uses of the term adiabatic in adiabatic theory and ...
Page 91
F But W gives a necessary and sufficient result for stability on the fluid theory . Hence if the fluid theory gives stability so must the adiabatic theory . Thus , we see the fluid theory gives reliable results even in cases where one ...
F But W gives a necessary and sufficient result for stability on the fluid theory . Hence if the fluid theory gives stability so must the adiabatic theory . Thus , we see the fluid theory gives reliable results even in cases where one ...
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