Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 121
... negative ion component and in the are column ( volume recombination ) . We decide to consider the three following problems : 1 ) The weakly ionized , nonthermal , four - component system ( including negative ions ) without a magnetic ...
... negative ion component and in the are column ( volume recombination ) . We decide to consider the three following problems : 1 ) The weakly ionized , nonthermal , four - component system ( including negative ions ) without a magnetic ...
Page 124
... negative ions and the third electron loss due to attachment of electrons . For the negative ions we have ( 4.21 ) A_ 124 G. ECKER.
... negative ions and the third electron loss due to attachment of electrons . For the negative ions we have ( 4.21 ) A_ 124 G. ECKER.
Page 125
For the negative ions we have ( 4.21 ) A_ = ẞn ̧ — on + n_ — Sn ̧n- , where the first term is due to electron attachment , the second due to recom- bination of positive with negative ions and the third due to detachment processes ...
For the negative ions we have ( 4.21 ) A_ = ẞn ̧ — on + n_ — Sn ̧n- , where the first term is due to electron attachment , the second due to recom- bination of positive with negative ions and the third due to detachment processes ...
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