Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 129
... radial potential distribution by integrating the equation of the radial field X. For the case of ambipolar diffusion we find eu ( 4.33 ) kT 1 + u + uc [ ( μ + / μe ) ( T + / Te ) ] 1 + U + U o • In x + . In u + u [ 1 + ( T + / T ...
... radial potential distribution by integrating the equation of the radial field X. For the case of ambipolar diffusion we find eu ( 4.33 ) kT 1 + u + uc [ ( μ + / μe ) ( T + / Te ) ] 1 + U + U o • In x + . In u + u [ 1 + ( T + / T ...
Page 130
... radial particle current is simply ( 4.36 ) Г. nn d B2 dr [ nk ( T ++ T. ) ] . eU / KT_ 03 0.2 01 01 -02 T U q = 0 9 = 100 9 = 50 9 = 20 9 = 15 Voo -0.3 9-10 Uo -04 -05 9 = 5 9 = 0 -06 0 0.2 04 06 08 r / R 1.0 Fig . 20. Ambipolar radial ...
... radial particle current is simply ( 4.36 ) Г. nn d B2 dr [ nk ( T ++ T. ) ] . eU / KT_ 03 0.2 01 01 -02 T U q = 0 9 = 100 9 = 50 9 = 20 9 = 15 Voo -0.3 9-10 Uo -04 -05 9 = 5 9 = 0 -06 0 0.2 04 06 08 r / R 1.0 Fig . 20. Ambipolar radial ...
Page 133
... radial distribution . One can give more general information about the problem if one simply integrates the two eqs . ( 4.40 ) after introduction of the equations ( 4.41 ) over the radial co - ordinate . We get two complex equations for ...
... radial distribution . One can give more general information about the problem if one simply integrates the two eqs . ( 4.40 ) after introduction of the equations ( 4.41 ) over the radial co - ordinate . We get two complex equations for ...
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