Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 78
... zero order in ( 16 ) we need J to zero order which by ( 18 ) involves f ' . Because of ( 11 ) eq . ( 9 ) may be solved for f ' but not uniquely ; only up to a function of t , r , w and q as in the case of the solution for fo ( at first ) ...
... zero order in ( 16 ) we need J to zero order which by ( 18 ) involves f ' . Because of ( 11 ) eq . ( 9 ) may be solved for f ' but not uniquely ; only up to a function of t , r , w and q as in the case of the solution for fo ( at first ) ...
Page 132
... zero - order solution is already given in the preceding chapter if we use σ = 0 due to the assumption of weak ionization . If the index ( 0 ) designates the zero order approximation , then we use ( 4.39 ) n = no + n ' , V = V。 + V ...
... zero - order solution is already given in the preceding chapter if we use σ = 0 due to the assumption of weak ionization . If the index ( 0 ) designates the zero order approximation , then we use ( 4.39 ) n = no + n ' , V = V。 + V ...
Page 163
... zero - order equilibrium condition of eq . ( 7 ) may be written as ishe F = F " . The usual boundary conditions are that both y and W should vanish at infinity or at conducting boundaries , located at μμ1 , M2 . = 3 . - General remarks ...
... zero - order equilibrium condition of eq . ( 7 ) may be written as ishe F = F " . The usual boundary conditions are that both y and W should vanish at infinity or at conducting boundaries , located at μμ1 , M2 . = 3 . - General remarks ...
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