Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 33
... Calculation of the spectrum . To calculate the spectrum we can again assume that the electric field within the plasma is weak , and the interactions are small . At the same time , the effect of the field on the distribution function ...
... Calculation of the spectrum . To calculate the spectrum we can again assume that the electric field within the plasma is weak , and the interactions are small . At the same time , the effect of the field on the distribution function ...
Page 189
... calculations , but will not be discussed here . The more interesting effect is the slow time variation of the ... calculation , which may be represented by the equation ( 4.7 ) da ( k ) dt = i Σ C ( k1 , k2 , ka , k1 ) a * ( k2 ) ...
... calculations , but will not be discussed here . The more interesting effect is the slow time variation of the ... calculation , which may be represented by the equation ( 4.7 ) da ( k ) dt = i Σ C ( k1 , k2 , ka , k1 ) a * ( k2 ) ...
Page 239
... calculation : and assume a discontinuous transition between the sheath and the rest of the plasma . The asymptotic analysis of the problem shows instead that such a point does not exist , but a meaningful sheath concept can instead be ...
... calculation : and assume a discontinuous transition between the sheath and the rest of the plasma . The asymptotic analysis of the problem shows instead that such a point does not exist , but a meaningful sheath concept can instead be ...
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