Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 15
... distribution and + in the ion distribution ; the equations becoming 1 w2 1 2 ( 2 VV : ( 2010 - 10+ 1 ) + ( 102 ) and ... angular depend- ence by a harmonic expansion , i.e. p = Σi ± n { Ti ± n ( 9 , q ) = Nin P ( cos 0 ) Isin no · cos ng ...
... distribution and + in the ion distribution ; the equations becoming 1 w2 1 2 ( 2 VV : ( 2010 - 10+ 1 ) + ( 102 ) and ... angular depend- ence by a harmonic expansion , i.e. p = Σi ± n { Ti ± n ( 9 , q ) = Nin P ( cos 0 ) Isin no · cos ng ...
Page 38
... angular integration merely selects those parts of kk orthogonal to g , i.e. ef . ( III.1.6 ) , hence fa2 kk 8 ( k1g ) ... distribution function perturbed by the incident r — f field . 0 1 . IV . The Kinetic Equation in a Magnetic 38 W. B. ...
... angular integration merely selects those parts of kk orthogonal to g , i.e. ef . ( III.1.6 ) , hence fa2 kk 8 ( k1g ) ... distribution function perturbed by the incident r — f field . 0 1 . IV . The Kinetic Equation in a Magnetic 38 W. B. ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
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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