Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 78
... quantities . This system is ( 11 ) , ( 15 ) , ( 16 ) and ( 24 ) with side conditions ( 14 ) , ( 22 ) and ( 23 ) ... quantities which are necessary conditions for the solu- tions of the first order equations have been obtained . Thus , we ...
... quantities . This system is ( 11 ) , ( 15 ) , ( 16 ) and ( 24 ) with side conditions ( 14 ) , ( 22 ) and ( 23 ) ... quantities which are necessary conditions for the solu- tions of the first order equations have been obtained . Thus , we ...
Page 121
... quantities without index refer to the par- ticle under consideration , the index ( i ) to the particle components with which the test particle collides . The prime ( ' ) characterizes quantities after collision . The bar indicates the ...
... quantities without index refer to the par- ticle under consideration , the index ( i ) to the particle components with which the test particle collides . The prime ( ' ) characterizes quantities after collision . The bar indicates the ...
Page 133
... quantities . If we had solved this problem then we could judge by the imaginary part of the eigenvalues whether a given mode grows or decays , that means whether the mode is unstable or stable . This question is of interest for the ...
... quantities . If we had solved this problem then we could judge by the imaginary part of the eigenvalues whether a given mode grows or decays , that means whether the mode is unstable or stable . This question is of interest for the ...
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