Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 57
... corresponds to very large 7 which seems to contradict our previous assumption . However , in this case , σ large ... corresponds to the neglect of displacement current and the electric force term in the momentum eq . ( 2 ) . Also we wish ...
... corresponds to very large 7 which seems to contradict our previous assumption . However , in this case , σ large ... corresponds to the neglect of displacement current and the electric force term in the momentum eq . ( 2 ) . Also we wish ...
Page 82
... corresponds to the fact that for x = = 0 Eo = 0 ) and E constant , & is a constant of the motion . These facts may ... correspond to one of ƒ we must sum the integrals over the + and values . Thus the Σ . ― Note also for toroidal ...
... corresponds to the fact that for x = = 0 Eo = 0 ) and E constant , & is a constant of the motion . These facts may ... correspond to one of ƒ we must sum the integrals over the + and values . Thus the Σ . ― Note also for toroidal ...
Page 170
... corresponds to large nega- tive 4 ' , we find that the eigenvalues A lie slightly below the points 1 , 2 , 3 , For the fastest growing mode , which corresponds to a solution U that is basically symmetric near Mo , we have 4. As we move ...
... corresponds to large nega- tive 4 ' , we find that the eigenvalues A lie slightly below the points 1 , 2 , 3 , For the fastest growing mode , which corresponds to a solution U that is basically symmetric near Mo , we have 4. As we move ...
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