Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 55
... principle in each case are formally the same . When the energy principles are derived they will be compared for ... energy prin- ciple is not completed as yet but it has been shown that the energy principle of KRUSKAL and OBERMAN [ 2 ] ...
... principle in each case are formally the same . When the energy principles are derived they will be compared for ... energy prin- ciple is not completed as yet but it has been shown that the energy principle of KRUSKAL and OBERMAN [ 2 ] ...
Page 64
... energy principle for stability i.e. an expression SW ( E , E ) quadratic in such that stability can be reduced to examining the sign of SW ( E , E ) . SW will turn out to be the variation in potential energy of the system . For a simple ...
... energy principle for stability i.e. an expression SW ( E , E ) quadratic in such that stability can be reduced to examining the sign of SW ( E , E ) . SW will turn out to be the variation in potential energy of the system . For a simple ...
Page 67
... energy principle has the advantage . This is facilitated by the fact that the energy has a physically intuitive significance . The first two terms represent the variation of the magnetic energy and the last two of the plasma energy ...
... energy principle has the advantage . This is facilitated by the fact that the energy has a physically intuitive significance . The first two terms represent the variation of the magnetic energy and the last two of the plasma energy ...
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