Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 9
Page 65
... always positive . Hence SW < 0 for some E implies instability . If w < 0 , SW ( §n , §n ) < 0 and thus instability → SW < 0 for 5 Rendiconti S.I.F. - XXV . some an's ( or ) . Hence 8W > 0 GENERAL STABILITY THEORY IN PLASMA PHYSICS 65.
... always positive . Hence SW < 0 for some E implies instability . If w < 0 , SW ( §n , §n ) < 0 and thus instability → SW < 0 for 5 Rendiconti S.I.F. - XXV . some an's ( or ) . Hence 8W > 0 GENERAL STABILITY THEORY IN PLASMA PHYSICS 65.
Page 96
... implies . Again the derivation of the comparison theorems follows that given in both references [ 2 ] and [ 5 ] . *** I should like to thank DIETRICH VOSLAMBER for critically reading these notes and making useful comments on them . Part ...
... implies . Again the derivation of the comparison theorems follows that given in both references [ 2 ] and [ 5 ] . *** I should like to thank DIETRICH VOSLAMBER for critically reading these notes and making useful comments on them . Part ...
Page 254
... imply that any change in it must vanish more rapidly than any power of the parameter of smallness , i.e. , the relative change of the field over the Larmor radius . This does not imply that it must be a rigorous constant . For instance ...
... imply that any change in it must vanish more rapidly than any power of the parameter of smallness , i.e. , the relative change of the field over the Larmor radius . This does not imply that it must be a rigorous constant . For instance ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
3 other sections not shown
Other editions - View all
Common terms and phrases
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