Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 57
... satisfied . This latter is more stringent . ( Of course , there are other conditions that must be satisfied in the fluid theory such as small gyration radius , small Debye length , etc. We do not stress these in the fluid theory ...
... satisfied . This latter is more stringent . ( Of course , there are other conditions that must be satisfied in the fluid theory such as small gyration radius , small Debye length , etc. We do not stress these in the fluid theory ...
Page 77
... satisfied . ( This is just ( do - 1 / dt ) + ▽ · J - 1 = 0. ) Similarly the time derivative of ( 23 ) gives Ne2 ( 24 ) Σ E1 = Σ — n · ( V · Po ° ) , m m where Po = m [ ( v_ — α — vn ) ( v — α — v1 n ) ƒo d3v , is the zero order ...
... satisfied . ( This is just ( do - 1 / dt ) + ▽ · J - 1 = 0. ) Similarly the time derivative of ( 23 ) gives Ne2 ( 24 ) Σ E1 = Σ — n · ( V · Po ° ) , m m where Po = m [ ( v_ — α — vn ) ( v — α — v1 n ) ƒo d3v , is the zero order ...
Page 86
... satisfy restriction ( 75 ) , and one must be able to determine h from eq . ( 76 ) . It is easily seen that the latter re- quires that ( 75 ) be satisfied by . In summary the stability problem is re- duced to examining all solutions of ...
... satisfy restriction ( 75 ) , and one must be able to determine h from eq . ( 76 ) . It is easily seen that the latter re- quires that ( 75 ) be satisfied by . In summary the stability problem is re- duced to examining all solutions of ...
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