Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 57
... Debye length , etc. We do not stress these in the fluid theory . ) Substituting ( 8 ′ ) in ( 5 ) and ( 7 ) and these in ( 2 ) we have dv Q Vp + dt 1 ( ▽ × B ) × B + Απ 1 a 4лc2 t 1 V. ( VB ) V > B ( V × B ) × B Απ C2 The last two terms ...
... Debye length , etc. We do not stress these in the fluid theory . ) Substituting ( 8 ′ ) in ( 5 ) and ( 7 ) and these in ( 2 ) we have dv Q Vp + dt 1 ( ▽ × B ) × B + Απ 1 a 4лc2 t 1 V. ( VB ) V > B ( V × B ) × B Απ C2 The last two terms ...
Page 78
... Debye length of both ions and electrons are small compared to macroscopic lengths and 2 ) both gyration frequencies and plasma frequencies are large compared to macroscopic frequencies . It is not always the case that these conditions ...
... Debye length of both ions and electrons are small compared to macroscopic lengths and 2 ) both gyration frequencies and plasma frequencies are large compared to macroscopic frequencies . It is not always the case that these conditions ...
Page 239
... lengths , whose ratio is very small : the Debye length and the mean free path for collisions or ionization . It can be expected , therefore , that the transition from vacuum or from a conductor to a free plasma occurs in two stages ...
... lengths , whose ratio is very small : the Debye length and the mean free path for collisions or ionization . It can be expected , therefore , that the transition from vacuum or from a conductor to a free plasma occurs in two stages ...
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 electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ k₂ KRUSKAL KULSRUD l'axe magnétique limit lowest order m₁ magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle perturbation Phys plasma oscillations plasma physics Poisson's equation potential problem quantities R₁ radial region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity voisinage waves in plasmas zero zero-order Απ