Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 6
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 dt 1 Απ Vp + ( ▽ × B ) × B + 1 a 4лc2 Сt ( VXB ) × B 1 V. ( VXB ) VXB Απ C2 The last two terms are ...
... 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 dt 1 Απ Vp + ( ▽ × B ) × B + 1 a 4лc2 Сt ( VXB ) × B 1 V. ( VXB ) VXB Απ C2 The last two terms are ...
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 97
... Debye length is small compared with other lengths of interest . Conse- quently in a course on the theory of the plasma you will expect that one model , namely an unbounded many - particle system consisting of an electron , ion and ...
... Debye length is small compared with other lengths of interest . Conse- quently in a course on the theory of the plasma you will expect that one model , namely an unbounded many - particle system consisting of an electron , ion and ...
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