Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
From inside the book
Results 1-3 of 46
Page 101
... velocity . v с Relative particle velocity . Va R I E Γ α β Drift velocity . Radius of the column . Discharge current . Longitudinal electric field component . Radial potential distribution . Ionization coefficient for electron - neutral ...
... velocity . v с Relative particle velocity . Va R I E Γ α β Drift velocity . Radius of the column . Discharge current . Longitudinal electric field component . Radial potential distribution . Ionization coefficient for electron - neutral ...
Page 148
... velocity becomes comparable to the electron thermal velocity . Only in situations where T. > T ; does the critical velocity approach the ion thermal velocity . In the following , we shall show that for a collisionless plasma instability ...
... velocity becomes comparable to the electron thermal velocity . Only in situations where T. > T ; does the critical velocity approach the ion thermal velocity . In the following , we shall show that for a collisionless plasma instability ...
Page 185
... velocity . Since the distribution function must be indepen- dent of the time , ions of energy E + = eq1 must be equally distributed between the two directions of the velocity , and simi- larly for all trapped ions . On the other hand ...
... velocity . Since the distribution function must be indepen- dent of the time , ions of energy E + = eq1 must be equally distributed between the two directions of the velocity , and simi- larly for all trapped ions . On the other hand ...
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