Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 99
... diffusion and wall recombination . Characteristic for the subnormal region is that the diffusion is not ambipolar since the particle den- sities are too small to build up the ambipolar field . When with current increase the particle ...
... diffusion and wall recombination . Characteristic for the subnormal region is that the diffusion is not ambipolar since the particle den- sities are too small to build up the ambipolar field . When with current increase the particle ...
Page 100
... diffusion in a magnetic field . 2. List of symbols . - The following symbols with their subsequent meanings are chosen for the description of the observations and the formulation of the laws . For technical reasons different symbols had ...
... diffusion in a magnetic field . 2. List of symbols . - The following symbols with their subsequent meanings are chosen for the description of the observations and the formulation of the laws . For technical reasons different symbols had ...
Page 111
... diffusion ) . To assess this effect it is important to remember that the electrons them- selves alter the potential distribution . Otherwise one might come to the inaccurate conclusion that because of their small thermal energy ( order ...
... diffusion ) . To assess this effect it is important to remember that the electrons them- selves alter the potential distribution . Otherwise one might come to the inaccurate conclusion that because of their small thermal energy ( order ...
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