Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 146
... limit of this instability from the point of view of the generalized entropy discussed earlier . We recall that , consistent with the conservation of momentum , the lowest possible internal energy state for the plasma constituents is ...
... limit of this instability from the point of view of the generalized entropy discussed earlier . We recall that , consistent with the conservation of momentum , the lowest possible internal energy state for the plasma constituents is ...
Page 164
... limit on v corresponds to a growth rate that is of the same order as the rate of resistive diffusion , and is therefore insignificant . The upper limit on is reached only by modes that exist also in the standard infinite - conductivity ...
... limit on v corresponds to a growth rate that is of the same order as the rate of resistive diffusion , and is therefore insignificant . The upper limit on is reached only by modes that exist also in the standard infinite - conductivity ...
Page 247
... limit L → ∞ ; which boils down to the charge neutrality condition ( 37 ) R * * ( * ) exp [ 9 * ( * ) ] αξ * ' p * % ( 5 * ) — p * ( x * ) ( 0 * ( x * ) = o ( Lx * ) ; R * = R / L is assumed to stay finite in the limit ) . The trick to ...
... limit L → ∞ ; which boils down to the charge neutrality condition ( 37 ) R * * ( * ) exp [ 9 * ( * ) ] αξ * ' p * % ( 5 * ) — p * ( x * ) ( 0 * ( x * ) = o ( Lx * ) ; R * = R / L is assumed to stay finite in the limit ) . The trick to ...
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