Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 7
... frequency is much greater than any hydrodynamic frequency , i.e. if we introduce a macroscopic time scale , T , length scale , L , and a characteristic velocity , V = LT - 1 , then , if the external forces are small , so that T - 21 ...
... frequency is much greater than any hydrodynamic frequency , i.e. if we introduce a macroscopic time scale , T , length scale , L , and a characteristic velocity , V = LT - 1 , then , if the external forces are small , so that T - 21 ...
Page 122
... frequency ( 4.6 ) vi ( ci ) = Vi Qi ( 1 cos x ) d2 , ( 2 ) where is the deflection angle in the laboratory system . We see that for the χ collision integral simple expressions in terms of the current density occur only if we can neglect ...
... frequency ( 4.6 ) vi ( ci ) = Vi Qi ( 1 cos x ) d2 , ( 2 ) where is the deflection angle in the laboratory system . We see that for the χ collision integral simple expressions in terms of the current density occur only if we can neglect ...
Page 148
... frequency in a tepid Cs plasma when the electron drift velocity parallel to the magnetic field exceeds about three times the ion thermal velocity . Under the conditions of this experiment the ratio of kinetic to magnetic pressure is ...
... frequency in a tepid Cs plasma when the electron drift velocity parallel to the magnetic field exceeds about three times the ion thermal velocity . Under the conditions of this experiment the ratio of kinetic to magnetic pressure is ...
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