Advanced Plasma TheoryM. N. Rosenbluth |
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Page 49
... produced by a particle in a plasma , namely ( in the absence of a magnetic field ) ( V.1.1 ) p ( k , w ) : = d ( w + k⋅v ) k2 ε ( k , w ) exp [ — ik . x , ] , we may now use the Vlasov equation to calculate the disturbance that this ...
... produced by a particle in a plasma , namely ( in the absence of a magnetic field ) ( V.1.1 ) p ( k , w ) : = d ( w + k⋅v ) k2 ε ( k , w ) exp [ — ik . x , ] , we may now use the Vlasov equation to calculate the disturbance that this ...
Page 103
M. N. Rosenbluth. produced which provide the current continuity in front of the cathode and anode ? 2 ) How is it ... produced in the gas area . The liberation of ions from the electrode is hardly of practical interest . Electrons can ...
M. N. Rosenbluth. produced which provide the current continuity in front of the cathode and anode ? 2 ) How is it ... produced in the gas area . The liberation of ions from the electrode is hardly of practical interest . Electrons can ...
Page 109
... produced in the anode region to those to be produced in the cathode region is μ / μ . Therefore in front of the anode the question of current continuity is less problematic and interesting . Further a considerable simplification arises ...
... produced in the anode region to those to be produced in the cathode region is μ / μ . Therefore in front of the anode the question of current continuity is less problematic and interesting . Further a considerable simplification arises ...
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 KRUSKAL KULSRUD l'axe magnétique limit 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 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