Advanced Plasma TheoryM. N. Rosenbluth |
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Page 105
... charge region . V. , X , and j have to be measured in V , V / cm and A / cm2 , respectively . MacKeowns formula is based on the assump- tion that electrons and ions move inertia - limited under the influence of their own space - charge ...
... charge region . V. , X , and j have to be measured in V , V / cm and A / cm2 , respectively . MacKeowns formula is based on the assump- tion that electrons and ions move inertia - limited under the influence of their own space - charge ...
Page 117
... charge region conditions of the type ( bß ) . Because of the thermal motion , ions and electrons leave the discharge zone . In a stationary state the loss of ions and electrons must be equal . For this a radial potential fall V is ...
... charge region conditions of the type ( bß ) . Because of the thermal motion , ions and electrons leave the discharge zone . In a stationary state the loss of ions and electrons must be equal . For this a radial potential fall V is ...
Page 183
... charge equal to en per unit area , where no is the equilibrium ( uniform ) number density of electrons . Here and ... charge to either side of the electron sheet due to the electron gas is unchanged , so that the electric field now ...
... charge equal to en per unit area , where no is the equilibrium ( uniform ) number density of electrons . Here and ... charge to either side of the electron sheet due to the electron gas is unchanged , so that the electric field now ...
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