Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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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 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 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 ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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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 electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function 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 region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ