Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 112
... temperature T .. For the following more precise evaluations we have to define the temperature at the end of the contraction region T , and the temperature T , of the cathode from the energy balance . This can be done as follows . BC If ...
... temperature T .. For the following more precise evaluations we have to define the temperature at the end of the contraction region T , and the temperature T , of the cathode from the energy balance . This can be done as follows . BC If ...
Page 113
... temperature T. ( R ) is shown in Fig . 9 for various currents J and gas temperatures T. The depen- dence of the temperature T. on the par- ameter R / R is open to a physical inter- pretation on the basis of heat - conduction and ...
... temperature T. ( R ) is shown in Fig . 9 for various currents J and gas temperatures T. The depen- dence of the temperature T. on the par- ameter R / R is open to a physical inter- pretation on the basis of heat - conduction and ...
Page 131
... temperature . Here the temperature of the particles is not governed by the ener- gy gain in a homogeneous electrical field and an ener- gy loss due to collisions with uniformly distributed balance . We omit the de- tails of this ...
... temperature . Here the temperature of the particles is not governed by the ener- gy gain in a homogeneous electrical field and an ener- gy loss due to collisions with uniformly distributed balance . We omit the de- tails of this ...
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