Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 124
... electron temperature and the X = E - field of the column . Otherwise the relations ( 4.14 ) may be disregarded ... electron production can be given in the form ( 4.20 ) A2 = an ̧ + Sn ̧n- ßn ̧ , where the first term describes electron ...
... electron temperature and the X = E - field of the column . Otherwise the relations ( 4.14 ) may be disregarded ... electron production can be given in the form ( 4.20 ) A2 = an ̧ + Sn ̧n- ßn ̧ , where the first term describes electron ...
Page 183
... electron sheet due to the electron gas is unchanged , so that the electric field now experienced by the electron sheet is due to the excess positive charge , and is therefore given by ( 2.2 ) E = 4леn . The equation of motion of the ...
... electron sheet due to the electron gas is unchanged , so that the electric field now experienced by the electron sheet is due to the excess positive charge , and is therefore given by ( 2.2 ) E = 4леn . The equation of motion of the ...
Page 198
... electron which , in the quiescent state of the electron gas , is at position a ,. The quie- scent state is that in which electrons are uniformly distributed and are at rest . If we describe the electrostatic interaction between ...
... electron which , in the quiescent state of the electron gas , is at position a ,. The quie- scent state is that in which electrons are uniformly distributed and are at rest . If we describe the electrostatic interaction between ...
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