Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 102
... rule . From this experimental knowledge we formulate our theoretical problem in the following set of questions : 1 ) As is obvious from Fig . 2 a very large production of electrons and ions is required in the small cathode onset area ...
... rule . From this experimental knowledge we formulate our theoretical problem in the following set of questions : 1 ) As is obvious from Fig . 2 a very large production of electrons and ions is required in the small cathode onset area ...
Page 189
... rule ( 4.9 ) k1 + k2 = k ̧ + k ̧ · 3 If any one such interaction is considered independently of the rest , it is found that energy is exchanged between such a group according to the relations ( 4.10 ) dɛ ( k1 ) dt dε ( k2 ) dt = dε ( kз ) ...
... rule ( 4.9 ) k1 + k2 = k ̧ + k ̧ · 3 If any one such interaction is considered independently of the rest , it is found that energy is exchanged between such a group according to the relations ( 4.10 ) dɛ ( k1 ) dt dε ( k2 ) dt = dε ( kз ) ...
Page 195
... rules of the type ( 4.9 ) and ( 5.4 ) , and it also leads to relations such as ( 4.10 ) and ( 5.8 ) governing the exchange of energy between waves . One might expect energy and momentum to be separately conserved in an interacting group ...
... rules of the type ( 4.9 ) and ( 5.4 ) , and it also leads to relations such as ( 4.10 ) and ( 5.8 ) governing the exchange of energy between waves . One might expect energy and momentum to be separately conserved in an interacting group ...
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