Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 20
... result by considering a Lorentz gas ( in which I ( __ ) = 0 ) , which may be solved exactly , and claim 10 % accuracy for all results . The results of these rather elaborate calculations differ from the m.f. time 0/00 2.4 01100 ( R and ...
... result by considering a Lorentz gas ( in which I ( __ ) = 0 ) , which may be solved exactly , and claim 10 % accuracy for all results . The results of these rather elaborate calculations differ from the m.f. time 0/00 2.4 01100 ( R and ...
Page 111
... results show deviations from the experimental data which are outside of the uncertainties of the parameters and the ... result means that the extension of the space - charge region is not identical with the extension of the inertia ...
... results show deviations from the experimental data which are outside of the uncertainties of the parameters and the ... result means that the extension of the space - charge region is not identical with the extension of the inertia ...
Page 135
... results as for v = 0 but remarkable quantitative differences . This can be seen from Fig . 24 where we have plotted the critical field vs. pressure for three values of v . Particularly noteworthy is the difference between the results ...
... results as for v = 0 but remarkable quantitative differences . This can be seen from Fig . 24 where we have plotted the critical field vs. pressure for three values of v . Particularly noteworthy is the difference between the results ...
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