Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 53
... cross- section 87 ( e2 / mc2 ) 2 ~ 10-25 cm2 which determines the scale of the phenomenon . If because of an instability An ( w , k ) becomes very large for some narrow range of o , k a much more spectacular effect would be expected ...
... cross- section 87 ( e2 / mc2 ) 2 ~ 10-25 cm2 which determines the scale of the phenomenon . If because of an instability An ( w , k ) becomes very large for some narrow range of o , k a much more spectacular effect would be expected ...
Page 117
... cross - section of the discharge , as can be seen from the evaluation of the space - charge problem . We ... transverse magnetic field . For a description of the ion motion we use the Lorentz equations ant at + √ ( n + v + ) = 0 , v . B ...
... cross - section of the discharge , as can be seen from the evaluation of the space - charge problem . We ... transverse magnetic field . For a description of the ion motion we use the Lorentz equations ant at + √ ( n + v + ) = 0 , v . B ...
Page 241
... section is determined by the probe's cross- section ( which we take to be circular ) . A diffusion process -- whose nature we need not specify here - exchanges continuously particles between the interior of the tube and the rest of the ...
... section is determined by the probe's cross- section ( which we take to be circular ) . A diffusion process -- whose nature we need not specify here - exchanges continuously particles between the interior of the tube and the rest of the ...
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