Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 114
tion , R. Therefore the contraction is not the result of a minimum principle , but an essential physical necessity to satisfy the laws of nature . Generally the E - diagram can show up to four E - points . Which one of the several ...
tion , R. Therefore the contraction is not the result of a minimum principle , but an essential physical necessity to satisfy the laws of nature . Generally the E - diagram can show up to four E - points . Which one of the several ...
Page 117
... tion q≫ 1. However , under this condition the mechanism of T - F or I - F - field electron emission leads to difficulties . Only if the conditions of the surface favour the process of emission is there any hope of igniting the arc with ...
... tion q≫ 1. However , under this condition the mechanism of T - F or I - F - field electron emission leads to difficulties . Only if the conditions of the surface favour the process of emission is there any hope of igniting the arc with ...
Page 261
... tion and hence a large velocity ( of order 1 / ɛ ) . This would contradict the con- dition that the fields seen by the particle be nearly constant during one gyra- tion period . Only the components of R , orthogonal to B are determined ...
... tion and hence a large velocity ( of order 1 / ɛ ) . This would contradict the con- dition that the fields seen by the particle be nearly constant during one gyra- tion period . Only the components of R , orthogonal to B are determined ...
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