Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 86
... definition for y * we may write the two second - order equa- tions as ( 78 ) - = F ( § , } ) , J ( § , } ) , and ... define our perturbations to higher order ( as in the fluid theory ) we define ( 79 ) દ at a ( r + E , t ) , so is the ...
... definition for y * we may write the two second - order equa- tions as ( 78 ) - = F ( § , } ) , J ( § , } ) , and ... define our perturbations to higher order ( as in the fluid theory ) we define ( 79 ) દ at a ( r + E , t ) , so is the ...
Page 99
... definition . It is indeed very difficult to assign a group of necessary and sufficient characteristics to the glow ... definitions : a glow discharge is a self - sustained conducting gas region between two electrodes . In the column the ...
... definition . It is indeed very difficult to assign a group of necessary and sufficient characteristics to the glow ... definitions : a glow discharge is a self - sustained conducting gas region between two electrodes . In the column the ...
Page 239
... definition and its explicit calculation : and assume a discontinuous transition between the sheath and the rest of ... defined and conveniently used in the calculation BOUNDARY LAYER PROBLEMS IN PLASMA PHYSICS 239.
... definition and its explicit calculation : and assume a discontinuous transition between the sheath and the rest of ... defined and conveniently used in the calculation BOUNDARY LAYER PROBLEMS IN PLASMA PHYSICS 239.
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