Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 21
Page 159
Instabilities due to Finite Resistivity or Finite Current - Carrier Mass . H. P. FURTH Lawrence Radiation Laboratory Livermore , Cal . This lecture series will be composed of two parts . Part A ... finite resistivity or finite current-
Instabilities due to Finite Resistivity or Finite Current - Carrier Mass . H. P. FURTH Lawrence Radiation Laboratory Livermore , Cal . This lecture series will be composed of two parts . Part A ... finite resistivity or finite current-
Page 160
... finite - conductivity region . In Section 5 , we find solutions for the finite - conductivity region , which , combined with the boundary condi- tions , give us an eigenvalue relation that determines the instability growth rates ...
... finite - conductivity region . In Section 5 , we find solutions for the finite - conductivity region , which , combined with the boundary condi- tions , give us an eigenvalue relation that determines the instability growth rates ...
Page 163
... finite shear , we may choose k so that k BF passes through a null . The typical u - dependence of F and n that will be considered here is illustrated in Fig . 1a . F ~ k Bo ñ B10 B ... FINITE RESISTIVITY OR FINITE CURRENT - CARRIER MASS 163.
... finite shear , we may choose k so that k BF passes through a null . The typical u - dependence of F and n that will be considered here is illustrated in Fig . 1a . F ~ k Bo ñ B10 B ... FINITE RESISTIVITY OR FINITE CURRENT - CARRIER MASS 163.
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
3 other sections not shown
Other editions - View all
Common terms and phrases
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