Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 38
Page 35
... hence ɛ is complex . In normal systems an imaginary part to ɛ represents the loss due to collisions , here the loss process is Landau damping . The field at a charge e , introduced by its own presence is ( III.3.9 ) E ( vt , t ) = Re ...
... hence ɛ is complex . In normal systems an imaginary part to ɛ represents the loss due to collisions , here the loss process is Landau damping . The field at a charge e , introduced by its own presence is ( III.3.9 ) E ( vt , t ) = Re ...
Page 138
... Hence , such instabilities do not remain for long in the exponentially growing phase . We would not expect then that these micro- instabilities would lead to a gross disassembly of the plasma such as occurs for example in the ...
... Hence , such instabilities do not remain for long in the exponentially growing phase . We would not expect then that these micro- instabilities would lead to a gross disassembly of the plasma such as occurs for example in the ...
Page 184
... Hence if W ( ) is everywhere less than o initially , it is always everywhere less than 3 , and hence ( 2.6 ) is always satisfied everywhere . We may carry out a similar analysis for cylindrical oscillations . If the electrons initially ...
... Hence if W ( ) is everywhere less than o initially , it is always everywhere less than 3 , and hence ( 2.6 ) is always satisfied everywhere . We may carry out a similar analysis for cylindrical oscillations . If the electrons initially ...
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