Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
From inside the book
Results 1-3 of 23
Page 57
... corresponds to very large 7 which seems to contradict our previous assumption . However , in this case , o large ... corresponds to the neglect of displacement current and the electric force term in the momentum eq . ( 2 ) . Also we wish ...
... corresponds to very large 7 which seems to contradict our previous assumption . However , in this case , o large ... corresponds to the neglect of displacement current and the electric force term in the momentum eq . ( 2 ) . Also we wish ...
Page 170
... corresponds to large nega- tive 4 ' , we find that the eigenvalues 4 lie slightly below the points 1 , 3 , 2 , For the fastest growing mode , which corresponds to a solution U that is basically symmetric near μo , we have 4. As we move ...
... corresponds to large nega- tive 4 ' , we find that the eigenvalues 4 lie slightly below the points 1 , 3 , 2 , For the fastest growing mode , which corresponds to a solution U that is basically symmetric near μo , we have 4. As we move ...
Page 179
... corresponds to the limit of high conduc- tivity ) . The case treated in ref . [ 4 ] corresponds to the opposite limit , N → 0 . To obtain a comparison , we may make use of the low - conductivity result , derived in Appendix B of ref ...
... corresponds to the limit of high conduc- tivity ) . The case treated in ref . [ 4 ] corresponds to the opposite limit , N → 0 . To obtain a comparison , we may make use of the low - conductivity result , derived in Appendix B of ref ...
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 electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ k₂ KRUSKAL KULSRUD l'axe magnétique limit lowest order m₁ magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle perturbation Phys plasma oscillations plasma physics Poisson's equation potential problem quantities R₁ radial region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity voisinage waves in plasmas zero zero-order Απ