Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 37
... approximation . The integrals required to evaluate the D , take the form fdgfdok dok d ( k · g ) k • — , f ( v + g ) , from ( III.3.10 ) d ( w + k.v ) . \ k2 ε ( k , w ) | 2 from ( III.3.13 ) fagf d3k do kk d ( w + k.v ) | k2 ɛ ( k , w ) ...
... approximation . The integrals required to evaluate the D , take the form fdgfdok dok d ( k · g ) k • — , f ( v + g ) , from ( III.3.10 ) d ( w + k.v ) . \ k2 ε ( k , w ) | 2 from ( III.3.13 ) fagf d3k do kk d ( w + k.v ) | k2 ɛ ( k , w ) ...
Page 38
... approximation to a kinetic equation which includes both the static correlation effects which produce screening with the dynamic effects that represent the production of plasma oscillations . It is of particular interest to observe that ...
... approximation to a kinetic equation which includes both the static correlation effects which produce screening with the dynamic effects that represent the production of plasma oscillations . It is of particular interest to observe that ...
Page 182
... approximation , we may still represent what goes on in a plasma instantaneously in terms of these waves , but we must allow for coupling between them so that the presence of one wave affects the dispersion relation of another , and ...
... approximation , we may still represent what goes on in a plasma instantaneously in terms of these waves , but we must allow for coupling between them so that the presence of one wave affects the dispersion relation of another , and ...
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