Advanced Plasma TheoryM. N. Rosenbluth |
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Page 142
... instability of superposed fluids . Let us now briefly discuss what happens if the two streams instead of being d - functions possess some thermal spread as shown in the diagram . th -V V th Fig . 2 . Then , we would expect that the ...
... instability of superposed fluids . Let us now briefly discuss what happens if the two streams instead of being d - functions possess some thermal spread as shown in the diagram . th -V V th Fig . 2 . Then , we would expect that the ...
Page 148
... instabilities . -- 3. We discuss next another version of the two - stream instability appro- priate to the magnetic field . e In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency ...
... instabilities . -- 3. We discuss next another version of the two - stream instability appro- priate to the magnetic field . e In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency ...
Page 159
... instabilities due to finite resistivity and instabilities of the collisionless sheet - pinch type , which may be said to be due to the finite mass of the current carriers . In both cases the instability depends on E ÷ v × B 0. In the ...
... instabilities due to finite resistivity and instabilities of the collisionless sheet - pinch type , which may be said to be due to the finite mass of the current carriers . In both cases the instability depends on E ÷ v × B 0. In the ...
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 KRUSKAL KULSRUD l'axe magnétique limit 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 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