Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 39
... magnetic field . As in the absence of a magnetic field , it is possible to use the Liouville equation to describe the dynamics of a complete system , and again one may integrate this to obtain the Boltzmann equation of af e ( IV.1.1 ) ...
... magnetic field . As in the absence of a magnetic field , it is possible to use the Liouville equation to describe the dynamics of a complete system , and again one may integrate this to obtain the Boltzmann equation of af e ( IV.1.1 ) ...
Page 148
... magnetic field . e ཀ In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency in a tepid Cs plasma when the electron drift velocity parallel to the magnetic field exceeds about three ...
... magnetic field . e ཀ In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency in a tepid Cs plasma when the electron drift velocity parallel to the magnetic field exceeds about three ...
Page 254
... magnetic field remains constant . Combined with the conservation of energy this enables one to show that a magnetic field can reflect such a spiraling particle . The magnetic moment of this patricle is not really a rigo- rous constant ...
... magnetic field remains constant . Combined with the conservation of energy this enables one to show that a magnetic field can reflect such a spiraling particle . The magnetic moment of this patricle is not really a rigo- rous constant ...
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