Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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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 af ( IV.1.1 ) at af ...
... 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 af ( IV.1.1 ) at af ...
Page 148
... magnetic field . In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency in a tepid C's plasma when the electron drift velocity parallel to the magnetic field exceeds about three ...
... magnetic field . In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency in a tepid C's 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 ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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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