Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 82
... constant of the motion . Also the coefficient of aƒ / Ət vanishes if and dy / êt vanish which corresponds to the fact that for x = 0 E ° = 0 ) and E constant , ɛ is a constant of the motion . These facts may be derived directly from eq ...
... constant of the motion . Also the coefficient of aƒ / Ət vanishes if and dy / êt vanish which corresponds to the fact that for x = 0 E ° = 0 ) and E constant , ɛ is a constant of the motion . These facts may be derived directly from eq ...
Page 87
... constant . We consider only those perturbation which have the same value of u as the equilibrium for any choice of G ... constant by means of the equations of Section 3'3 Expanding it to second order in 4 , we get U = = A ( A ) + B ( Å ) ...
... constant . We consider only those perturbation which have the same value of u as the equilibrium for any choice of G ... constant by means of the equations of Section 3'3 Expanding it to second order in 4 , we get U = = A ( A ) + B ( Å ) ...
Page 254
... 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 but is nearly so if the ...
... 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 but is nearly so if 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 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