Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 21
... solution some other approaches have been used . One , due to Rosenbluth and Kaufmann , alters the ordering of the ... solution f , but the value of the moments c , cc , ce2 which have hydrodynamic significance , and further , that what ...
... solution some other approaches have been used . One , due to Rosenbluth and Kaufmann , alters the ordering of the ... solution f , but the value of the moments c , cc , ce2 which have hydrodynamic significance , and further , that what ...
Page 62
... solution to get a more complete solution in an obvious way . ) If all o , are real is bounded . If any o is complex w , or O has a negative imaginary part and is generally unbounded if a , 0 , = { m gives an unstable perturbation . Thus ...
... solution to get a more complete solution in an obvious way . ) If all o , are real is bounded . If any o is complex w , or O has a negative imaginary part and is generally unbounded if a , 0 , = { m gives an unstable perturbation . Thus ...
Page 165
... solution therefore consists in solv- ing for and W in a small region R , about the point F = 0 , with the boun- dary conditions that y ' / p matches the solutions of eq . ( 20 ) , and that Wis well behaved outside the region R 。. In ...
... solution therefore consists in solv- ing for and W in a small region R , about the point F = 0 , with the boun- dary conditions that y ' / p matches the solutions of eq . ( 20 ) , and that Wis well behaved outside the region R 。. In ...
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