Advanced Plasma TheoryM. N. Rosenbluth |
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Page 65
... self - adjoint , since it is symmetric . Our theory corresponds to a continuum of dimensions but is otherwise algebraically the same . The proof of d ) follows the remarks in c ) with SW given by ( 20 ) . We make some moré remarks on d ...
... self - adjoint , since it is symmetric . Our theory corresponds to a continuum of dimensions but is otherwise algebraically the same . The proof of d ) follows the remarks in c ) with SW given by ( 20 ) . We make some moré remarks on d ...
Page 67
... self- adjointness . If SW < 0 for this need not imply instability in a general case since need not be a normal mode ... self - adjointness for the energy principle to work both ways . 25. Proof of self - adjointness of F. of F one direct ...
... self- adjointness . If SW < 0 for this need not imply instability in a general case since need not be a normal mode ... self - adjointness for the energy principle to work both ways . 25. Proof of self - adjointness of F. of F one direct ...
Page 86
... self - adjointness . This self - adjointness was first discovered by NEWCOMB [ 15 ] who gave a direct proof of it . In these notes we follow the indirect method of the fluid theory in finding and de- monstrating this self - adjointness ...
... self - adjointness . This self - adjointness was first discovered by NEWCOMB [ 15 ] who gave a direct proof of it . In these notes we follow the indirect method of the fluid theory in finding and de- monstrating this self - adjointness ...
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