Advanced Plasma TheoryM. N. Rosenbluth |
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Page 17
... consider ( II.4.3 ) 2 ( x ) = ( x , y ) 3 / ( x , Kx ) · If now , we insist that 2 be stationary with respect to zx ... consider a pair of equations ( II.4.5 ) A partial integration shows ( II.4.6 ) Now consider ( II.4.7 ) 21 - a y ( c ) ...
... consider ( II.4.3 ) 2 ( x ) = ( x , y ) 3 / ( x , Kx ) · If now , we insist that 2 be stationary with respect to zx ... consider a pair of equations ( II.4.5 ) A partial integration shows ( II.4.6 ) Now consider ( II.4.7 ) 21 - a y ( c ) ...
Page 97
... consider electrons , ions and neutral particles . But already the number of particle components may be larger . Multiply charged positive and negative ions can influence the behaviour of our system . More important we consider the ...
... consider electrons , ions and neutral particles . But already the number of particle components may be larger . Multiply charged positive and negative ions can influence the behaviour of our system . More important we consider the ...
Page 138
... consider a generalized entropy ( 1.1 ) S d3x d3v , where G is any functional of ƒ like f In f . Let us compare S ( t1 ) and S ( t2 ) where t1 and t are two different times in the course of the motion . Consider an element of phase ...
... consider a generalized entropy ( 1.1 ) S d3x d3v , where G is any functional of ƒ like f In f . Let us compare S ( t1 ) and S ( t2 ) where t1 and t are two different times in the course of the motion . Consider an element of phase ...
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