Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 17
... consider a pair of equations ( II.4.5 ) A partial integration shows ( II.4.6 ) Now consider ( II.4.7 ) If X1 a y ( c ) = w $ 2 ( c ) + Kp1 ( c ) a W $ 1 ( c ) = Kp2 ( c ) . ( X1 , 69 ) a X2 X2 , W Χι 2.1 ( X1 , 4 ) 2 X2 / T4 ) 2 / ( X2 ...
... consider a pair of equations ( II.4.5 ) A partial integration shows ( II.4.6 ) Now consider ( II.4.7 ) If X1 a y ( c ) = w $ 2 ( c ) + Kp1 ( c ) a W $ 1 ( c ) = Kp2 ( c ) . ( X1 , 69 ) a X2 X2 , W Χι 2.1 ( X1 , 4 ) 2 X2 / T4 ) 2 / ( X2 ...
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 uniform infinite plasma , which may contain a static uniform magnetic field , and in which the ... consider a generalized entropy ( 1.1 ) S d3x d3v , x = faaxar , where G is any functional of ƒ like f In f . Let us compare S ...
... Consider a uniform infinite plasma , which may contain a static uniform magnetic field , and in which the ... consider a generalized entropy ( 1.1 ) S d3x d3v , x = faaxar , where G is any functional of ƒ like f In f . Let us compare S ...
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