Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 165
... vanish at μ = μ1 , μ2 , the external boundaries . These solutions cannot , in general , be joined without a discontinuity in y ' , ( 21 ) 4 ' ψε ψί Ψί 9 Y2 Y1 where the subscripts refer to values on either side of the point of juncture ...
... vanish at μ = μ1 , μ2 , the external boundaries . These solutions cannot , in general , be joined without a discontinuity in y ' , ( 21 ) 4 ' ψε ψί Ψί 9 Y2 Y1 where the subscripts refer to values on either side of the point of juncture ...
Page 254
... vanish more rapidly than any power of the parameter of smallness , i.e. , the relative change of the field over the Larmor radius . This does not imply that it must be a rigorous constant . For instance , Ac = exp [ -1/2 ] has this ...
... vanish more rapidly than any power of the parameter of smallness , i.e. , the relative change of the field over the Larmor radius . This does not imply that it must be a rigorous constant . For instance , Ac = exp [ -1/2 ] has this ...
Page 264
... vanish and the invariant is just R12 | B | . ɛ . 1 The method of proof was suggested by Kulsrud's proof of an analogous statement for the harmonic oscillator [ 3 ] . If in ( 2 ) we replace the bracketed exponent by ni0 and specify that ...
... vanish and the invariant is just R12 | B | . ɛ . 1 The method of proof was suggested by Kulsrud's proof of an analogous statement for the harmonic oscillator [ 3 ] . If in ( 2 ) we replace the bracketed exponent by ni0 and specify that ...
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