Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 26
... parameter b : indeed , using the impulse approximation sin 0 Vo = F , dt 1 dx + Sp1 at = + Sp . dr = Vo 1 .2 = e2 b dx - de m , vz S 2 ( x2 + b2 ) 1 e2 dt 2e2 = bm , v3 ( 1 + 12 ) 1 bm , r 21 0 ... sin ༤༡ sin0 ~ € 2 bm , vå 88 To ...
... parameter b : indeed , using the impulse approximation sin 0 Vo = F , dt 1 dx + Sp1 at = + Sp . dr = Vo 1 .2 = e2 b dx - de m , vz S 2 ( x2 + b2 ) 1 e2 dt 2e2 = bm , v3 ( 1 + 12 ) 1 bm , r 21 0 ... sin ༤༡ sin0 ~ € 2 bm , vå 88 To ...
Page 102
6 , Interaction parameters of positive ions with electrons . Q x Ω 91018 Scattering function . Scattering angle . Solid angle of the scattering parameters . Identity tensor . Instability parameter . 3 . - Electrode components of the arc ...
6 , Interaction parameters of positive ions with electrons . Q x Ω 91018 Scattering function . Scattering angle . Solid angle of the scattering parameters . Identity tensor . Instability parameter . 3 . - Electrode components of the arc ...
Page 254
... parameter approaches zero or infinity is an adia- batic invariant . For instance , in Fermi's theory [ 1 ] for the acceleration of cosmic rays , it is assumed that the magnetic moment of a spiraling particle in a varying magnetic field ...
... parameter approaches zero or infinity is an adia- batic invariant . For instance , in Fermi's theory [ 1 ] for the acceleration of cosmic rays , it is assumed that the magnetic moment of a spiraling particle in a varying magnetic field ...
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