Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 16
... integral operator I is invariant under rotation the spherical harmonics are eigen - functions thereof and I ( $ TN ) = KTN = 2 ( c2 ) pTN , where 2 is a function ( unknown ! ) of c2 ; and K is an integral operator acting on the ...
... integral operator I is invariant under rotation the spherical harmonics are eigen - functions thereof and I ( $ TN ) = KTN = 2 ( c2 ) pTN , where 2 is a function ( unknown ! ) of c2 ; and K is an integral operator acting on the ...
Page 25
... integral for an ionized gas of like par- ticles ( for the moment ) . Using e 2 -4 σ = OR - g sin 9 where gv - v ... integral ( III.1.1 ) and if the series is cut off at the second term , the expansion ( III.1.2 ) used for Ag and the ...
... integral for an ionized gas of like par- ticles ( for the moment ) . Using e 2 -4 σ = OR - g sin 9 where gv - v ... integral ( III.1.1 ) and if the series is cut off at the second term , the expansion ( III.1.2 ) used for Ag and the ...
Page 147
... integral appearing in ( 3 ) is thus where ( 2.10 ) 0 exp [ pt ] exp [ ik Z ] exp [ ik_y ] dτ , Jexp [ p z = v2t y ... integral indicated above as well as the integral over all velocities . Thus we have to do the integrals fr . dr . fde ...
... integral appearing in ( 3 ) is thus where ( 2.10 ) 0 exp [ pt ] exp [ ik Z ] exp [ ik_y ] dτ , Jexp [ p z = v2t y ... integral indicated above as well as the integral over all velocities . Thus we have to do the integrals fr . dr . fde ...
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