Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 5
... angle af at int - fanfange = d3v2go ( g , 0 ) [ ƒ ( v1 ) ƒ ( V2 ) — ƒ ( v1 ) f ( V2 ) ] , where 1 , 2 are related to v1 , v2 and 0 , being in fact the negatives of the veloc- ities resulting when a collision between v1 and v2 occurs ...
... angle af at int - fanfange = d3v2go ( g , 0 ) [ ƒ ( v1 ) ƒ ( V2 ) — ƒ ( v1 ) f ( V2 ) ] , where 1 , 2 are related to v1 , v2 and 0 , being in fact the negatives of the veloc- ities resulting when a collision between v1 and v2 occurs ...
Page 24
... angle scattering , which dominates the collision process . Having done this we are free to discuss the effect of long - range correlations on the small - angle scattering and to develop forms for the transport equation which are valid ...
... angle scattering , which dominates the collision process . Having done this we are free to discuss the effect of long - range correlations on the small - angle scattering and to develop forms for the transport equation which are valid ...
Page 102
... angle . Solid angle of the scattering parameters . Identity tensor . Instability parameter . 3 . - Electrode components of the arc discharge . Fifty years of intensive experimental research have produced a vast amount of experimental ...
... angle . Solid angle of the scattering parameters . Identity tensor . Instability parameter . 3 . - Electrode components of the arc discharge . Fifty years of intensive experimental research have produced a vast amount of experimental ...
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