Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 109
... question of current continuity is less problematic and interesting . Further a considerable simplification arises from the lack of any emission process at the anode if we disregard , for the time being , the Beck - arc . Thus the ...
... question of current continuity is less problematic and interesting . Further a considerable simplification arises from the lack of any emission process at the anode if we disregard , for the time being , the Beck - arc . Thus the ...
Page 113
... question of charge conservation . For this purpose we plot the diagram showing on the one hand the ion saturation ... questions 3 ) -8 ) : Answ . 3 ) The arc must contract in front of the cathode since otherwise the laws of ...
... question of charge conservation . For this purpose we plot the diagram showing on the one hand the ion saturation ... questions 3 ) -8 ) : Answ . 3 ) The arc must contract in front of the cathode since otherwise the laws of ...
Page 119
... questions which we used to characterize the are elec- trode problem . It was es- sential that we restricted Vr ( m / s ) Vr ( m / s ) 125 175 100 75 50 a ) 25 0 2000 4000 6000 8000 10000 12000 B ( G ) 8 7 5 ง 0 Fig . 15 . J = 2A D 2000 ...
... questions which we used to characterize the are elec- trode problem . It was es- sential that we restricted Vr ( m / s ) Vr ( m / s ) 125 175 100 75 50 a ) 25 0 2000 4000 6000 8000 10000 12000 B ( G ) 8 7 5 ง 0 Fig . 15 . J = 2A D 2000 ...
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