Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 63
... exists for computing on's . Consider λ = − 1 √5 · F ( § ) dr 2 δλ = 85 · ( F ( E ) + λgg ) dr ρξε ατ 820 for all 8 is equivalent to 2 , 9 = for some n . A minimum of 2 gives the most unstable » En . If 2 is always positive o is always ...
... exists for computing on's . Consider λ = − 1 √5 · F ( § ) dr 2 δλ = 85 · ( F ( E ) + λgg ) dr ρξε ατ 820 for all 8 is equivalent to 2 , 9 = for some n . A minimum of 2 gives the most unstable » En . If 2 is always positive o is always ...
Page 103
... exist under certain experimental conditions or can exist only if certain favourable surface conditions are present ? 9 ) Is there a reason why the arc exhibits retrograde motion in a trans- verse magnetic field ? - 31. Current ...
... exist under certain experimental conditions or can exist only if certain favourable surface conditions are present ? 9 ) Is there a reason why the arc exhibits retrograde motion in a trans- verse magnetic field ? - 31. Current ...
Page 163
... exist at all for S∞ . The situation is similar to that for hydrodynamic sher - flow stability at high Reynolds number . In the incompressible case , we can show that no overstable modes exist at all , provided that nonequilibrium zero ...
... exist at all for S∞ . The situation is similar to that for hydrodynamic sher - flow stability at high Reynolds number . In the incompressible case , we can show that no overstable modes exist at all , provided that nonequilibrium zero ...
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