Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 98
... discharge where we have several interacting model regions governed by a large number of essentially different physical laws . Just for this reason most calculations in gas discharge theory are extremely cumbersone . Therefore in this ...
... discharge where we have several interacting model regions governed by a large number of essentially different physical laws . Just for this reason most calculations in gas discharge theory are extremely cumbersone . Therefore in this ...
Page 99
... discharge which consists of a cylindrical plasma column and the typical cathodic parts of the glow . In these ... discharge . Here with increasing current the voltage does not change , but the area covered by the discharge increases with ...
... discharge which consists of a cylindrical plasma column and the typical cathodic parts of the glow . In these ... discharge . Here with increasing current the voltage does not change , but the area covered by the discharge increases with ...
Page 117
... discharge . This last discussion leads us to our final question 9 ) related to the « problem of retrograde motion » . The reason is that a critical discussion ( * ) of all pos- sible contraction types shows that retrograde motion can be ...
... discharge . This last discussion leads us to our final question 9 ) related to the « problem of retrograde motion » . The reason is that a critical discussion ( * ) of all pos- sible contraction types shows that retrograde motion can be ...
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