Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 112
... effective energy supply from the end of the contraction zone to the electrode then this is a function of T. , T. and R ; e.g. II ( T . , T. , R ) . This energy supply must be compensated by a corresponding loss L of the electrode ...
... effective energy supply from the end of the contraction zone to the electrode then this is a function of T. , T. and R ; e.g. II ( T . , T. , R ) . This energy supply must be compensated by a corresponding loss L of the electrode ...
Page 130
... current continuity equation ( 4.37 ) d dr Toro B2 ( Te 1 n — [ n ( T + + T2 ) ] = — Nok Tol r where the index ( 0 ) designates quantities at the edge ( r ) of the effective particle source . 1 Гого 10 * = 1123 52 € 878 = 130 G. ECKER.
... current continuity equation ( 4.37 ) d dr Toro B2 ( Te 1 n — [ n ( T + + T2 ) ] = — Nok Tol r where the index ( 0 ) designates quantities at the edge ( r ) of the effective particle source . 1 Гого 10 * = 1123 52 € 878 = 130 G. ECKER.
Page 161
... effective mass density and thus decreases the growth rates somewhat ) . 4 ) Perturbations in plasma resistivity are assumed to result only from convection , ( 5 ) an at + v⋅ √n = 0 . The neglect of thermal conductivity along magnetic ...
... effective mass density and thus decreases the growth rates somewhat ) . 4 ) Perturbations in plasma resistivity are assumed to result only from convection , ( 5 ) an at + v⋅ √n = 0 . The neglect of thermal conductivity along magnetic ...
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