Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 108
... contraction region ( s ) . To find the particle density ( n ) , and the average velocity ( c + ) , it is necessary to know the tem- perature close to the boundary ( s ) of the contraction region . This in turn requires the evaluation of ...
... contraction region ( s ) . To find the particle density ( n ) , and the average velocity ( c + ) , it is necessary to know the tem- perature close to the boundary ( s ) of the contraction region . This in turn requires the evaluation of ...
Page 112
We claim that the contraction itself and the extension of the contraction follows simply from the application of the physical laws of electrodynamics , statistical mechanics and quantum mechanics to our problem . + To prove this ...
We claim that the contraction itself and the extension of the contraction follows simply from the application of the physical laws of electrodynamics , statistical mechanics and quantum mechanics to our problem . + To prove this ...
Page 115
... contraction ( Ro / R ≈ 1 ) . In addition we have only one other E - point which belongs to extreme contraction . The point with very little contraction ( 01 ) is generally favoured by the minimum principle . Thus the weaker contraction ...
... contraction ( Ro / R ≈ 1 ) . In addition we have only one other E - point which belongs to extreme contraction . The point with very little contraction ( 01 ) is generally favoured by the minimum principle . Thus the weaker contraction ...
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