Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 12
... centre of mass of the total system does not coincide with the centre of mass of either component , and ( 2 ) because trajectories are curved by the magnetic field , the transport processes are considerably complicated ; the heat flux 12 ...
... centre of mass of the total system does not coincide with the centre of mass of either component , and ( 2 ) because trajectories are curved by the magnetic field , the transport processes are considerably complicated ; the heat flux 12 ...
Page 13
... centre - of - mass motion is constant ; i.e. ( II.3.2 ) V = M1 V1 + M2 V 2 m1 + m2 = M 1 v 1 + M 2 v 2 m1 + m2 and on removing this , the collision is described as the motion of a particle of the reduced mass m1m2 / ( m1 + ma ) , moving ...
... centre - of - mass motion is constant ; i.e. ( II.3.2 ) V = M1 V1 + M2 V 2 m1 + m2 = M 1 v 1 + M 2 v 2 m1 + m2 and on removing this , the collision is described as the motion of a particle of the reduced mass m1m2 / ( m1 + ma ) , moving ...
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