Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 13
... collision in order to discover the value of v , v ' . On a collision , the 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 ...
... collision in order to discover the value of v , v ' . On a collision , the 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 ...
Page 110
... collision - free description is possible . The cases are : ( ax ) one - dimensional collision - free motion ; ( ap ) one - dimensional motion with collision ; ( ba ) multi - dimensional problem with collisions ; ( b ) multi ...
... collision - free description is possible . The cases are : ( ax ) one - dimensional collision - free motion ; ( ap ) one - dimensional motion with collision ; ( ba ) multi - dimensional problem with collisions ; ( b ) multi ...
Page 122
... collision frequency ( 4.6 ) vi ( ci ) = - cos x ) d2 , ( 2 ) where is the deflection angle in the laboratory system . We see that for the X collision integral simple expressions in terms of the current density occur only if we can ...
... collision frequency ( 4.6 ) vi ( ci ) = - cos x ) d2 , ( 2 ) where is the deflection angle in the laboratory system . We see that for the X collision integral simple expressions in terms of the current density occur only if we can ...
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