Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 43
... orbits instead of straight lines ; and the dielectric coefficient becomes compli- cated by the presence of the magnetic field . 2. The dielectric coefficient of a magnetized plasma . - We will require the field induced in a plasma by ...
... orbits instead of straight lines ; and the dielectric coefficient becomes compli- cated by the presence of the magnetic field . 2. The dielectric coefficient of a magnetized plasma . - We will require the field induced in a plasma by ...
Page 147
... orbits in the constant magnetic field . We take B along the z axis and k in the ( y , z ) plane . The orbit integral appearing in ( 3 ) is thus where ( 2.10 ) 0 exp [ pt ] exp [ ik Z ] exp [ ik_y ] dτ , Jexp [ p z = v2t y [ sin ( 2 + ) ...
... orbits in the constant magnetic field . We take B along the z axis and k in the ( y , z ) plane . The orbit integral appearing in ( 3 ) is thus where ( 2.10 ) 0 exp [ pt ] exp [ ik Z ] exp [ ik_y ] dτ , Jexp [ p z = v2t y [ sin ( 2 + ) ...
Page 240
... orbits in a strong magnetic field is based on a formal expansion in powers of me [ 8 ] , the coefficient of the acceleration . The drift motion is then determined only by four initial data ( position and longitudinal velocity ) instead ...
... orbits in a strong magnetic field is based on a formal expansion in powers of me [ 8 ] , the coefficient of the acceleration . The drift motion is then determined only by four initial data ( position and longitudinal velocity ) instead ...
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