Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 11
... axis OX the magnetic field and represent the peculiar velocity c by ( II.2.1 ) = c1 = c1 cos q , - c1 = C , sin q , whereupon ( II.2.2 ) af af CXB . W m dv and the equation to be solved becomes ( II.2.3 ) af f ωτ aq = ƒo [ 1 − ̃P ] ...
... axis OX the magnetic field and represent the peculiar velocity c by ( II.2.1 ) = c1 = c1 cos q , - c1 = C , sin q , whereupon ( II.2.2 ) af af CXB . W m dv and the equation to be solved becomes ( II.2.3 ) af f ωτ aq = ƒo [ 1 − ̃P ] ...
Page 147
... 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 + ) - sin q ] , - x = V Ω - [ cos ( 2x + y ) cos q ] . Here is the ...
... 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 + ) - sin q ] , - x = V Ω - [ cos ( 2x + y ) cos q ] . Here is the ...
Page 149
in a co - ordinate system in which one of the axes is parallel to k , determining j from the Boltzmann equation ; we ... axis for x in the lower half - plane ( growing waves ) , Limiting forms are given by ( 3.4 ) W 1 + iv π x 1 W 2x2 ...
in a co - ordinate system in which one of the axes is parallel to k , determining j from the Boltzmann equation ; we ... axis for x in the lower half - plane ( growing waves ) , Limiting forms are given by ( 3.4 ) W 1 + iv π x 1 W 2x2 ...
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