Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 235
... boundary layers , corresponding to the two boundary conditions ( e.g. y ( -1 ) = y ( 1 ) = 1 ) . In our example one of them is absent , having chosen the left boundary condition to fit the ... BOUNDARY LAYER PROBLEMS IN PLASMA PHYSICS 235.
... boundary layers , corresponding to the two boundary conditions ( e.g. y ( -1 ) = y ( 1 ) = 1 ) . In our example one of them is absent , having chosen the left boundary condition to fit the ... BOUNDARY LAYER PROBLEMS IN PLASMA PHYSICS 235.
Page 237
... boundary condition . The first theorem proves that there exist solutions y = y 。( x , ε ) of ( 8 ) which fulfil Yo ( B , ε ) = l2 , but not , in general , the other boundary condition , and ... BOUNDARY LAYER PROBLEMS IN PLASMA PHYSICS 237.
... boundary condition . The first theorem proves that there exist solutions y = y 。( x , ε ) of ( 8 ) which fulfil Yo ( B , ε ) = l2 , but not , in general , the other boundary condition , and ... BOUNDARY LAYER PROBLEMS IN PLASMA PHYSICS 237.
Page 239
... boundary layer could be provided by an expansion of w ( x , ɛ ) in ɛ ; for more details and a far reach- ing generalization of this method , see [ 3 ] . In the case of eqs . ( 5 ) and ( 2 ) the boundary layer eq . ( 11 ) reads d2w dw + ...
... boundary layer could be provided by an expansion of w ( x , ɛ ) in ɛ ; for more details and a far reach- ing generalization of this method , see [ 3 ] . In the case of eqs . ( 5 ) and ( 2 ) the boundary layer eq . ( 11 ) reads d2w dw + ...
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