Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 97
... boundary conditions , our analysis - using these solutions - will be governed just by these initial and boundary conditions . This produces two consequences : first , since we have an infinite number of possible initial and boundary ...
... boundary conditions , our analysis - using these solutions - will be governed just by these initial and boundary conditions . This produces two consequences : first , since we have an infinite number of possible initial and boundary ...
Page 234
Boundary Layer Problems in Plasma Physics . B. BERTOTTI Laboratorio Gas ... conditions ( 2 ) is ( 3 ) εy " + y = 0 , y ( 0 ) = 0 , y ( 1 ) = 1 , y ( x ... boundary condition . A small region of rapid change ( boundary layer ) is thus ...
Boundary Layer Problems in Plasma Physics . B. BERTOTTI Laboratorio Gas ... conditions ( 2 ) is ( 3 ) εy " + y = 0 , y ( 0 ) = 0 , y ( 1 ) = 1 , y ( x ... boundary condition . A small region of rapid change ( boundary layer ) is thus ...
Page 235
... 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 fundamental solution y 。= 0 . ( 5 ) An entirely different behaviour occurs instead for ...
... 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 fundamental solution y 。= 0 . ( 5 ) An entirely different behaviour occurs instead for ...
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