Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
From inside the book
Results 1-3 of 23
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 . - The purpose of these lectures is to point out a ... 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 . - The purpose of these lectures is to point out a ... 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 yo = 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 yo = 0 . ( 5 ) An entirely different behaviour occurs instead for ...
Common terms and phrases
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 electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ k₂ KRUSKAL KULSRUD l'axe magnétique limit lowest order m₁ magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle perturbation Phys plasma oscillations plasma physics Poisson's equation potential problem quantities R₁ radial region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity voisinage waves in plasmas zero zero-order Απ