Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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Page 188
... variables are appropriate for setting up an action principle to describe the behavior of the plasma . By introducing a Green function to characterize the ... variables . In linear theory , the variables a ( k , 188 P. A. STURROCK.
... variables are appropriate for setting up an action principle to describe the behavior of the plasma . By introducing a Green function to characterize the ... variables . In linear theory , the variables a ( k , 188 P. A. STURROCK.
Page 189
M. N. Rosenbluth. In linear theory , the variables a ( k , t ) are in fact independent of time . When nonlinear terms of the equations of motion are taken into account , it is found that the resulting modification of the dynamical variables ...
M. N. Rosenbluth. In linear theory , the variables a ( k , t ) are in fact independent of time . When nonlinear terms of the equations of motion are taken into account , it is found that the resulting modification of the dynamical variables ...
Page 247
... variable x * = x / L and then taking the limit L → ∞ ; which boils down to the charge neutrality condition ( 37 ) R * * ( * ) exp [ 9 * ( * ) ] αξ * ' p * % ( 5 * ) — p * ( x * ) ( 0 * ( x * ) = o ( Lx * ) ; R * = R / L is assumed to ...
... variable x * = x / L and then taking the limit L → ∞ ; which boils down to the charge neutrality condition ( 37 ) R * * ( * ) exp [ 9 * ( * ) ] αξ * ' p * % ( 5 * ) — p * ( x * ) ( 0 * ( x * ) = o ( Lx * ) ; R * = R / L is assumed to ...
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