Advanced Plasma TheoryM. 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 206
... variables P ,, Q , and a new Hamiltonian H ( P ,, Q. , t ) . We consider the transformation or variables to be expressible in the form ( A - 4.2 ) p1 = P , + ~ P + 2PH + ... qr = Qr + õQ ; + ☎2Q ! 312 + ... wherein P etc. are to be ...
... variables P ,, Q , and a new Hamiltonian H ( P ,, Q. , t ) . We consider the transformation or variables to be expressible in the form ( A - 4.2 ) p1 = P , + ~ P + 2PH + ... qr = Qr + õQ ; + ☎2Q ! 312 + ... wherein P etc. are to be ...
Page 265
... variables and H ( q , p , t ) the Hamiltonian . Sup- pose q and p can be written as functions of two independent variables t and periodic in with period 2л , in such a way that there is a similar function of t and with the property that ...
... variables and H ( q , p , t ) the Hamiltonian . Sup- pose q and p can be written as functions of two independent variables t and periodic in with period 2л , in such a way that there is a similar function of t and with the property that ...
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 KRUSKAL KULSRUD l'axe magnétique limit 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 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