Advanced Plasma TheoryM. N. Rosenbluth |
From inside the book
Results 1-3 of 24
Page 14
... quantities , and the integral equation may be written ( I │v — v ' │σ1 ( │v— v ' \ , ☺ ) ƒ1 ( v ) ƒ1 ( v ' ) [ $ 1 ( v ) + $ 1 ( v ' ) − $ 1 ( ~ ) − $ 1 ( v ' ) ] + ( 11.3.6 ) far få2 \ r + - v — v ' | σ12 ( v v ' , O ) ƒ , ( v ) ...
... quantities , and the integral equation may be written ( I │v — v ' │σ1 ( │v— v ' \ , ☺ ) ƒ1 ( v ) ƒ1 ( v ' ) [ $ 1 ( v ) + $ 1 ( v ' ) − $ 1 ( ~ ) − $ 1 ( v ' ) ] + ( 11.3.6 ) far få2 \ r + - v — v ' | σ12 ( v v ' , O ) ƒ , ( v ) ...
Page 78
... quantities which are necessary conditions for the solu- tions of the first order equations have been obtained . Thus , we have attained our goal of determining a system of equations for the zeroth - order quantities . In these notes we ...
... quantities which are necessary conditions for the solu- tions of the first order equations have been obtained . Thus , we have attained our goal of determining a system of equations for the zeroth - order quantities . In these notes we ...
Page 121
... quantities without index refer to the par- ticle under consideration , the index ( i ) to the particle components with which the test particle collides . The prime ( ' ) characterizes quantities after collision . The bar indicates the ...
... quantities without index refer to the par- ticle under consideration , the index ( i ) to the particle components with which the test particle collides . The prime ( ' ) characterizes quantities after collision . The bar indicates the ...
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