Advanced Plasma TheoryM. N. Rosenbluth |
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Page 13
... collision in order to discover the value of v , v ' . On a collision , the centre - of - mass motion is constant ; i.e. ( II.3.2 ) V M1 V1 + M2 V 2 m1 + m2 = M1 v 1 + M 2 V2 m1 + m2 2 and on removing this , the collision is described as ...
... collision in order to discover the value of v , v ' . On a collision , the centre - of - mass motion is constant ; i.e. ( II.3.2 ) V M1 V1 + M2 V 2 m1 + m2 = M1 v 1 + M 2 V2 m1 + m2 2 and on removing this , the collision is described as ...
Page 110
... collision - free description is possible . The cases are : ( ax ) one - dimensional collision - free motion ; ( aß ) one - dimensional motion with collision ; ( ba ) multi - dimensional problem with collisions ; ( bp ) multi ...
... collision - free description is possible . The cases are : ( ax ) one - dimensional collision - free motion ; ( aß ) one - dimensional motion with collision ; ( ba ) multi - dimensional problem with collisions ; ( bp ) multi ...
Page 122
... collision terms on the right - hand side . This is shown by a simple transformation ( V ' [ [ [ { V - [ [ ( v . ( 4.5 ) ( 3 ) ( 3 ) ( 2 ) v ) c¿Q¿ ( c ; ) ƒ¡ ( v . ) f ( v ) d3v¡d3vd2Q = introducing the collision frequency ( 4.6 ) ( 3 ) ...
... collision terms on the right - hand side . This is shown by a simple transformation ( V ' [ [ [ { V - [ [ ( v . ( 4.5 ) ( 3 ) ( 3 ) ( 2 ) v ) c¿Q¿ ( c ; ) ƒ¡ ( v . ) f ( v ) d3v¡d3vd2Q = introducing the collision frequency ( 4.6 ) ( 3 ) ...
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