Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 41
Page 34
and since the fields are assumed small , we may use a perturbation solution of this about some distribution fo , assumed known , transforming , ( III.3.2 ) whereupon , on Fourier- f = fo + f ' , f ' ( w , k ) e E ( w , k ) ( d / dv ) ƒo ...
and since the fields are assumed small , we may use a perturbation solution of this about some distribution fo , assumed known , transforming , ( III.3.2 ) whereupon , on Fourier- f = fo + f ' , f ' ( w , k ) e E ( w , k ) ( d / dv ) ƒo ...
Page 160
... assumed in eq . ( 2 ) , and the mass of the electrons is neglected . ( 3 ) 2 ) The fluid is assumed to be incompressible , ▽ ⋅v = 0 . Generalization of the present equations to include the compressible case 160 H. P. FURTH.
... assumed in eq . ( 2 ) , and the mass of the electrons is neglected . ( 3 ) 2 ) The fluid is assumed to be incompressible , ▽ ⋅v = 0 . Generalization of the present equations to include the compressible case 160 H. P. FURTH.
Page 161
... assumed to result only from convection d ( go ) at + v⋅V ( go ) = 0 . 6 ) The zero - order distribution will be assumed to have v = 0. Strictly speaking , this condition implies ( 7 ) VX ( VxBo ) = 0 , which will be referred to as the ...
... assumed to result only from convection d ( go ) at + v⋅V ( go ) = 0 . 6 ) The zero - order distribution will be assumed to have v = 0. Strictly speaking , this condition implies ( 7 ) VX ( VxBo ) = 0 , which will be referred to as the ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
3 other sections not shown
Other editions - View all
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 electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function 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 region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ