Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 16
... operator acting on the functions ( c2 ) . If now we consider dOY , the second two equations take the form ( II.3.9 ) ... operator representing the change in produced by collisions . A variational principle may be derived by observing first ...
... operator acting on the functions ( c2 ) . If now we consider dOY , the second two equations take the form ( II.3.9 ) ... operator representing the change in produced by collisions . A variational principle may be derived by observing first ...
Page 61
... operator . The boundary condition on is ( 17 ) e · = 0 . - Equation ( 16 ) is self - contained giving in terms of E. ( A dot denotes time differentiation ) . From condition ( 11 ) , B'e = 0 follows . ( Note : one might consider ...
... operator . The boundary condition on is ( 17 ) e · = 0 . - Equation ( 16 ) is self - contained giving in terms of E. ( A dot denotes time differentiation ) . From condition ( 11 ) , B'e = 0 follows . ( Note : one might consider ...
Page 65
The matrix V / dx , dx , corresponds to our operator F and is obviously self - adjoint , since it is symmetric . Our theory corresponds to a continuum of dimensions but is otherwise algebraically the same . The proof of d ) follows the ...
The matrix V / dx , dx , corresponds to our operator F and is obviously self - adjoint , since it is symmetric . Our theory corresponds to a continuum of dimensions but is otherwise algebraically the same . The proof of d ) follows the ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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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