Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 104
... denotes the emission probability of an electron of energy E , ( E ) the supply function . Both functions are given in the work of MURPHY and Good ( † ) . There is no general analytical formulation of this emission current as a function ...
... denotes the emission probability of an electron of energy E , ( E ) the supply function . Both functions are given in the work of MURPHY and Good ( † ) . There is no general analytical formulation of this emission current as a function ...
Page 161
... Denoting perturbed quantities by the subscript 1 , f1 ( r , t ) = f ( y ) exp [ i ( k ̧x + k22 ) + wt ] we obtain to first order the set of equations ( 8 ) ( 9 ) 1 @ B1 = ▽ × ( v1 × Bo ) ▽ × [ no ▽ × B1 + n1 ▽ × Bo ] , Απ ▽ × Qovi ...
... Denoting perturbed quantities by the subscript 1 , f1 ( r , t ) = f ( y ) exp [ i ( k ̧x + k22 ) + wt ] we obtain to first order the set of equations ( 8 ) ( 9 ) 1 @ B1 = ▽ × ( v1 × Bo ) ▽ × [ no ▽ × B1 + n1 ▽ × Bo ] , Απ ▽ × Qovi ...
Page 162
... denote differentiation with respect to a dimensionless variable μ = ya , where a is a measure of the thickness of the current layer . The quan- tities B , ( n ) , and ( g ) are measures of the field strength , resistivity , and mass ...
... denote differentiation with respect to a dimensionless variable μ = ya , where a is a measure of the thickness of the current layer . The quan- tities B , ( n ) , and ( g ) are measures of the field strength , resistivity , and mass ...
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