Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 274
... plasma frequency , the assumptions of no charge separation and neglect of displacement current are also untenable . One can now adopt the kinetic theory approach of introducing a distribution function and use Boltzmann's equation . If f ...
... plasma frequency , the assumptions of no charge separation and neglect of displacement current are also untenable . One can now adopt the kinetic theory approach of introducing a distribution function and use Boltzmann's equation . If f ...
Page 275
... plasma although the Coulomb force is a long range one , one has effectively a short range force field about any charged particle . This may be seen as follows . A positively charged particle attracts the electrons and repels the ...
... plasma although the Coulomb force is a long range one , one has effectively a short range force field about any charged particle . This may be seen as follows . A positively charged particle attracts the electrons and repels the ...
Page 277
... plasma by the relation p = nKT or < 1/2 mV2 > = 2KT . 3 1 . The collision integral on the right of equation ( 12 ) would vanish if there be only one type of particles for in collisions the total momentum is conserved . In case there are ...
... plasma by the relation p = nKT or < 1/2 mV2 > = 2KT . 3 1 . The collision integral on the right of equation ( 12 ) would vanish if there be only one type of particles for in collisions the total momentum is conserved . In case there are ...
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
Copyright | |
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angle angular axes axis B₁ boundary conditions calculate called charge density charged particle coil components conductor consider coordinates cos² cose dielectric constant dipole dipole moment direction distance E₁ electric field electromagnetic field electromotive force electron electrostatic equation 16 expression field due field point finite fluid formula frame frequency function gives Hence incident interaction Laplace's equation linear Lorentz Lorentz transformation magnetic field magnitude Maxwell's equations momentum motion normal obtain orthogonal P₁ permanent magnets perpendicular photon plane plasma point charge polarization Poynting vector R₁ radiation field radiation reaction radius refracted region scalar sin² solution spherical surface integral symmetry tensor term theorem theory of relativity transformation transverse uniform vanishes vector potential velocity wave length Απ дв дг ді дх