Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 109
... oscillations are damped out because of the irreversible joule heat production . In reality there is an additional source of damping due to the radiation of electromagnetic waves which is however being neglected in the quasi - stationary ...
... oscillations are damped out because of the irreversible joule heat production . In reality there is an additional source of damping due to the radiation of electromagnetic waves which is however being neglected in the quasi - stationary ...
Page 274
(a Course of Lectures) A. K. Raychaudhuri. 21 Two component plasma oscillations In case the frequency of collisions is not so high , the continuous fluid approximation is no longer appropriate . Further for frequencies of oscillation ...
(a Course of Lectures) A. K. Raychaudhuri. 21 Two component plasma oscillations In case the frequency of collisions is not so high , the continuous fluid approximation is no longer appropriate . Further for frequencies of oscillation ...
Page 277
... oscillations of both electrons and protons . We consider oscillations of electric field unaccompanied by any magnetic field . The equations of motion of the protons and electrons are from ( 13 ) in terms of the PLASMA OSCILLATIONS 277.
... oscillations of both electrons and protons . We consider oscillations of electric field unaccompanied by any magnetic field . The equations of motion of the protons and electrons are from ( 13 ) in terms of the PLASMA OSCILLATIONS 277.
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
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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