Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 51
... satisfied and also the combined potential due to these two charges will satisfy the equation V2ø = -4лq 8 ( г - OP ) everywhere on the right - hand side of the plane AA ' . In the left - half space the hypothetical charge is not to be ...
... satisfied and also the combined potential due to these two charges will satisfy the equation V2ø = -4лq 8 ( г - OP ) everywhere on the right - hand side of the plane AA ' . In the left - half space the hypothetical charge is not to be ...
Page 115
... satisfied at all subsequent instants everywhere . Thus ( 3 ) becomes some sort of an initial or boundary condition ... satisfy . ) Of course matters are sometimes differently stated - one uses ( 4 ) and ( 1 ) , to obtain ( 8 ) and says ...
... satisfied at all subsequent instants everywhere . Thus ( 3 ) becomes some sort of an initial or boundary condition ... satisfy . ) Of course matters are sometimes differently stated - one uses ( 4 ) and ( 1 ) , to obtain ( 8 ) and says ...
Page 162
... satisfied as the denominators cannot all be of the same sign . However , the equation has been obtained on the assumption P1 P2 P3 + 0 , so one of them must vanish for the roots to be equal . Let p2 = 0 , then equation ( 20 ) will ...
... satisfied as the denominators cannot all be of the same sign . However , the equation has been obtained on the assumption P1 P2 P3 + 0 , so one of them must vanish for the roots to be equal . Let p2 = 0 , then equation ( 20 ) will ...
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