Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 51
... plane AA ' and the sphere at infinity . Now con - sider a charge - q at P ' such that OP ' = OP i.c. P ' is the position of the optical image of a source at P by a reflecting planc AA ' . The potential everywhere on the plane due to ...
... plane AA ' and the sphere at infinity . Now con - sider a charge - q at P ' such that OP ' = OP i.c. P ' is the position of the optical image of a source at P by a reflecting planc AA ' . The potential everywhere on the plane due to ...
Page 52
... plane is equal to q . However , that result can be inferred directly by considering the flux over a closed surface consisting of the hemi- sphere on the right at infinity and surface either within the conducting plane or entirely on the ...
... plane is equal to q . However , that result can be inferred directly by considering the flux over a closed surface consisting of the hemi- sphere on the right at infinity and surface either within the conducting plane or entirely on the ...
Page 128
... plane containing k and n ( this plane is called the plane of incidence ) ; correspon- dingly B in this case will be normal to the plane of incidence . In the second case the situation will be reversed - E will be normal to the plane of ...
... plane containing k and n ( this plane is called the plane of incidence ) ; correspon- dingly B in this case will be normal to the plane of incidence . In the second case the situation will be reversed - E will be normal to the plane of ...
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