Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 75
... surface to consist of the infinite YZ plane through the origin and the ... integral over the hemisphere will make no contribution . At any point on the ... surface integral ) is given by E 2q sine 8π Eď sec2 0 2 ik The surface integral ...
... surface to consist of the infinite YZ plane through the origin and the ... integral over the hemisphere will make no contribution . At any point on the ... surface integral ) is given by E 2q sine 8π Eď sec2 0 2 ik The surface integral ...
Page 100
... integral to a surface integral and obtain Notes V × E = - - B C ( 5 ) 1. Subject to the condition that the boundary of the surface coincides with the coil , the surface of integration in ( 4 ) is otherwise arbitrary . This is justified ...
... integral to a surface integral and obtain Notes V × E = - - B C ( 5 ) 1. Subject to the condition that the boundary of the surface coincides with the coil , the surface of integration in ( 4 ) is otherwise arbitrary . This is justified ...
Page 120
... surface integral over an entire closed surface as the energy flux through that surface and must not consider the value of ( E × H ) / 4л as giving the flux at each point separately . Such an argument has an apparent justification in the ...
... surface integral over an entire closed surface as the energy flux through that surface and must not consider the value of ( E × H ) / 4л as giving the flux at each point separately . Such an argument has an apparent justification in the ...
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