Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 51
... considered and we assert that on the left side the potential is simply zero everywhere . Thus the proposed solution is ø ( r ) = 9 - 9 for x≥ 0 and ø ( r ) = 0 for x ≤ 0 Ir - OP ! Ir - OP ' and because of the uniqueness theorem is the ...
... considered and we assert that on the left side the potential is simply zero everywhere . Thus the proposed solution is ø ( r ) = 9 - 9 for x≥ 0 and ø ( r ) = 0 for x ≤ 0 Ir - OP ! Ir - OP ' and because of the uniqueness theorem is the ...
Page 58
... considered or as surface charges on the boundary . In case ( b ) G ( r , r ) is so chosen that its gradient normal to the boundary surface has a constant value over the entire surface , being equal to - 4π / S , where S is the total ...
... considered or as surface charges on the boundary . In case ( b ) G ( r , r ) is so chosen that its gradient normal to the boundary surface has a constant value over the entire surface , being equal to - 4π / S , where S is the total ...
Page 113
... considered the electron as a distribution of charge and magnetic dipoles in a finite spherical region of radius r . Show that if the mass of the electron is to be interpreted as electromagnetic field energy , then the contribution of ...
... considered the electron as a distribution of charge and magnetic dipoles in a finite spherical region of radius r . Show that if the mass of the electron is to be interpreted as electromagnetic field energy , then the contribution 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