Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 2
... field is assumed to exist in space surrounding any electrical charge and ( ii ) this field is considered responsible ... mean is this — suppose the force on charge e , due to charge e is of the form f ( e ) ø ( e ) , apart from the ...
... field is assumed to exist in space surrounding any electrical charge and ( ii ) this field is considered responsible ... mean is this — suppose the force on charge e , due to charge e is of the form f ( e ) ø ( e ) , apart from the ...
Page 207
... field we obtain for the uniformly moving charged particle . The second term ... mean any loss of generality from the point of view of the special theory of ... field with 1 / R2 dependence . ( This is a non - radiative field . ) The ...
... field we obtain for the uniformly moving charged particle . The second term ... mean any loss of generality from the point of view of the special theory of ... field with 1 / R2 dependence . ( This is a non - radiative field . ) The ...
Page 244
... field , a charged particle describes a helix which can be considered to be a ... field F other than the magnetic field . We shall take this force field to be ... mean that the characteristic time of variation of E is large compared to the ...
... field , a charged particle describes a helix which can be considered to be a ... field F other than the magnetic field . We shall take this force field to be ... mean that the characteristic time of variation of E is large compared to 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