Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 3
... linear while those in general relativity are not . The linear differential equations are much easier to handle but there is an intrinsic logical incompleteness in linear field theories . Thus it is sometimes speculated that the ultimate ...
... linear while those in general relativity are not . The linear differential equations are much easier to handle but there is an intrinsic logical incompleteness in linear field theories . Thus it is sometimes speculated that the ultimate ...
Page 66
... linear isotropic , D = E with e independent of E , then we can , integrate the above expression to obtain W = 1 √ √ € E2dv = 1 877JE - Ddv Hence we have the result that the field energy density is E - D / 8л or € E2 / 8л . Notes 1. In ...
... linear isotropic , D = E with e independent of E , then we can , integrate the above expression to obtain W = 1 √ √ € E2dv = 1 877JE - Ddv Hence we have the result that the field energy density is E - D / 8л or € E2 / 8л . Notes 1. In ...
Page 321
... linear field equation , 3 linear superposition principle , 3-5 Lorentz force , 236 , 256 , 294 gauge ( see under gauge ) invariants for magnetic field , 308 transformation , 207 , 245 , 291,295 , 297,304 , 306 , 309 , 310 magnetic ...
... linear field equation , 3 linear superposition principle , 3-5 Lorentz force , 236 , 256 , 294 gauge ( see under gauge ) invariants for magnetic field , 308 transformation , 207 , 245 , 291,295 , 297,304 , 306 , 309 , 310 magnetic ...
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