Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 126
... medium 1 and z < 0 constitutes medium 2 . reflected ray refracted ray то incident ray 2 z = 0 Fig . 1 The unit vector normal to the interface at the point of incidence will be indicated by n , thus , its only nonvanishing component is ...
... medium 1 and z < 0 constitutes medium 2 . reflected ray refracted ray то incident ray 2 z = 0 Fig . 1 The unit vector normal to the interface at the point of incidence will be indicated by n , thus , its only nonvanishing component is ...
Page 134
... medium relative to the second -- this is appropriate ; for one studies total reflection with the first medium say glass and the second medium is air . Thus n is the refractive index of glass with the second medium understood ...
... medium relative to the second -- this is appropriate ; for one studies total reflection with the first medium say glass and the second medium is air . Thus n is the refractive index of glass with the second medium understood ...
Page 221
... medium can emit electromagnetic radiation if its velocity exceeds the velocity of electromagnetic waves in the medium . This radiation is called Cerenkov radiation and it may appear somewhat paradoxical in view of our earlier conclusion ...
... medium can emit electromagnetic radiation if its velocity exceeds the velocity of electromagnetic waves in the medium . This radiation is called Cerenkov radiation and it may appear somewhat paradoxical in view of our earlier conclusion ...
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