Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 126
... propagation ( the reflected wave ) and a part penetrates into the second medium ( refracted wave ) . In reality matters are more complicated - there will be absorption i.c. derangement of the energy to heat and irregular scattering ...
... propagation ( the reflected wave ) and a part penetrates into the second medium ( refracted wave ) . In reality matters are more complicated - there will be absorption i.c. derangement of the energy to heat and irregular scattering ...
Page 133
... wave in the second medium and the incident energy is completely reflected ... propagating wave along the x - axis i.c. parallel to the interface but its ... propagation is along x - axis , E , does not vanish . Turning now to the ...
... wave in the second medium and the incident energy is completely reflected ... propagating wave along the x - axis i.c. parallel to the interface but its ... propagation is along x - axis , E , does not vanish . Turning now to the ...
Page 141
... ( wave guides ) or closed ( cavity reso- nators ) the basis is still Maxwell's ... ( wave guides ) or a diminution of the stored energy ( cavity resonators ) ... propagation of the waves . As we are talking of propagation , the case is of ...
... ( wave guides ) or closed ( cavity reso- nators ) the basis is still Maxwell's ... ( wave guides ) or a diminution of the stored energy ( cavity resonators ) ... propagation of the waves . As we are talking of propagation , the case is 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