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The electromagnetic potentials and fields are assumed to have the same time dependence . It was shown in Chapter 6 that the solution for the vector potential A ( x , 1 ) in the Lorentz gauge is J ( x ' , t ' ) A ( x , t ) | x – x'l dx ...
Both formulas contain the same “ diffraction " distribution factor [ J / ( kaş ) / kaķ ] and the same dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in $ ) , whereas the vector ...
The essential characteristics of this spectrum are its strong peaking at the X - ray energy and its dependence on atomic number as 22 . So far we have considered the radiation which accompanies the disappearance of the charge of an ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
TimeVarying Fields Maxwells Equations Con
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