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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 , t ) in the Lorentz gauge is с J ( x ' , t ' ) A | x – X ' ! d'x ' | dt ...
Both formulas contain the same “ diffraction " distribution factor [ J / ( kaş ) / kag ] and the same dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in 5 ) , 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 Z ?. So far we have considered the radiation which accompanies the disappearance of the charge of an ...
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Introduction to Electrostatics
References and suggested reading
Multipoles Electrostatics of Macroscopic Media
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