Final Note for UFT385: The Hodge dual potentials

This method expresses the Hodge dual of the electromagnetic field tensor in terms of the same covariant derivatives as usually used for the field tensor itself. With this method the conservation of antisymmetry for the magnetic dipole field can be proven using the same method as in Note 385(4) for the electric dipole field. This new method looks very useful and entirely, and will be the subject of the last note for UFT385.


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