This will be the last note for UFT385. I intend to use the Hodge dual of the field tensor and develop the little known magnetic scalar potential described by Jackson on page 180 into a new antisymmetry law. So the development can continue in exactly the same was as for the electric dipole field. The electric scalar potential is replaced by the much less well known magnetic scalar potential, and the new concept of electric vector potential is replaced by the well known magnetic vector potential. The Hodge dual of a two form is also a two form, so the Hodge dual field tensor is antisymmetric. There are many other ways of developing the problem of conservation of antisymmetry, but this is an elegant solution. The general problem is one of n equations in n unknowns.

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