Broken symmetry 0 electrodynamics

The broken symmetry of a dipole in its vacuum flux exchange has been known in particle physics since the late 1950s. In classical electrodynamics (CEM) the active vacuum and its exchange are omitted altogether, even though experimentally established for many years. As Lee also pointed out, there can be no symmetry of any observable system anyway, unless the vacuum interaction is included. 

A broken 3-space symmetry exists of a magnetic dipole [18] of a permanent magnet, well known in particle physics since 1957 but inexplicably not yet added into classical electrodynamics theory, wherein the broken symmetry of the magnetic dipole rigorously requires that the dipole continually absorb magnetic energy from the active vacuum in unusable form, and that the... 

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