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| | David Guarrera's Worldsheet: Magnetic Monopoles |
 | | In fact, things are actually much nicer with magnetic charge, as Maxwell's equations are perfectly symmetric between E and B fields (I would write them out if I knew how to do equations in my blog, anybody know?), so the physics is much more beautiful if magnetic charge exists. |
 | | Well, you might ask: what about the vector potential A? We know that B= \del X A, and that if magnetic charges exist \del (dot) B=m \delta^3 (r) (up to a constant for a monopole at the origin, where m is the "magnetic charge", and the delta is the Dirac delta function). |
 | | So, we can put back the monopole if we just get rid of the vector potential (which, for classical electrodynamics, is not necessary), and just use E and B in our calculations. |
| web.mit.edu /guarrera/www/2005/02/magnetic-monopoles.html (1092 words) |
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