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Maxwell's Equations -p037ugRvxTI
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Gauss and Faraday
and Ampere found a lot of ways to
Solve for EM fields
But this did not always work for capacitors
Then Maxwell came
Invented displacement current, and now we have:
Del dot D; is free charge (density)
Del cross E; is minus the change in B
Del cross H; is current (density) plus the change in D
Needless to say
There's no such thing as magnetic monopoles
So, del dot B
Must equal zero, but you knew that anyway.
Say after me:
Maxwell's consistent with special relativity
Del dot D; is free charge (density)
Del cross E; is minus the change in B
Del cross H; is current (density) plus the change in D
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