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Re: Maxwell's equations |
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| Oct18-07, 05:00 AM | #1 |
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Re: Maxwell's equations
drl wrote:
> Get a copy of Panofsky and Phillips and study chapter 1 until it is in > your bones. They prove the following theorem: > Give any vector field V (satisfying natural differentiability > conditions) and let > D = div V > C = curl V > Define > phi(x,y,z) = (1/4pi) integral over all space ( D(X,Y,Z) / R ) dX dY dZ > A(x,y,z) = (1/4pi) integral over all space ( C(X,Y,Z) / R ) dX dY dZ > where R = sqrt ( (x - X)^2 + (y - Y)^2 + (z - Z)^2 ) and the integration > is over X,Y,Z. Then >V = -grad phi + curl A > If s -> 0 and C -> 0 at infinity, then this resolution is unique. The > import of this theorem is - if there are no sources at infinity, then a > vector field is uniquely determined by its divergence and curl. One > cannot overstate the importance of this result for a proper understanding > of EM. > Corollary - any non-uniqueness in the resolution of a vector > field in terms of its sources must come from additional sources at > infinity. My question: Does the theorem above apply to fields that depend on time or only to static fields? |
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