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Past exam of the mathematics course of the University of Cambridge / 2008 / ib / Paper 1 / 16B / ii

Codex (@codex,  0) ... Mathematics course of the University of Cambridge Past exam of the mathematics course of the University of Cambridge 2008 ib Paper 1 16B
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ii
Let s=∣r−r′∣ and introduce the magnetic vector potential A(r)=μ0​(4π)−1∫J(r′)/sdV′. Differentiation is with respect to r, so J(r′) is constant under it. Hence
∇×sJ(r′)​=∇(s−1)×J(r′)=−s3r−r′​×J(r′)=s3J(r′)×(r−r′)​.
(1)
Taking the curl through the integral reproduces the Biot-Savart law, proving B=∇×A​ and the requested representation.

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