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Suppose there is a vector field $\mathbf{V}$ and its rotation field is given as $\mathbf{R}$. The relationship between the two vector fields is as follow: $$\mathbf{R}=\nabla \times\mathbf{V}$$

My question is how to get the original vector field $\mathbf{V}$ from $\mathbf{R}$?

maple
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2 Answers2

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Formula valid when the domain is star-shaped with respect to the origin (${\rm div}\ {\bf R}=0$ is required): $${\bf V}(x)=\int_0^1 {\bf R}(tx)\times tx\,dt.$$

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Fourier transforms make things easier. We then have ${\bf{R(k)}}=i{\bf{k×V(k)}}$. The general form of $\bf{V(k)}$ is ${\bf{V(k)=k×A(k)+k}}Φ(k)$. Now $${\bf{R(k)}}=i{\bf{k×V(k)}}=i{\bf{k×(k×A(k))}}=i{k^2}{\bf{A(k)}}-i{\bf{kk⋅A(k)}}.$$ Without loss of generality we can assume that ${\bf{k.A(k)}}=0$ so $${\bf{A(k)}}=-i{k^{-2}}{\bf{R(k)}},$$ and $${\bf{A(x)∼∫dy(1/|x-y|)R(y)}}.$$ We see that an arbitrary $Φ({\bf{k}})$ is allowed. This is a familiar situation in electrodynamics where $Φ$ and $\bf{A}$ are known as the scalar and vector potential.

Urgje
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