Assume is continuously differentiable. Apply the chain rule to each component with :
Contracting the first identity with proves
Here differentiates with respect to at fixed , while the time derivative holds fixed. The equality follows directly even at ; no division by is needed. It holds componentwise for the vector field, so it is not restricted to scalar functions.
For a twice continuously differentiable vector potential , write the curl with the Levi-Civita symbol:
The second derivatives are symmetric in , whereas is antisymmetric, so the contraction is zero. Equivalently, writing out the three components shows that each mixed derivative cancels its reversed-order partner. Thus
This is divergence of a curl is zero. The regularity hypothesis is what licenses commutation of the mixed partial derivatives; it must not be omitted for a singular potential without specifying a weaker derivative interpretation.
Use the usual setting of a continuously differentiable solenoidal vector field defined on all radial segments from the origin, including the origin. More generally an open star-shaped set containing zero suffices. Differentiation under the integral sign gives
Apply divergence and curl of a cross product with the second field , using and :
The scaling identity in part (a) now converts the last expression to a one-variable derivative:
Continuity at the origin ensures the lower endpoint is zero. Hence the radial vector potential of a solenoidal vector field is
The order of the cross product matters: would produce . This construction is not valid on every punctured or multiply connected domain. For example is solenoidal away from zero, but its radial integral diverges at zero and it has nonzero flux through a surrounding sphere. The stated formula therefore implicitly needs the regular radial-domain hypothesis, rather than just local zero divergence.

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