The logarithm is defined away from the axis, where . For the vector potential , its curl is . Since
we obtain
For this is clockwise circulation about the axis, the velocity structure of a point vortex in each transverse plane.
On the same domain, differentiate the Cartesian components:
Thus
This is also an instance of divergence of a curl is zero, since the potential is smooth off the axis. The classical field is undefined on the axis, so that identity must not be applied there without specifying an extension.
In cylindrical coordinates, and , so
The potential vector has components . Expanding the prescribed cylindrical curl formula gives
Therefore
Since , this agrees with the Cartesian result and its clockwise orientation.

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