Put . On the specified domain, , and direct differentiation gives the divergence and vorticity
For example, the third component of the curl is ; the other two components vanish because depends only on and the transverse velocity is independent of . Hence the flow is both incompressible and irrotational exactly when
The exclusion of the axis matters: these are ordinary derivatives on the domain, with no assertion of regularity on the removed axis.
In cylindrical coordinates, the transverse velocity is , so its contribution to the circulation is . The vertical contribution is , the differential of an antiderivative of , and therefore has zero integral around any closed curve. If is the oriented winding number of the curve's projection about the origin, then
In particular, a single positive winding gives ; reversing orientation reverses the sign. The nonzero circulation is compatible with irrotational flow because the domain is not simply connected. For , an enclosing curve cannot bound a surface contained entirely in the domain to which Stokes theorem would apply.

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