First calculate the curl:
By Stokes theorem, use the positively oriented equator , . Its tangent is , while the restricted field is . Thus
The first term integrates to zero over a full period and the second uses .
One can also calculate directly on the curved surface. With spherical coordinates , ,
Substitution gives the scalar integrand . Its azimuthal sine term vanishes, and the rest gives , confirming the orientation and the same result.

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