Stokes theorem states
with boundary orientation induced by the chosen surface normal and with sufficient smoothness of the field and surface. Choose the outward normal on the upper unit hemisphere; its equatorial boundary runs counterclockwise as viewed from .
For the stated field, the curl is
On the unit sphere, the outward normal is . In spherical coordinates, the surface integral over the upper hemisphere is
For the boundary calculation, parametrize , with . Then and
Thus both sides equal . Reversing the hemisphere orientation reverses both signs. The hemisphere's flux calculation can also be read as the projected area of its equatorial unit disk.
Figure 1.
Two equal-endpoint paths and the oriented hemisphere used in Stokes' theorem
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