For an oriented piecewise smooth surface and a continuously differentiable vector field, Stokes theorem states
where the boundary orientation is induced by through the right-hand rule. Choose the upward orientation of the elliptic paraboloid. Its band has cylindrical radius , and a parametrization is
Its oriented surface element and scalar area element are
The requested sketch shows the open band, not a capped solid.
Figure 1.
Upward-oriented annular paraboloid band, with counterclockwise outer boundary and clockwise inner boundary
. Details.
For the specified vector field, direct differentiation gives . Hence
To check this by Stokes theorem, parametrize a counterclockwise circle of radius at height by . Along it , and
Using gives . The induced outer circle is counterclockwise as viewed from above, and the inner circle is clockwise. Therefore
This verifies the direct surface integral and the Stokes flux through an annular paraboloid. Reversing the chosen surface orientation reverses the final sign.
For an oriented smooth surface with piecewise smooth, consistently oriented boundary, Stokes theorem gives
for a continuously differentiable vector field defined on a neighborhood of . Choose the upward normal vector here. The surface is an annular band of an elliptic paraboloid, parametrized by
Using as the oriented vector area element gives
The sketch below shows the open band, not a capped solid. Its upper circle has radius one and its lower circle radius one third.
Figure 1.
Annular paraboloid with upward normal and opposite induced orientations on the outer and inner boundary circles
. Details.
Differentiating the given vector field yields
The surface integral is therefore
For the boundary line integral, the upward normal vector induces counterclockwise traversal of the outer circle and clockwise traversal of the inner circle, as viewed from above. On a circle of radius , parametrized counterclockwise, is constant and
Since each fourth power integrates to , the two-circle line integral is
confirming Stokes theorem and the Stokes flux through an annular paraboloid. Reversing the chosen orientation changes both integrals to .