Let and . The region is the first-octant portion of the ellipsoid . In cylindrical coordinates, write and . Away from the axis, the divergence is
The field is singular on the axis, so applying the classical divergence theorem there without qualification would be invalid. Instead remove and apply it to the remaining region. On the added cylindrical boundary the unit normal is , and
Its area element is , so its flux is . The axial component of the field has zero dot product with this normal. The volume integral of the divergence is locally integrable, because its factor cancels the cylindrical measure. Thus removing a singular axis in a flux integral gives the desired improper surface integral with no extra axial term.
The divergence theorem now reduces the calculation to
The integral over is the area of a quarter unit disk. All boundary fluxes are interpreted as convergent improper integrals at the axis.

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