In solid body rotation, the velocity at any point is proportional to the distance from the axis of rotation, i.e., $v = r\Omega$. The circulation per unit area, which is the line integral of velocity around a closed loop, is given by:
\[
\Gamma = \oint \vec{v} \cdot d\vec{r}.
\]
For a circular loop of radius $r$, the circulation becomes:
\[
\Gamma = r \Omega,
\]
since the velocity is tangential and is given by $v = r \Omega$. Thus, the circulation per unit area is proportional to $r \Omega$.
Thus, the correct answer is:
\[
\boxed{\text{(A) } r\Omega}.
\]