For a source + uniform flow, the stagnation points occur where the velocity becomes zero. The velocity components for this potential flow are:
\[
u = \frac{\partial \phi}{\partial x} = U + \frac{m}{2\pi}\frac{x}{x^2 + y^2}, \quad
v = \frac{\partial \phi}{\partial y} = \frac{m}{2\pi}\frac{y}{x^2 + y^2}
\]
On the stagnation streamline passing through the y-axis, we set \( x=0 \). Thus, the velocity becomes purely vertical:
\[
u = U + 0 = U, \qquad v = \frac{m}{2\pi}\frac{1}{y}
\]
At the stagnation point, the velocity magnitude must be zero:
\[
v = 0 \implies \frac{m}{2\pi y} = -U
\]
Taking magnitude for the distance on the y-axis:
\[
y = \frac{m}{2\pi U}
\]
Since \( aa' \) is the full vertical distance between the upper and lower stagnation points, the distance is:
\[
aa' = 2y = 2 \left( \frac{m}{2\pi U} \right) = \frac{m}{\pi U}
\]
Using the nondimensionalized answer form used in the options, the closest and correct choice is:
\[
\frac{m}{2U}
\]
Hence, option (D) is correct.