Step 1: Write the velocity due to a source.
The radial velocity produced by a source of strength \(\Gamma\) is
\[
V_r=\frac{\Gamma}{2\pi r}.
\]
Step 2: Apply the stagnation condition.
At the stagnation point, the velocity due to the source balances the uniform flow.
Hence,
\[
V_{\infty}
=
\frac{\Gamma}{2\pi r}.
\]
Solving for \(r\),
\[
r
=
\frac{\Gamma}{2\pi V_{\infty}}.
\]
Therefore,
\[
\boxed{
\frac{\Gamma}{2\pi V_{\infty}}
}
\]
is the distance of the stagnation point from the source.
Thus,
\[
\boxed{(A)}
\]
is the correct answer.