Step 1: Recall the Kutta--Joukowski theorem.
The lift per unit span acting on an airfoil is
\[
\boxed{
L'=\rho V_{\infty}\Gamma,
}
\]
where
• \(L'\) = lift per unit span,
• \(\rho\) = fluid density,
• \(V_{\infty}\) = free-stream velocity,
• \(\Gamma\) = circulation strength.
Step 2: Identify the directly proportional quantity.
From the equation,
\[
L'
\propto
\Gamma.
\]
Hence,
\[
\boxed{\text{Lift per unit span is directly proportional to circulation strength}.}
\]
Therefore,
\[
\boxed{\text{Circulation strength}}
\]
is the correct answer.
Thus,
\[
\boxed{(A)}
\]
is the correct answer.