Step 1: Terminal velocity law
\(v_T=\frac{2r^2(\rho-\sigma)g}{9\eta}\), so \(v_T\propto r^2\).
Step 2: Volume conservation
Two drops merge: \(\frac43\pi R^3=2\cdot\frac43\pi r^3\), so \(R^3=2r^3\).
Step 3: Result
\(\frac{V^{\prime}}{V}=\frac{R^2}{r^2}\), so \(V^{\prime}=\frac{VR^2}{r^2}\). Option (A).
Final Answer:
The terminal velocity is \(\frac{VR^2}{r^2}\), option (A).
\[ \boxed{\text{(A)}} \]