Step 1: Understanding Terminal Velocity and Volume Conservation The terminal velocity \( v \) of a small drop is given by Stokes' law: \[ v \propto R^2 \] where \( R \) is the radius of the drop. When \( n \) small identical drops merge, the volume remains conserved: \[ n \times \frac{4}{3} \pi r^3 = \frac{4}{3} \pi R^3 \] where \( r \) is the radius of each small drop and \( R \) is the radius of the bigger drop.
Step 2: Finding the Radius of the Bigger Drop From volume conservation, \[ n r^3 = R^3 \] \[ R = n^{1/3} r \]
Step 3: Finding the Terminal Velocity of the Bigger Drop Since terminal velocity is proportional to the square of the radius, we can write: \[ V \propto R^2 \] \[ V \propto (n^{1/3} r)^2 \] \[ V \propto n^{2/3} r^2 \] Since the terminal velocity of the small drop is \( v \propto r^2 \), we can write: \[ V = n^{2/3} v \]
Thus, the terminal velocity of the bigger drop is \( n^{2/3} v \).