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 \( n^{2/3} v \).
A cube of side 10 cm is suspended from one end of a fine string of length 27 cm, and a mass of 200 grams is connected to the other end of the string. When the cube is half immersed in water, the system remains in balance. Find the density of the cube.