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 \( n^{2/3} v \).
Consider the following statements:
A. Surface tension arises due to extra energy of the molecules at the interior as compared to the molecules at the surface of a liquid.
B. As the temperature of liquid rises, the coefficient of viscosity increases.
C. As the temperature of gas increases, the coefficient of viscosity increases.
D. The onset of turbulence is determined by Reynolds number.
E. In a steady flow, two streamlines never intersect.
Choose the correct answer from the options given below:
$\text{The fractional compression } \left( \frac{\Delta V}{V} \right) \text{ of water at the depth of } 2.5 \, \text{km below the sea level is } \_\_\_\_\_\_\_\_\_\_ \%. \text{ Given, the Bulk modulus of water } = 2 \times 10^9 \, \text{N m}^{-2}, \text{ density of water } = 10^3 \, \text{kg m}^{-3}, \text{ acceleration due to gravity } g = 10 \, \text{m s}^{-2}.$