The mean free path \( \lambda \) of a molecule is the average distance it traverses between consecutive collisions. This is mathematically expressed as:
\[ \lambda = \frac{1}{\sqrt{2} \pi d^2 n}, \]
where:
- \( n \) signifies the number density of molecules (number of molecules per unit volume),
- \( d \) represents the diameter of a molecule,
- \( \pi \) is the mathematical constant.
Kinetic theory forms the basis for this formula, which accounts for collision probabilities among molecules within a defined volume. The \( \sqrt{2} \) factor incorporates the random nature of molecular velocities and collision probabilities.
Consequently, the average distance a molecule travels between two successive collisions is given by:
\[ \lambda = \frac{1}{\sqrt{2} \pi d^2 n}. \]
Option (3) is therefore correct.

For an ideal gas, a cyclic process ABCA as shown in the P–T diagram. When represented in P–V plot, it would be 