If the mean free path is constant, the collision frequency \(f\) is directly proportional to the square root of temperature (\(\sqrt{T}\)):
\[ f \propto \sqrt{T} \]
Parameters:
\[ T_1 = 27^\circ C = 300 \, \text{K}, \quad T_2 = 127^\circ C = 400 \, \text{K} \]
The ratio of collision frequencies is calculated as:
\[ \frac{f_2}{f_1} = \sqrt{\frac{T_2}{T_1}} = \sqrt{\frac{400}{300}} = \sqrt{\frac{4}{3}} \]
Consequently:
\[ f_2 = \sqrt{\frac{4}{3}} \cdot f_1 = \frac{2}{\sqrt{3}} f_1 \]

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