To solve this problem, we need to determine the ratio of specific heats \(\frac{C_P}{C_V}\) for a gas undergoing an adiabatic process.
For an adiabatic process in an ideal gas, the relation between pressure and volume is:
\(P V^{\gamma} = \text{constant}\), where \(\gamma = \frac{C_P}{C_V}\).
Using the ideal gas equation:
\(P V = n R T\)
We can eliminate \(V\) by writing \(V = \frac{nRT}{P}\) and substituting into the adiabatic equation.
This gives the temperature–pressure relation for an adiabatic process:
\(T^{\gamma} P^{1-\gamma} = \text{constant}\)
Rearranging, we get:
\(P \propto T^{\frac{\gamma}{\gamma-1}}\)
According to the question, pressure is directly proportional to the cube of absolute temperature:
\(P \propto T^3\)
Comparing the powers of \(T\):
\(\frac{\gamma}{\gamma - 1} = 3\)
Solving:
\(\gamma = \frac{3}{2}\)
Therefore, the ratio of specific heats is:
Correct Answer: \(\frac{C_P}{C_V} = \frac{3}{2}\)