To solve this problem, we need to understand the relationship between the pressure and temperature of a gas during an adiabatic process and its connection to the specific heat capacities C_p and C_v.
In an adiabatic process, the relation between pressure P and temperature T for an ideal gas can be expressed using the adiabatic equation:
P \cdot V^\gamma = \text{constant}
where \gamma (gamma) is the adiabatic index or the ratio of specific heats C_p / C_v.
The given condition states that pressure P is proportional to the cube of temperature T:
P \propto T^3
From the ideal gas law, we know:
PV = nRT
Thus, for an adiabatic process, combining both equations, we have:
PV^\gamma = \text{constant} \quad \Rightarrow \quad P \cdot \left(\frac{nRT}{P}\right)^\gamma = \text{constant}
Simplifying gives:
P^{1-\gamma} \cdot T^\gamma = \text{constant}
With P \propto T^3, we equate the exponents:
1-\gamma + 3\gamma = 0
1+2\gamma = 0 \quad \Rightarrow \quad \gamma = \frac{3}{2}
Therefore, the ratio C_p/C_v = \gamma = \frac{3}{2}.
Thus, the correct answer is 3/2.
