$\frac{7}{3}$
Step 1: In an adiabatic process, pressure ($P$) and temperature ($T$) follow the relation: \[ P \propto T^n \] where $n$ is a constant. Given that pressure is proportional to the cube of the temperature, \[ P \propto T^3 \] thus, $n = 3$.
Step 2: The adiabatic relation between pressure and temperature for an ideal gas is given by: \[ P T^{-\frac{\gamma}{\gamma - 1}} = {constant} \] where $\gamma = \frac{C_p}{C_v}$ is the heat capacity ratio.
Step 3: Comparing with the given relation $P \propto T^3$, we equate: \[ -\frac{\gamma}{\gamma - 1} = 3 \]
Step 4: Solving for $\gamma$: \[ \gamma = \frac{3}{2} \]
Step 5: Therefore, the correct answer is (D). \bigskip
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of