Step 1: Understanding the Question:
An ideal gas undergoes a two-step thermodynamic process: first, an isothermal expansion from volume $V$ to $9V$, followed by an adiabatic compression returning the volume back to $V$. We need to calculate the final pressure of the gas at the end of these two steps.
Step 2: Key Formula or Approach:
1.
For the Isothermal Stage: Temperature is constant, satisfying Boyle's Law:
$$P_1 V_1 = P_2 V_2$$
2.
For the Adiabatic Stage: The system follows Poisson's relation:
$$P_2 V_2^{\gamma} = P_3 V_3^{\gamma}$$
where $\gamma = \frac{C_p}{C_v} = \frac{3}{2} = 1.5$.
Step 3: Detailed Explanation:
Let's track the state parameters across both processes:
Initial State 1: Pressure $= P$, Volume $= V$
Step 1: Isothermal Expansion to State 2 ($V_2 = 9V$):
$$P \cdot V = P_2 \cdot (9V) \implies P_2 = \frac{P}{9}$$
Step 2: Adiabatic Compression to State 3 ($V_3 = V$):
Using the adiabatic equation between state 2 and state 3:
$$P_2 V_2^{\gamma} = P_3 V_3^{\gamma} \implies P_3 = P_2 \left(\frac{V_2}{V_3}\right)^{\gamma}$$
Substitute the volume values and $P_2 = \frac{P}{9}$ into the expression:
$$P_3 = \left(\frac{P}{9}\right) \cdot \left(\frac{9V}{V}\right)^{3/2}$$
$$P_3 = \frac{P}{9} \cdot (9)^{3/2}$$
To compute $(9)^{3/2}$ easily, take the square root of $9$ first ($\sqrt{9} = 3$), and then cube it ($3^3 = 27$):
$$P_3 = \frac{P}{9} \cdot 27 = 3P$$
Step 4: Final Answer:
The final pressure of the gas is $3P$, which corresponds to option (C).