Step 1: Understanding the Question:
The problem compares two different thermodynamic processes starting from the exact same initial state $(P, V, T)$ to the same final volume $V' = 2V$.
In the first scenario, the gas undergoes an isothermal expansion to a final pressure $P_i$.
In the second scenario, the same gas undergoes an adiabatic expansion to a final pressure $P_a$. We need to find the ratio $\frac{P_i}{P_a}$.
Step 2: Key Formula or Approach:
1. For an isothermal process ($T = \text{constant}$):
$$PV = \text{constant} \implies P_1 V_1 = P_2 V_2$$
2. For an adiabatic process:
$$PV^\gamma = \text{constant} \implies P_1 V_1^\gamma = P_2 V_2^\gamma$$
Step 3: Detailed Explanation:
Let's analyze the isothermal expansion first:
$$P \cdot V = P_i \cdot (2V) \implies P_i = \frac{P}{2}$$
Now, let's analyze the adiabatic expansion:
$$P \cdot V^\gamma = P_a \cdot (2V)^\gamma$$
$$P \cdot V^\gamma = P_a \cdot 2^\gamma \cdot V^\gamma$$
Canceling out $V^\gamma$ from both sides gives:
$$P_a = \frac{P}{2^\gamma}$$
Now, take the ratio of the final pressure of the isothermal expansion ($P_i$) to that of the adiabatic expansion ($P_a$):
$$\frac{P_i}{P_a} = \frac{\left(\frac{P}{2}\right)}{\left(\frac{P}{2^\gamma}\right)} = \frac{2^\gamma}{2} = 2^{\gamma - 1}$$
Step 4: Final Answer:
The ratio $\frac{P_i}{P_a}$ is equal to $2^{\gamma - 1}$, which matches option (B).