The initial pressure and volume of an ideal gas are P0 and V0. The final pressure of the gas when the gas is suddenly compressed to volume \(\frac{V_0}{4}\) will be(Given γ = ratio of specific heats at constant pressure and at constant volume)
As the gas is suddenly compressed, the process is adiabatic.
The equation for the gas in an adiabatic process is:
\[
P V^\gamma = \text{constant}.
\]
For the initial state:
\[
P_0 V_0^\gamma = P_2 \left(\frac{V_0}{4}\right)^\gamma.
\]
Rearranging to solve for \( P_2 \):
\[
P_2 = P_0 \cdot \frac{V_0^\gamma}{\left(\frac{V_0}{4}\right)^\gamma}.
\]
Simplify the denominator:
\[
P_2 = P_0 \cdot \frac{V_0^\gamma}{\frac{V_0^\gamma}{4^\gamma}} = P_0 \cdot 4^\gamma.
\]
Thus, the final pressure is:
\[
P_2 = P_0 (4)^\gamma.
\]
Hence, the correct answer is \( \boxed{P_0 (4)^\gamma} \).