For an isothermal expansion, we know that the pressure and volume are inversely proportional:
\[
P_1 V_1 = P_2 V_2
\]
Given that the initial volume is \( V \) and the final volume is \( 27V \), the initial and final pressures for the isothermal process are:
\[
P_1 V = P_2 \cdot 27V \quad \Rightarrow \quad P_2 = \frac{P}{27}
\]
For the subsequent adiabatic compression, we use the formula for adiabatic processes:
\[
P V^{\gamma} = \text{constant}
\]
For a monatomic gas, \( \gamma = \frac{5}{3} \). Applying this to the isothermal pressure and volume:
\[
P_2 V^{\gamma} = P_3 V^{\gamma} \quad \Rightarrow \quad \left( \frac{P}{27} \right) \cdot (27V)^{\gamma} = P_3 \cdot V^{\gamma}
\]
Simplifying the equation:
\[
P_3 = 9P
\]
Thus, the final pressure is \( 9P \).