To solve this problem, we need to understand the behavior of a monoatomic gas under adiabatic processes. When a gas is compressed or expanded without any heat exchange with the environment, it undergoes an adiabatic process. For a monoatomic ideal gas, this process follows the equation:
PV^{\gamma} = \text{constant}
where \gamma, the adiabatic index, is the ratio of specific heats and equals \frac{5}{3} for a monoatomic gas.
P_i V_i^{\gamma} = P_f V_f^{\gamma}
Substituting the known values:
P \cdot V^{\frac{5}{3}} = P_f \cdot \left(\frac{V}{8}\right)^{\frac{5}{3}}
Solving for the final pressure P_f:
P_f = P \cdot \left(\frac{V}{\frac{V}{8}}\right)^{\frac{5}{3}} = P \cdot (8)^{\frac{5}{3}}
Calculating (8)^{\frac{5}{3}}:
Therefore, the final pressure P_f = 32P.
Thus, the correct answer is 32P.