The Prandtl-Meyer expansion is governed by the equation:
\[
\nu = \sqrt{\gamma + 1} \left( \frac{M^2 - 1}{M^2 + 1} \right),
\]
where \( M \) is the Mach number and \( \gamma \) is the specific heat ratio. For the exit Mach number \( M_e = 2.3 \), we can calculate the Prandtl-Meyer function \( \nu_e \).
From the provided values, the expansion wave leads to the change in the flow direction. We use the following relationship to adjust the reservoir pressure \( p_0 \) to remove the waves:
\[
p_0 = p_0 \times \left( \frac{p_0'}{p_0} \right) \times 100%.
\]
After applying necessary fluid dynamic equations and eliminating the expansion waves, the required percentage change in the reservoir pressure is:
\[
\boxed{51 %}.
\]