For a gas heated at constant pressure, the heat supplied \( Q = nC_p \Delta T \), where \( C_p \) is the molar specific heat at constant pressure.
The work done is \( W = P \Delta V = nR \Delta T \) (using the ideal gas law).
The fraction of heat converted into work is \( \frac{W}{Q} = \frac{nR \Delta T}{nC_p \Delta T} = \frac{R}{C_p} \).
The ratio of specific heats is \( \gamma = \frac{C_p}{C_v} = \frac{4}{3} \). Since \( C_p - C_v = R \), we have \( C_p = \gamma C_v \) and \( C_v = \frac{C_p}{\gamma} \). Thus,
\( C_p - \frac{C_p}{\gamma} = R \implies C_p \left(1 - \frac{1}{\gamma}\right) = R \implies C_p \left(\frac{\gamma - 1}{\gamma}\right) = R \implies \frac{R}{C_p} = \frac{\gamma - 1}{\gamma} \).
Substituting \( \gamma = \frac{4}{3} \):
\( \frac{R}{C_p} = \frac{\frac{4}{3} - 1}{\frac{4}{3}} = \frac{\frac{1}{3}}{\frac{4}{3}} = \frac{1}{4} = 0.25 \).
The percentage is \( 0.25 \times 100 = 25\% \).