(c) Change in internal energy
$dU = dQ - dW$
At constant pressure
$dU = C_{p}dT - p\ dV$
$= C_{p}dT - R\ dT$
$= \left( C_{p} - R \right)\ dT$
$= C_{v}\ dT$
$= \frac{R}{\gamma - 1}dT$
$= \frac{R}{\gamma - 1} \times \frac{pV}{R}$
$= \frac{pV}{\gamma - 1}$