Step 1: Use the first law directly. For one mole, $dQ = C\,dT$, $dU = C_v\,dT$, and $dW = P\,dV$, so $C = C_v + P\dfrac{dV}{dT}$.
Step 2: The gas obeys $P = kV$ and the ideal-gas law $PV = RT$. Substituting $P = kV$ gives $kV^2 = RT$, hence $V^2 = \dfrac{RT}{k}$ and $V = \sqrt{RT/k}$.
Step 3: Differentiate $kV^2 = RT$ with respect to $T$: $2kV\dfrac{dV}{dT} = R$, so $\dfrac{dV}{dT} = \dfrac{R}{2kV}$.
Step 4: Then $P\dfrac{dV}{dT} = (kV)\cdot\dfrac{R}{2kV} = \dfrac{R}{2}$. Therefore
\[C = C_v + \frac{R}{2}.\]
\[\boxed{C = C_v + \dfrac{R}{2}}\]