Step 1: Understanding relation.
The temperature dependence of K$_p$ is given by:
$\frac{d(\ln K_p)}{dT} = \frac{\Delta U^0}{RT^2}$.
On integrating,
$\ln K_p = -\frac{\Delta U^0}{R} \frac{1}{T} + \text{constant}$.
But for internal energy change, the temperature-based form gives slope proportional to $-\Delta U^0 / R$ with lnK$_p$ vs T.
Step 2: Identifying the correct plot.
When slope = $-\Delta U^0 / R$, the plot must be lnK$_p$ versus T.
Step 3: Conclusion.
Hence, the required plot is lnK$_p$ vs T.