(c) At steady state, rate of heat flow for both blocks will be same,
$i.e.,\ \frac{K_{1}A(\theta_{1} - \theta)}{l_{1}} = \frac{K_{2}A(\theta - \theta_{2})}{l_{2}}\lbrack Given\ l_{1} - l_{2}\rbrack$
$\Rightarrow K_{1}A\left( \theta_{1} - \theta \right) = K_{2}A\left( \theta - \theta_{2} \right) \Rightarrow \theta = \frac{K_{1}\theta_{1} + K_{2}\theta_{2}}{K_{1} + K_{2}}$