(c) Both the cylinders are in parallel, for the heat flow from one end as shown
Hence $K_{eq} = \frac{K_{1}A_{1} + K_{2}A_{2}}{A_{1} + A_{2}}$
Where $A_{1} =$ Area of cross-section of inner cylinder $\propto \pi R^{2}$ and $A_{2} =$ Area of cross-section of cylindrical shell
$= \pi\left\{ (2R)^{2} - (R)^{2} \right\} = 3\pi R^{2}$
$\Rightarrow K_{eq} = \frac{K_{1}(\pi R^{2}) + K_{2}(3\pi R^{2})}{\pi R^{2} + 3\pi R^{2}} = \frac{K_{1} + 3K_{2}}{4}$