(c) Rate of cooling $R_{C} = \frac{A\varepsilon\sigma(T^{4} - T_{0}^{4})}{mc} = \frac{A\varepsilon\sigma(T^{4} - T_{0}^{4})}{V\rho C}$
$\Rightarrow R_{C} \propto \frac{A}{V} \propto \frac{1}{r} \propto \frac{1}{(Diameter)}\ \ \lbrack\because m = \rho V\rbrack$
Since diameter of $A$ is half that of $B$ so it’s rate of cooling will be doubled that of $B$