(c) $\frac{d\theta}{dt} = \frac{\varepsilon A\sigma}{mc}4\theta_{0}^{3}\mathrm{\Delta}\theta$
For given sphere and cube $\frac{\varepsilon A\sigma}{mc}4\theta_{0}^{3}\mathrm{\Delta}\theta$ is constant so for both rate of fall of temperature $\frac{d\theta}{dt} =$ constant