Radiative power of a spherical body is given by
$P=\sigma A T^4$
$=\sigma 4 \pi R^2 T^4$
$\Rightarrow \quad P \propto R^2 T^4$
When temperature is halved and radius is doubled, then power becomes
$P^{\prime} =P \times(2)^2 \times\left(\frac{1}{2}\right)^4$
$=P\left(\frac{4}{16}\right)=\frac{P}{4}$
So, power is reduced to $\frac {1}{4}$ th.



