Step 1: Stefan-Boltzmann Law.
According to the Stefan-Boltzmann law, the power radiated by a black body is proportional to the fourth power of its temperature:
\[
P = \sigma A T^4
\]
where \( P \) is the power, \( \sigma \) is the Stefan-Boltzmann constant, \( A \) is the surface area, and \( T \) is the temperature of the body.
Step 2: Surface area of spherical bodies.
The surface area of a sphere is \( A = 4\pi r^2 \), where \( r \) is the radius of the sphere.
Step 3: Equating power radiated.
For both bodies to radiate the same power:
\[
\sigma A_1 T_1^4 = \sigma A_2 T_2^4
\]
\[
4\pi r_1^2 T_1^4 = 4\pi r_2^2 T_2^4
\]
Simplifying, we get:
\[
r_1^2 T_1^4 = r_2^2 T_2^4
\]
Step 4: Conclusion.
The ratio \( \frac{r_1}{r_2} \) is:
\[
\left( \frac{T_2}{T_1} \right)^2
\]
Hence, the correct answer is (A).