The problem involves two spherical black bodies radiating the same amount of heat per second. According to Stefan-Boltzmann Law, the power radiated \( P \) by a spherical black body is given by:
\[ P = \sigma A T^4 \]
where \( \sigma \) is the Stefan-Boltzmann constant, \( A \) is the surface area, and \( T \) is the temperature of the black body.
For a sphere, the surface area \( A = 4\pi R^2 \). Thus, the power radiated by each sphere can be given as:
\[ P_1 = \sigma (4\pi R_1^2) T_1^4 \]
\[ P_2 = \sigma (4\pi R_2^2) T_2^4 \]
Since both bodies radiate the same amount of heat per second, we equate \( P_1 \) and \( P_2 \):
\[ \sigma (4\pi R_1^2) T_1^4 = \sigma (4\pi R_2^2) T_2^4 \]
We can cancel \(\sigma\) and \(4\pi\) from both sides:
\[ R_1^2 T_1^4 = R_2^2 T_2^4 \]
Rearranging the equation, we get:
\[ \left(\frac{T_1}{T_2}\right)^4 = \left(\frac{R_2}{R_1}\right)^2 \]
Taking the fourth root on both sides:
\[ \frac{T_1}{T_2} = \left(\frac{R_2}{R_1}\right)^{1/2} \]
Now, if we assume the relation \( T_1 = \sqrt{2} T_2 \), it implies:
\[ \frac{T_1}{T_2} = \sqrt{2} \]
Thus, \(\left(\frac{R_2}{R_1}\right)^{1/2} = \sqrt{2}\).
Since both sides match, the correct relation is indeed \( T_1 = \sqrt{2} T_2 \).