For a wire under tension, the elongation $\Delta L$ is given by:
\[
\Delta L = \frac{F L}{A Y}
\]
where:
$F$ is the force,
$L$ is the length of the wire,
$A$ is the cross-sectional area, and
$Y$ is the Young's modulus.
Since the elongation is the same for both wires, we can equate the elongations:
\[
\frac{F L}{A_B Y_B} = \frac{F L}{A_S Y_S}
\]
The cross-sectional area $A = \pi r^2$, so:
\[
\frac{r_B^2}{Y_B} = \frac{r_S^2}{Y_S}
\]
Thus, we find:
\[
r_S = \frac{r_B}{\sqrt{2}}
\]