In this problem, we have two spring systems: the first system with spring constant \( k \) and the second system with two springs in series, each with spring constant \( k \). When two springs are arranged in series, the equivalent spring constant \( k_{\text{eq}} \) is given by:
\[
\frac{1}{k_{\text{eq}}} = \frac{1}{k} + \frac{1}{k} = \frac{2}{k}
\]
Thus, the equivalent spring constant for the second system is:
\[
k_{\text{eq}} = \frac{k}{2}
\]
Now, according to Hooke's Law:
\[
F = k \Delta x
\]
For the first system, the force required to stretch the spring by \( \Delta x \) is:
\[
F_1 = k \Delta x
\]
For the second system, since the equivalent spring constant is \( \frac{k}{2} \), the stretch \( \Delta x_2 \) for the same force is:
\[
F_2 = k_{\text{eq}} \Delta x_2 = \frac{k}{2} \Delta x_2
\]
Equating the forces in both systems, \( F_1 = F_2 \), we get:
\[
k \Delta x = \frac{k}{2} \Delta x_2
\]
Solving for \( \Delta x_2 \):
\[
\Delta x_2 = 2 \Delta x
\]
Thus, the stretch for the second system is \( \frac{\Delta x}{2} \).