The force in a wire is given by Hooke's Law:
\[
F = kx
\]
Where:
- \( F \) is the applied force,
- \( k \) is the spring constant, and
- \( x \) is the elongation in the wire.
From the problem statement, we are given that:
\[
F = k \Delta x
\]
Now, for tensions \( F_1 = 100 \, \text{N} \) and \( F_2 = 120 \, \text{N} \), the corresponding lengths of the wire will be:
For \( F_1 \):
\[
100 = k (l_1 - l_0) \quad \text{(1)}
\]
For \( F_2 \):
\[
120 = k (l_2 - l_0) \quad \text{(2)}
\]
Now, let the natural length of the wire be \( l_0 \). From the given information, \( l_1 = 11l_0 \).
From equation (1), we can write:
\[
100 = k(11l_0 - l_0) \Rightarrow k(10l_0) = 100
\]
Thus,
\[
k = \frac{10}{l_0}
\]
Substituting into equation (2):
\[
120 = \frac{10}{l_0} (l_2 - l_0)
\]
\[
l_2 - l_0 = \frac{120 l_0}{10} = 12 l_0
\]
Thus,
\[
l_2 = 13 l_0
\]
The ratio of \( l_2 \) to \( l_1 \) is:
\[
\frac{l_2}{l_1} = \frac{13 l_0}{11 l_0} = \frac{13}{11}
\]
Therefore, \( x = 2 \).