To solve this problem, we need to use the concept of elasticity and specifically the formula for elongation due to a tensile force. The elongation (\( \Delta L \)) of a material subjected to a force is given by:
\(\Delta L = \frac{FL}{A \cdot Y}\)
where:
For the first wire:
The cross-sectional area \( A \) for the first wire is \( \pi r^2 \).
The elongation is given by:
\(l = \frac{fL}{\pi r^2 Y}\)
For the second wire:
The cross-sectional area \( A \) for the second wire is \( \pi (2r)^2 = 4\pi r^2 \).
The elongation \( \Delta L \) for the second wire is given by:
\(\Delta L = \frac{(2f)(2L)}{4\pi r^2 Y}\)
Simplifying the expression:
\(\Delta L = \frac{4fL}{4\pi r^2 Y} = \frac{fL}{\pi r^2 Y} = l\)
Thus, the elongation in the second wire is the same as in the first wire, which is \( l \). Therefore, the correct answer is l.