By Hooke's law, we have the relation for the elongation of a wire due to force:
\( \gamma = \frac{F}{A} = \frac{\Delta L}{L} \)
where \( A \) is the cross-sectional area and \( L \) is the length of the wire. The elongation is directly proportional to \( F \) and \( L \), and inversely proportional to the area. The change in length is given by:
\( \Delta L = \frac{F L}{A} = \frac{F L}{\pi r^2} \)
For the second wire, we can write:
\( \frac{\Delta L_2}{\Delta L_1} = \frac{F_2 L_2}{F_1 L_1} \times \frac{A_1}{A_2} \)
Given that \( L_2 = 2L \), \( r_2 = 2r \), and \( F_2 = 2F \), we have:
\( \frac{\Delta L_2}{\Delta L_1} = \frac{2F \times 2L}{F \times L} \times \frac{\pi r^2}{\pi (2r)^2} \)
\( \frac{\Delta L_2}{\Delta L_1} = \frac{4F L}{F L} \times \frac{1}{4} = 1 \)
Thus, the elongation of the second wire is equal to that of the first wire.
Therefore, the ratio \(\frac{\Delta L_2}{\Delta L_1}\) is 1.

Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to: