The increase in the length of a wire under an applied force is given by the formula:
\[
\Delta L = \frac{F L}{A Y}
\]
where:
- \( F \) is the applied force,
- \( L \) is the original length of the wire,
- \( A \) is the cross-sectional area of the wire, and
- \( Y \) is Young's modulus of the material.
Since the wires are made of the same material, the value of \( Y \) is the same for both wires. Also, the applied force \( F \) is the same for both wires. Therefore, the increase in length is proportional to the ratio \( \frac{L}{A} \).
The cross-sectional area \( A \) of a wire with diameter \( d \) is given by:
\[
A = \frac{\pi d^2}{4}
\]
Let the diameter of wire A be \( d_1 \) and the diameter of wire B be \( d_2 \). Since \( d_1 : d_2 = 1 : 2 \), we can write:
\[
A_1 = \frac{\pi d_1^2}{4}, \quad A_2 = \frac{\pi d_2^2}{4} = \frac{\pi (2 d_1)^2}{4} = 4 A_1
\]
Now, the increase in length for wire A and wire B will be:
\[
\frac{\Delta L_A}{\Delta L_B} = \frac{L_A / A_A}{L_B / A_B} = \frac{L_A A_B}{L_B A_A}
\]
Given that \( L_A : L_B = 1 : 3 \) and \( A_A : A_B = 1 : 4 \), we get:
\[
\frac{\Delta L_A}{\Delta L_B} = \frac{1 \times 4}{3 \times 1} = \frac{4}{3}
\]
Thus, the ratio of the increase in lengths of wires A and B is \( 4 : 3 \).