The elongation \( \Delta L \) of a wire under a stretching force \( F \) is described by \( \Delta L = \frac{F L}{A Y} \), where \( L \) is the wire's length, \( A \) is its cross-sectional area, and \( Y \) is the Young's modulus. Given that \( Y \) is constant for both wires as they are of the same material, and the applied force \( F \) is also the same for both, the elongations are determined by the wire lengths and areas.
Step 1: Wire Dimensions
The lengths of wire A and wire B are related by \( \frac{L_A}{L_B} = \frac{1}{3} \), implying \( L_A = \frac{L_B}{3} \). The cross-sectional area \( A \) of a wire is given by \( A = \frac{\pi d^2}{4} \), where \( d \) is its diameter. The ratio of the areas of wires A and B is \( \frac{A_A}{A_B} = \left( \frac{d_A}{d_B} \right)^2 \). Since \( \frac{d_A}{d_B} = 2 \), it follows that \( \frac{A_A}{A_B} = 2^2 = 4 \), or \( A_A = 4 A_B \).
Step 2: Elongation Ratio Calculation
The ratio of the elongations \( \Delta L_A \) to \( \Delta L_B \) is computed as follows:
\[ \frac{\Delta L_A}{\Delta L_B} = \frac{F L_A / A_A Y}{F L_B / A_B Y} \]
This simplifies to:
\[ \frac{\Delta L_A}{\Delta L_B} = \frac{L_A}{L_B} \times \frac{A_B}{A_A} \]
Substituting the derived ratios:
\[ \frac{\Delta L_A}{\Delta L_B} = \frac{1/3}{1} \times \frac{1}{4} = \frac{1}{12} \]
Therefore, the ratio of the elongations is \( 1 : 12 \), corresponding to option (2).