Step 1:
The energy stored in a stretched wire is given by:
\[
E = \frac{1}{2} \cdot \frac{T L}{A} \cdot \Delta L
\]
where:
- \( E \) is the energy stored,
- \( T \) is the tension in the wire,
- \( L \) is the length of the wire,
- \( A \) is the cross-sectional area of the wire,
- \( \Delta L \) is the elongation of the wire.
Step 2:
The elongation \( \Delta L \) is proportional to \( \frac{L}{A} \) for a constant tension \( T \). Hence, we focus on the expression for the energy stored.
Step 3:
For wires A and B, the energy stored is proportional to:
\[
E \propto \frac{L}{A}
\]
Since the length of wire A is twice that of wire B (\( L_A = 2L_B \)), and the diameter of wire A is twice that of wire B (\( d_A = 2d_B \)), the cross-sectional area \( A \) is proportional to \( d^2 \), so:
\[
A_A = \pi \left( \frac{d_A}{2} \right)^2 = 4 \pi \left( \frac{d_B}{2} \right)^2 = 4A_B
\]
Step 4:
The ratio of the energies stored in wires A and B is:
\[
\frac{E_A}{E_B} = \frac{L_A / A_A}{L_B / A_B} = \frac{2L_B / 4A_B}{L_B / A_B} = \frac{2}{4} = \frac{1}{2}
\]
Step 5:
Thus, the ratio of the energies stored in wires A and B is \( 1:2 \), so Option (3) is correct.