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.
If the interval in which the real-valued function \[ f(x) = \log\left(\frac{1+x}{1-x}\right) - 2x - \frac{x^{3}}{1-x^{2}} \] is decreasing in \( (a,b) \), where \( |b-a| \) is maximum, then {a}⁄{b} =