Step 1: Understanding the Concept:
Total energy of a simple pendulum for small oscillations is $E = \frac{1}{2} m \omega^2 A^2$, where $\omega = \sqrt{g/L}$.
Step 2: Formula Application:
$E = \frac{1}{2} M \left( \frac{g}{L} \right) A^2 \implies E \propto \frac{A^2}{L}$ (since $M$ and $g$ are constant).
Step 3: Explanation:
For $E_A = E_B$: $\frac{A_A^2}{L_1} = \frac{A_B^2}{L_2}$.
Given $L_1 = 2L_2$, so $\frac{A_A^2}{2L_2} = \frac{A_B^2}{L_2} \implies A_A^2 = 2 A_B^2$.
Wait, looking at the math: $A_B^2 = \frac{1}{2} A_A^2$, so $A_B < A_A$. However, let's check the energy formula $E = mgh$. For same energy, $h_1 = h_2$. $h = L(1-\cos\theta) \approx L \frac{\theta^2}{2} = \frac{A^2}{2L}$.
If $A^2/2L$ is constant, then $A^2 \propto L$. Since $L_1 > L_2$, $A_A > A_B$.
Therefore, amplitude of B is smaller than A.
Step 4: Final Answer:
Amplitude of B is smaller than amplitude of A.