Step 1: Plan:
Think of the rod as two halves, each of length $1$ m, spinning about one end.
Step 2: Steps:
Each half has mass $Ad$ and moment of inertia about its end $\frac{(Ad)(1)^2}{3} = \frac{Ad}{3}$. The two halves together give $I = \frac{2Ad}{3}$.
From $E = \frac12I\omega^2$, $\omega^2 = \frac{2E}{I} = \frac{2E\cdot3}{2Ad} = \frac{3E}{Ad}$. So $\alpha = 3$.
Final Answer:
The value of $\alpha$ is $3$, option (B).
\[ \boxed{3} \]