Step 1: Understanding the Concept:
Rotational kinetic energy is \(E = \frac12I\omega^2\). For a thin uniform rod of mass \(M\) and length \(L\) about its centre, \(I = \frac{ML^2}{12}\).
Step 2: Find the mass and I:
\(L = 2\) m, so \(M = \text{volume}\times\text{density} = A\cdot2\cdot d = 2Ad\).
\[ I = \frac{2Ad\times4}{12} = \frac{2Ad}{3} \]
Step 3: Solve for omega:
\(E = \frac12\cdot\frac{2Ad}{3}\omega^2 = \frac{Ad\,\omega^2}{3}\), so \(\omega^2 = \frac{3E}{Ad}\), and \(\omega = \left(\frac{3E}{Ad}\right)^{1/2}\).
Comparing with \(\left(\frac{\alpha E}{Ad}\right)^{1/2}\): \(\alpha = 3\).
Final Answer:
The value of \(\alpha\) is \(3\), option (B).
\[ \boxed{3} \]