Let the moment of inertia of the rod about the axis passing through its center and normal to its length be \( \alpha = \frac{ML^2}{12} \), where \( M \) is the mass and \( L \) is the length.
Now, the rod is cut into two equal parts, each having mass \( \frac{M}{2} \) and length \( \frac{L}{2} \).
Each part has a moment of inertia \( \alpha' \).
For the cross shape, the total moment of inertia will be the sum of the moments of inertia of the two parts, considering the distance from the center of the rod.
After using the parallel axis theorem, we get: \[ \alpha' = 2 \times \frac{M L^2}{48} = \frac{\alpha}{4} \] Thus, the correct option is \( \frac{\alpha}{4} \).
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is: