The moment of inertia of a rod about an axis through its center and perpendicular to its length is \( \alpha = \frac{ML^2}{12} \), where \( M \) is mass and \( L \) is length. When the rod is divided into two equal segments, each segment has mass \( \frac{M}{2} \) and length \( \frac{L}{2} \). The moment of inertia for each segment is denoted by \( \alpha' \). For a cross shape, the total moment of inertia is the sum of the moments of inertia of the two segments, accounting for their distances from the rod's center. Applying the parallel axis theorem yields: \[ \alpha' = 2 \times \frac{M L^2}{48} = \frac{\alpha}{4} \] Consequently, the correct moment of inertia is \( \frac{\alpha}{4} \).
Two point charges 2q and q are placed at vertex A and centre of face CDEF of the cube as shown in figure. The electric flux passing through the cube is : 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
