Suppose there is a uniform circular disc of mass M kg and radius r m shown in figure. The shaded regions are cut out from the disc. The moment of inertia of the remainder about the axis A of the disc is given by $\frac{x{256} Mr^2$. The value of x is ___.
To find the value of x such that the moment of inertia of the remainder of the disc about axis A is given by –––x·256·Mr2, we need to calculate the moment of inertia of the original disc then subtract the moments of inertia of the cut-out regions.
1. Moment of Inertia of Original Disc: The moment of inertia of a full disc about its center is –––(1/2)·M·r2.
2. Moment of Inertia of Each Cut-Out: Each cut-out is a disc of radius r/4, and the moment of inertia for one cut-out about its center would be –––(1/2)·(M–-–-2)·(r/4)2 but we need it about A using parallel axis theorem: –––(1/2).(M/32)––r2/16––+M/32.(3r/4)2.
Substitute to find total contribution from one cut-out: –––(Mr2/128)––+9–xߝM/32×r2/16 = –––(r²/128)(1/2)...
3. Total Moment of Inertia of Remaining Part: Original - 2*cut-outs: –––(1/2)M·r2-(3–x-×-&Ks–x-(M–-—>––—5↑–)(Mr²/32(1.766)M–4.7118;r)}
4. Equating to Given Expression: Set equal: –––M*256 Find x so that solution within Expected Range:
Thus, x = 236M,
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\(^{-2}\).
