Let mass per unit area of the original disc = σ
Thus mass of original disc = M = σπR2
Radius of smaller disc = R/2.
Thus mass of the smaller disc = σπ(R/2)2 = M/4
After the smaller disc has been cut from the original, the remaining portion is considered to be a system of two masses. The two masses are:
M(concentrated at O), and -M(=M/4) concentrated at O'
(The negative sign indicates that this portion has been removed from the original disc.)
Let x be the distance through which the centre of mass of the remaining portion shifts from point O.
The relation between the centres of masses of two masses is given as:
\(x = \frac{(m_1r_1 + m_2r_2)}{m_1 + m_2}\)
\(= (M \times 0 - \frac{M}{4}) \times \frac{\frac{R}{2}}{M - \frac{M}{4}} = \frac{-R}{6}\)
(The negative sign indicates that the centre of mass gets shifted toward the left of point O)
