Let the initial mass entire disk = M
∴ Average mass/unit area = \(\frac {M}{(π R^2)}\)
mass of the unit cut out = \(\frac {M}{(π R^2)}\) π (R/2)2
∴ Mass of remaining planar object = M - \(\frac{M}{4}\) =\(\frac {3M}{4}\)
Consider region 1. it has a mass \(\frac{M}{4}\) and has a centre of mass (R/2,0)
Let the plane 2 has a centre of mass at (Xcm, Ycm) and has a man of (3M/4)
For the entire disc of radius R, the CM lies at (R, O)
From the definition, Rcm = \(\frac {∑m_ir_i}{∑m_i}\)
∴ The new CM is at (7R/6,0).