Let σ be the mass per unit area of the disc. Then the mass of the complete disc =σ(π(2R)2)
The mass of the removed disc =σ(πR2)=πσR2 Let us consider the above situation to be a complete disc of radius 2R on which a disc of radius R of negative mass is superimposed. Let O be the origin. Then the above figure can be redrawn keeping in mind the concept of centre of mass as :