Let the mass per unit area be Then the mass of the complete disc =σ[π(2R)2]=4πσR2 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 discof 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 : 4πσ