A thin uniform disc of mass M and radius R is rotating in a horizontal plane about an axis passing through its centre and perpendicular to it with angular velocity ω. Another disc of the same radius but of mass M4 is placed gently on the first disc coaxially. The angular velocity of the system will now finally change to:
Given,
First mass =M
Second Mass =M4
From conservation of momentum
Final momentum = initial Momentum
Mω′R2+M4ω′R2=MωR2
ω′=MωR2MR2+M4R2=4ω5
Final Angular velocity is 4ω5