A particle of mass 'm' moving with velocity 'V', hits to a stationary disc of mass M and radius R and sticks to the disc on its rim. The angular velocity of the disc with which it starts to rotate about its centre is
Here we consider both the particle and disc as a single system
∴ Torque due to internal forces do not change the angular momentum of the system.
∴Li=Lf where Li=mVR [w.r.t the centre of disc]
Lf=Iω+mR2ω [w.r.t the centre of disc]
∴mVR=Iω+mR2ω
⇒mVR=MR22ω+mR2ω
⇒ω=VR−M2m