No external torques act on the system consisting of the child and the merry-go-round, so the total angular momentum of the system is conserved.
An object moving a straight line has angular momentum about any point that is not on the line. The magnitude of the angular momentum of the child the center of the merry-go-round is given by Eq. 11−21,mvR, where R is the radius of the merry-go-round.
The initial angular momentum is given by Lf=Lchild=mvR
; the final angular momentum is given by Lf=(I+mR2)w, where w is the final common angilar velocity of the merry-go-round and child. Thus mvR=(I+mR2)w and
w=mvRI+mR2=158 kg.m2/s149 kg.m2+(44.0 kg)(1.20 m)2=0.744 rod/s.
Note:The child initially had an angular velocity of
w=vR=3.00 m/s1.20 m=2.5 rod/s.
After he jumped onto the merry-go-round, the rotational inertia of the system (merry-go-round+child)increases, so the angular velocity decreases.