Correct Answer - A::B::D
In the absence of horizontal external force centre of mass of system S falls vertically. Since mass of ring and particle are equal their motion about CM of system is symmetrical. At given instant centre of ring will be instantaneous centre
From work energy theorem
`mgr=(1)/(2)mv_(1)^(2)+(1)/(2)mr^(2)omega^(2)`
also `v_(1)=romega`
thus `v_(1)=sqrt(gr)`
`|vec(a)_(C )|=|vec(a)_(1)|=(v_(rel)^(2))/((r//2))=(v_(1)//2)^(2)/(r//2)=(g)/(2)`
`[v_(rel)=v_(1)-v_(S)=(v_(1))/(2)]`
At the given instant acceleration of particle is equal to the centripetal acceleration of its rotaion about centre of mass.
`N,(r)/(2)=(3)/(2) mr^(2)alpha " " ....(i)`
`a_(s)=(r)/(2)alpha" "...(ii)`
`a_(s)=(2mg-N)/(2m)" "...(iii)`
Thus `N=(3)/(2)mg`