As there is no friction, the mechanical energy will remain constant. Let us apply the conservation of mechanical energy between the vertical position
(A) and the horizontal position
(B).
Using
ΔK+ΔU=0 (12IAω2−0)+(−mgL2)=0which gives
ω=√3gLConsidering the free-body diagram of the bar at this instant, the velocity of COM of bar at this instant is given below.
Let
α be the angular acceleration of bar about
A at the instant when it becomes horizontal.
α=τAIA=mgL2mL23=32gLLet
Nx and
Ny are the components of reaction at
A. Then in horizontal direction
Nx=mar=mω2(L2) in vertical direction and
mg−Ny=mat........(i)and
at=acceleration of COM in y-direction
=(L/2)aor,
Ny=mg−m(L2α)=mg−3mg4=mg4........(ii)Therefore, resultant reaction at support
A is
N=√Nx2+Ny2N=√(3mg2)2+(mg4)2=√374mgtanα=NyNx=mg/43mg/2=16⇒α=tan−1(16)Therefore, reaction at pivot is
√374mg at an angle
α=tan−1(16) with horizontal.