A uniform rigid rod of mass M and length L is hinged at one end as shown in the adjacent figure. A force P is applied at a distance of 2L3 from the hinge so that the rod swings to the right. The horizontal reaction at the hinge is
0
at this moment
ω=0
but α≠0[start of rotation]
→aCM=→ar+→at
(because centre of mass is in circular motion at a radius L2)
→ar=0[∴ω=0]
→aCM=→at=L2α(^i)
Torque, T=Iα (about hinge)
Taking moment about A,
P×2L3=ML23α
α=2PML
→aCM=L2×2PML^i
→aCM=PM^i
Let R be the reaction in horizontal direction at hinge:
[In horizontal direction]
(Σ→f)ext=M→aCM
P+R=MaCM
P+R=M×PM
P+R=P
R=0