The thin plate ABCD of mass 8 kg is held in the position shown by the wire BH and two links AE and DF. Neglecting the mass of the links, determine immediately after wire BH has been cut (a) the acceleration of the plate, (b) the force in each link.
Kinematics of Motion. After wire BH has been cut, we observe that corners A and D move along parallel circles of radius 150 mm centered, respectively, at E and F. The motion of the plate is thus a curvilinear translation; the particles forming the plate move along parallel circles of radius 150 mm.
At the instant wire BH is cut, the velocity of the plate is zero. Thus the acceleration a of the mass center G of the plate is tangent to the circular path which will be described by G.
Equations of Motion. The external forces consist of the weight W and the forces FAE and FDF exerted by the links. Since the plate is in translation, the effective forces reduce to the vector ma attached at G and directed along the t axis. A free-body-diagram equation is drawn to show that the system of the external forces is equivalent to the system of the effective forces.
a. Acceleration of the Plate.
+↙ΣFt=Σ(Ft)eff:Wcos30∘mgcos30∘aˉ=gcos30∘=maˉ=maˉ=(9.81 m/s2)cos30∘(1)
a=8.50m/s2 ⦫ 60∘
b. Forces in Links AE and DF.
+↖ΣFn=Σ(Fn)eff:FAE+FDF−Wsin30∘=0+↓ΣMG=Σ(MG)eff:(2)
(FAEsin30∘)(250 mm)−(FAEcos30∘)(100 mm)+(FDFsin30∘)(250 mm)+(FDFcos30∘)(100 mm)=038.4FAE+211.6FDF=0FDF=−0.1815FAE(3)
Substituting for FDF from (3) into (2), we write
FAE−0.1815FAE−Wsin30∘=0FAE=0.6109WFDF=−0.1815(0.6109W)=−0.1109W
Noting that W = mg = (8 kg)(9.81 m/s²) = 78.48 N, we have
FAE=0.6109(78.48 N)FDF=−0.1109(78.48 N)FAE=47.9 N T FDF=8.70 N C