Since the distance BC is not constant, this problem is well suited for using two frames of reference. Fix the local frame of reference, x-y, on bar BCD so that the motion of C can be easily modeled relative to B, (rC/B)rel. Then the velocity of C is,
vC = vB + Ω × rC/B + (vC/B)rel
This equation includes the unknown angular velocity of bar BD, Ω = ΩBC = ΩBD, that is required, and can be determined. The global frame of reference is fixed to the background and is not moving.
The velocity of B is zero (it is pinned).
vB = 0
The velocity of C with respect to B, vC/B, is
vC/B = -vC/Bi = -vC/Bcos45I - vC/Bsin45J m/s
The velocity of point C, based on the motion of bar AC, in the global coordinate system is
vC = -ωACrAC J = -3(0.15)J = -0.45J m/s
The relative position of C with respect to B is
rC/B = 0.15/cos45i = 0.15I + 0.15J m
Putting all the terms together, gives
-0.45J = -vC/Bcos45I - vC/Bsin45J + 0 +
+ ΩBDK × (0.15I + 0.15J)
-0.45J = -0.7071vC/BI - 0.7071vC/BJ +
+
0.15ΩBDJ -
0.15ΩBDI
Summing the I terms gives,
0.7071vC/B= -0.15 ΩBD
vC/B= -0.2121ΩBD
Summing J terms:
-0.45 = -0.7071 (-0.2121ΩBD) + 0.15ΩBD
ΩBD = -1.50K rad/s
ΩBD = 1.50 rad/s |