Since the distance between point D and C varies, two frames of reference is useful to solve the problem. Attach the local x-y coordinate to the rotating AE rod, and the global X-Y coordinate to the non-moving background.
Velocities:
Before accelerations can be found, the velocity of point C, vC/D, and angular velocity of ΩDE (= ΩDC) needs to be determined.
vC = vD + Ω × rC/D + ( vC/D)rel
vC = vD + ΩDC× rC/D + vC/D
vD = 0
ωAB = 4k
rC/D = 0.5 m i
ΩDC = ωDC
Since distance from A and C does not change, velocity of C can be determined from bar AB
vC = ωAB × rC/A = -4k × (0.5i
+ 0.5j)
=
2i - 2j m/s
Putting all terms together gives,
2i - 2j = 0 + (-ωDC
k) × (0.5i) + vC/D
reli
2i - 2j = -0.5ωDC
j + vC/D rel i
Comparing the i and j terms give
vC/D = 2 m/s and ωDC = 4 rad/s
Accelerations:
aC = aD + dΩDC/dt × rC/D + ΩDC× (ΩDC × rC/D)
+
2ΩDC × vC/D + aC/D
aC = aD + αDE × rC/D + ωDE× ( ωDE × rC/D)
+
2ωDE × vC/D + aC/D
where,
aD = 0
rC/D = 0.5i m
αDC = (-αDCk) × 0.5i = -0.5αDEj m/s2
ωDC × ( ωDC × rC/D) = (- 4)2 (0.5 i) = -8i rad/s
2ωDC × vC/D = 2 (-4k) × 2i = 16j m/s2
aC/D =
aC/Di
Acceleration of C can be determined from bar AC
aC = αAC × rC/A - ω2 rC/A
= -5k × (0.5i + 0.5j) - (4)2 (0.5i + 0.5j)
= -5.5i - 10.5j m/s2
-5.5i - 10.5j = 0 + (-αDEk)× 0.5i - (- 4)2 (0.5 i)
+
2 (-4k)×2i +
(aC/D)i
Putting all terms together gives,
-5.5i - 10.5j = 0 - 0.5αDCj
- 8i - 16j + aC/Di
Comparing the j terms
-10.5 = -16 - 0.5αDE
αDC = -11 rad/s2
αDC = 11k rad/s2 (counter-clockwise) |