Tutorial 6
16−70.
If the slider block C is moving at $v_{C}=3 \mathrm{~m} /...
Sep 30, 2024
Solution by Steps
step 1
Given that the slider block C is moving at vC=3m/s, we can find the angular velocity of the crank AB using the relationship between linear and angular velocity. The length of crank AB is 0.5m, so the angular velocity ωAB can be calculated as:
ωAB=LABvC=0.53=6rad/s.
step 2
To find the angular velocity of the rod BC, we need to consider the geometry of the system. The angle between crank AB and the horizontal is 60∘, and the angle between rod BC and the horizontal is 45∘. The relationship between the angular velocities can be expressed as:
ωBC=ωAB⋅LBCLAB⋅cos(60∘)=6⋅10.5⋅cos(60∘)=6⋅0.5⋅0.5=1.5rad/s.
step 3
Therefore, the angular velocities of the crank AB and the rod BC at the instant shown are:
ωAB=6rad/s,ωBC=1.5rad/s.
Answer
Angular velocity of crank AB is 6rad/s and angular velocity of rod BC is 1.5rad/s.
Key Concept
The relationship between linear and angular velocity in mechanical systems.
Explanation
The angular velocities are derived from the linear velocity of the slider block and the geometry of the system, demonstrating how motion is transmitted through connected components.
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Solution by Steps
step 1
For the spool rolling without slipping, the relationship between the linear velocity v of the cable and the velocity of the center O of the spool can be expressed as:
v=R⋅ω,
where R is the radius of the spool and ω is the angular velocity of the spool
step 2
Since the spool rolls without slipping, the linear velocity of the center O is equal to the velocity of the cable being pulled. Therefore, we can express the velocity of the center O as:
vO=v.
step 3
Thus, the velocity of the center O of the spool when the cable is pulled to the right with a velocity v is:
vO=v.
Answer
The velocity of the center O of the spool is equal to the velocity v of the cable being pulled.
Key Concept
The relationship between linear velocity and angular velocity in rolling motion.
Explanation
The center of the spool moves with the same velocity as the cable due to the no-slip condition, illustrating the connection between linear and angular motion in rolling objects.