Angular Acceleration and relative velocity

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SUMMARY

The discussion focuses on calculating the angular velocity and acceleration of link 3 in a mechanical system where link 2 has a constant angular velocity of 17 rad/s clockwise. The calculations involve using the law of sines and cosines to determine the distances and angles, leading to the angular velocity of link 3 being approximately 7.94 rad/s clockwise. Additionally, the relative velocity of point B with respect to link 2 is calculated to be around 808 mm/s. The participants emphasize the importance of understanding tangential and relative acceleration components in this context.

PREREQUISITES
  • Understanding of angular kinematics and dynamics
  • Familiarity with the law of sines and cosines
  • Knowledge of relative velocity concepts in mechanical systems
  • Proficiency in differentiating equations with respect to time
NEXT STEPS
  • Study the application of the law of sines in mechanical linkages
  • Learn about angular acceleration and its calculation in multi-link systems
  • Explore the concept of relative velocity in rigid body dynamics
  • Investigate the differentiation of parametric equations in motion analysis
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Mechanical engineers, students studying kinematics, and professionals involved in the design and analysis of mechanical linkages will benefit from this discussion.

Jonski
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Homework Statement


Question7.png

In the mechanism shown below, the angular velocity of link 2 is 17 rad/s CW, constant. Find the angular velocity (magnitude and direction) of link 3. The distance between A and C is 109 mm, the length of link 3 is 125 mm, and θ= 111°. Note: B is a pin-slider

In the mechanism shown above, find the relative velocity (magnitude) of point B with regards to link 2.

In the mechanism shown above, find the direction of the relative velocity of point B with regards to link 2. Take the right-hand direction as a reference axis and CCW positive.

In the mechanism shown above, determine the angular acceleration (magnitude and direction) of link 3.

Homework Equations


a3 = a3t + a3n + a rel + a cor
a3t = αr
a3n = ω^2r
a cor = 2ωv

The Attempt at a Solution


So I have done the first 3 parts of the question correctly getting
-7.853rad/s = wab
0.800m/s = Vb
-291deg

I am not sure how to get the acceleration though. I'm not sure how to find the tangential component and the relative acceleration.
Thanks
 
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You have the magnitude and the velocity of point B. If BC is of constant length, what is the component of the velocity of point B along the link BC? What does this tell you about the component of the velocity of point B perpendicular to the link BC?
 
Chestermiller said:
You have the magnitude and the velocity of point B. If BC is of constant length, what is the component of the velocity of point B along the link BC? What does this tell you about the component of the velocity of point B perpendicular to the link BC?
Does it have something to do with the fact that since the angular velocity of bar AB is constant the tangential acceleration of bar AB is 0.
 
Jonski said:
Does it have something to do with the fact that since the angular velocity of bar AB is constant the tangential acceleration of bar AB is 0.
No. Please try to answer my questions. If you have trouble with the first question, I'll tell you the answer.
 
Chestermiller said:
No. Please try to answer my questions. If you have trouble with the first question, I'll tell you the answer.
Wouldn't the velocity perpendicular to BC be equal to:
Vb = Vb' + Vb/b'
Vb = 17(0.0335) + 0.8
Vb = 1.37 m/s
 
I originally misinterpreted this question, so I'm going to start over by first checking your answers. Let ##\alpha## be the angle ABC and ##\phi## be the angle ACB. Using the law of sines, $$\frac{\sin{\alpha}}{109}=\frac{\sin{\theta}}{125}$$
So ##\alpha=54.5## degrees. That means that ##\phi = 180 -111-54.5=14.5## degrees.
Let r equal the distance of point B from point A. Again using the law of sines:
$$\frac{\sin 14.5}{r}=\frac{\sin{\theta}}{125}$$Solving for r yields: ##r=33.53## mm.

The law of cosines tells us that: $$r^2+109^2-2(109)r\cos{\theta}=125^2$$
If we differentiate this equation with respect to time, we obtain: $$2r\frac{dr}{dt}-2(109)\cos{\theta}\frac{dr}{dt}+2(109)r\sin{\theta}\frac{d\theta}{dt}=0$$
Solving for dr/dt yields:
$$\frac{dr}{dt}=-\frac{109r\sin{\theta}}{r-109\cos{\theta}}\frac{d\theta}{dt}=\frac{109r\sin{\theta}}{r-109\cos{\theta}}\omega\tag{1}$$
Substituting our values for r and ##\theta## in this equation yields:$$\frac{dr}{dt}=808\ mm/s$$This is the velocity of point B relative to link 2, and is very close to your answer.

The law of sines tells us that $$\frac{\sin{\phi}}{r}=\frac{\sin{\theta}}{125}$$
Differentiating this equation with respect to time yields:
$$\cos{\phi}\frac{d\phi}{dt}=\frac{\sin{\theta}}{125}\frac{dr}{dt}-\frac{r\cos{\theta}}{125}\omega\tag{2}$$
From this, I get that the angular velocity of link 3 is 7.94 radians per second CW. This is also close to your answer, but not quite.

For the direction of the velocity of B relative to link 2, I get that it is along link 2.

To get the angular acceleration of link 3, I would differentiate Eqns. 1 and 2 with respect to t and combine the results, taking into account that ##d\theta /dt## is constant.
 

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