Pendulum on a Cart - Is There a Max Swing Angle?

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SUMMARY

The discussion centers on the dynamics of a pendulum attached to a cart that collides with an inelastic barrier. The key conclusion is that the maximum angle through which the pendulum can swing depends on the initial velocity (v) of the cart and the length (l) of the pendulum. Specifically, if the parameter \(\frac{v^{2}}{2gl} \geq 1\), the pendulum will swing in circles; otherwise, it will swing to a maximum angle determined by energy conservation principles. The participants agree that the professor's assertion of a maximum angle is misleading, as the pendulum can indeed complete a full swing if the velocity is sufficiently high.

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  • Understanding of conservation of mechanical energy
  • Familiarity with pendulum dynamics
  • Knowledge of inelastic collisions
  • Basic physics concepts such as gravitational potential energy
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  • Calculate the maximum angle of a pendulum using energy conservation principles
  • Explore the effects of varying the initial velocity on pendulum motion
  • Investigate the conditions for a pendulum to complete a full circular swing
  • Study the implications of inelastic collisions on attached objects
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Physics students, educators, and anyone interested in the mechanics of pendulums and collision dynamics will benefit from this discussion.

ragidandy
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Please help; I think my professor might be wrong,

A cart travels toward an inelastic barrier at a constant speed v. On the cart is a pendulum that is not oscillating before the collision. (It is hanging straight down and traveling at the same speed as the cart.)

The cart then collides (perfectly inelastically) with the barrier and comes to a complete stop instantaneously. The pendulum support is fixed to the cart and comes to a complete stop, but the pendulum is free to swing.

Question: What is the maximum angle through which the pendulum can swing for an arbitrary v?

The puzzle:
My professor contends that there is a maximum angle, and I contend that there is not (the pendulum will swing in circles for a high enough v.)

If you think my professor is wrong, I agree, but that's not the question. If you think I am wrong, please be specific about the physics. The question is what train of thought (or physical approximation) would lead to his conclusion that there is a maximum angle to which the pendulum can swing? I cannot ask the professor, as he is trying so hard to be coy.

Thanks.
 
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I'm with you.

Assuming the usual ideal conditions for these kinds of pendulum questions (including the use of a rigid massless rod), the total energy of the pendulum's mass at the instant of collision is E=mv^2/2. Of course, v is the velocity of the cart/pendulum at impact and m is the mass of the bob. If the length of the rod is L then the maximum gravitational potential energy V that can be realized is 2mgL. If E<V the pendulum will swing up to some angle less than pi and proceed to swing back and forth. If E=V the bob will swing up through an angle of pi and come to rest balanced directly above the pivot point. If E>V the mass will rotate about the pivot point. [Unless I'm missing something here...]
 
The point is, you can calculate a maximum angle. For a high enough v it will go over, but you don't know beforehand if it's a high enough v. So you should find the formula for the angle from energy conservation. I suppose that's all the prof wants.
 
Your professor is dead wrong.
If the parameter \frac{v^{2}}{2gl}\geq{1}, the pendulum will swing in circles.
(g is the acceleration due to gravity, l the length of the pendulum, v being the initial velocity)
 
I don't see any implication in the professor's question that he thinks the pendulum cannot swing in a circle if v is large enough. He merely asks you to do the calculation for arbitrary v (note that v may or may not be large enough to swing over the top). He's being "coy" because he probably wants you to realize on your own that for speeds above some minimum the pendulum will make a complete swing. Specify that minimum speed and, for speeds below that limit, specify the maximum angle.
 
arildno said:
If the parameter \frac{v^{2}}{2gl}\geq{1}, the pendulum will swing in circles.
(g is the acceleration due to gravity, l the length of the pendulum, v being the initial velocity)
How did you arrive at that relationship?
 
Doc Al said:
How did you arrive at that relationship?
Well, I made a quick idealization:
After the collision (conceived as instantaneous), the fulcrum is at rest. Since the collision was perceived as instantaneous, no change in the position of the (mathematical) pendulum has occurred, i.e, it is hanging straight down.
Therefore, the bob of mass m
has retained its velocity v, since it has experienced no horizontal force during the collision.
(The pendulum string could, and have, only have transmitted forces in the vertical direction during the collision).


The relation follows easily from that, by conservation of mechanical energy, and the requirement that the value of, say, the cosine function, must be less than 1.
 
arildno said:
The relation follows easily from that, by conservation of mechanical energy, and the requirement that the value of, say, the cosine function, must be less than 1.
Looks to me like you set the initial KE equal to just enough for the pendulum bob to reach the height of the support, not necessarily enough to swing through a complete circle.
 
Doc Al said:
Looks to me like you set the initial KE equal to just enough for the pendulum bob to reach the height of the support, not necessarily enough to swing through a complete circle.
Oh dear, you are absolutely right. My mistake.

The critical condition should have an extra factor of 2 in its denominator.
 
  • #10
ragidandy:
Your prof's use of the term "maximum angle" probably just refers to the fact that a real pendulum would not swing quite so much, so your calc would be a maximum possible angle for a given v.
 
  • #11
Thank you all.

I think you must be right in that my prof. was looking for the angle as a function of v when v is below the critical value. Such trouble I make for myself!
 

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