Rolling Can with Rubber Band and Plasticine

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Discussion Overview

The discussion revolves around the mechanics of a rolling can that utilizes a rubber band and plasticine, exploring the reasons behind its behavior when rolled and how it returns after stopping. Participants delve into the theoretical underpinnings of the motion, including concepts of angular momentum, oscillation, and the effects of friction.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes a mechanism where a weight attached to the rubber band causes it to wind up as the can rolls, leading to a return motion when unwound.
  • Another participant questions this mechanism, arguing that the inner mass would gain angular velocity and continue rolling, thus contradicting the observed behavior of the can returning.
  • Some participants propose that the inner mass does not roll but hangs from the rubber band, which winds up without rolling, potentially allowing the can to return.
  • There is a suggestion that empirical testing with a transparent tube could clarify the mechanics at play.
  • Concerns are raised about damping effects from friction and how they might influence the expected oscillatory motion of the can.
  • One participant compares the setup to a scenario involving a vise and a metal rod to illustrate how external forces can affect oscillation and equilibrium.
  • Another participant emphasizes the rubber band as a potential energy storage device that can release energy at different times, contributing to the can's motion.

Areas of Agreement / Disagreement

Participants express differing views on the mechanics of the can's motion, with no consensus reached on the exact reasons for its behavior. Some agree on the role of the rubber band, while others challenge the interpretations of motion and energy transfer.

Contextual Notes

Participants note the complexity of the system, including the effects of friction and the assumptions about the inner mass's behavior, which remain unresolved. The discussion reflects various interpretations of the mechanics involved without reaching a definitive conclusion.

Jeno
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Imagine that now i have a can. I poke a hole at the centers of both the bottom and the cover of the can. Then i tie a rubber band onto the holes that it goes across the tin from the hole at the bottom to the hole on the cover. After that i stick some plasticine onto the rubber band. When i roll the can, it will stop and come back to me. What is the mechanism inside the can that make it stops and comes back? Thank you for answering my question.
 
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I think I made one of those when I was in cub scouts!

There is a heavy washer or other weight attached to the rubber band. As the can rolls, the weight causes the rubber band to wind up. When the can comes to a halt, the rubber band unwinds, sending the can back the other way.
 
Thank you for answering my question. But the problem is when the can rolls, the rubber band is twisted and the inner mass will also roll. thus, when the can stops, the inner mass will gain a angular velocity. it will continue to roll and this will unwind the rubber band as well. therefore, there will no any angular momentum that rolls the can back. this is, however, not match with the reality where the can really rolls back. so, can you explain why? thank you. -Jeno-
 
If the innner mass rolls until the rubber band unwinds, the can will not return.
 
Jeno said:
Thank you for answering my question. But the problem is when the can rolls, the rubber band is twisted and the inner mass will also roll. thus, when the can stops, the inner mass will gain a angular velocity. it will continue to roll and this will unwind the rubber band as well. therefore, there will no any angular momentum that rolls the can back. this is, however, not match with the reality where the can really rolls back. so, can you explain why? thank you. -Jeno-
The inner mass does not roll. It hangs from the rubber band, causing the mass and central portion of the rubber band to not roll, thus winding the rubber band up.
 
LURCH said:
If the innner mass rolls until the rubber band unwinds, the can will not return.
But in the experiment, the can really rolls back. So can you explain this?

DaveC426913 said:
The inner mass does not roll. It hangs from the rubber band, causing the mass and central portion of the rubber band to not roll, thus winding the rubber band up.
But when the can is rolling and winding up the rubber band, the rubber band will unwind at the same time, with a smaller rate. Therefore, it will give both the can and the rubber band a torque in opposite direction, just like the action and reaction forces mentioned in Newton's third law. Thus, i think that the mass will roll at the same time the can rolls. Besides that, in my experiment, when i roll the can, the can will stop at a distance from me and then rolls back. but it didn't stop at the point where i roll it. it will continue rolling until a point behind me (assume that i am facing the direction where i first roll the can to). After that, it will stop at the point there and won't come back anymore. If the inner mass does not roll, then we can think that it is a simple harmonic motion where the equilibrium point is the place i start rolling the can. so the can suppose to oscillate and stop at that point finally. But it didn't match with the result of the experiment. The can just go and back one time and stop at a distance from where it start to roll. can you explain this? thank you.
 
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Why don't we just prove this empirically? Use a transparent plastic tube instead of a can, and watch what happens inside.
 
Jeno said:
Besides that, in my experiment, when i roll the can, the can will stop at a distance from me and then rolls back. but it didn't stop at the point where i roll it. it will continue rolling until a point behind me (assume that i am facing the direction where i first roll the can to). After that, it will stop at the point there and won't come back anymore. If the inner mass does not roll, then we can think that it is a simple harmonic motion where the equilibrium point is the place i start rolling the can. so the can suppose to oscillate and stop at that point finally. But it didn't match with the result of the experiment. The can just go and back one time and stop at a distance from where it start to roll. can you explain this? thank you.
I'm not sure there's any big mystery to this. Isn't any SHM just being damped by the rolling friction and the friction of the rubber band against itself as it twists up?
 
Danger said:
Why don't we just prove this empirically? Use a transparent plastic tube instead of a can, and watch what happens inside.
Ya, i think this is a good way, but i can't find any suitable transparent tube to do this experiment.
zoobyshoe said:
I'm not sure there's any big mystery to this. Isn't any SHM just being damped by the rolling friction and the friction of the rubber band against itself as it twists up?
i think even though it is a damped oscillation, it will finally stop at the equilibrium point, except those overdamped oscillation. but the can can come back to the equilibrium point once, that means that it is not a overdamped oscillation. so why don't it stop at the equilibrium point?
 
  • #10
Jeno said:
Ya, i think this is a good way, but i can't find any suitable transparent tube to do this experiment.
You could do a quick and dirty version by sticking one end of the rubber band to the bottom of a glass jar with chewing gum or Plasticene and running the other end through a hole in the lid.
 
  • #11
Jeno said:
i think even though it is a damped oscillation, it will finally stop at the equilibrium point, except those overdamped oscillation. but the can can come back to the equilibrium point once, that means that it is not a overdamped oscillation. so why don't it stop at the equilibrium point?
I had to think about this a bit. Your set up is something like an imperfect set up for SHM. Suppose you clamped a metal rod in a vise then pulled the rod back and let it go. It would oscillate with SHM. But now suppose your vise was not attached to a bench, only sitting on it. The only things preventing the vise from moving is its inertia. If you now set the rod into motion the rod will oscillate but also exert force on the vise and move it. The SHM will come to a halt very quickly and since the vise has been moved it will not be at the original position of equilibrium.
 
  • #12
Jeno said:
But in the experiment, the can really rolls back. So can you explain this?


But when the can is rolling and winding up the rubber band, the rubber band will unwind at the same time, with a smaller rate. Therefore, it will give both the can and the rubber band a torque in opposite direction, just like the action and reaction forces mentioned in Newton's third law.
I think there is a misunderstanding of this experiment.

You let the can roll a few feet until it is about to change direction, then you can grab it, and pick it up (gently).
You get distracted by the TV for a few minutes, and then return to your experiment, which you have been holding in your hands.
You set the can back down on the ground. The can will, of its own accord, roll backwards several feet.

The rubber band acts as a storage device whose potential can be released immediately, or at an arbitrary time later.

Are we agreed?
 
  • #13
Thusly:
10 char
 
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