Rolling Motion Test: Take the Challenge and Justify Your Answers

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SUMMARY

The forum discussion centers around a rolling motion test designed to clarify misconceptions about forces, torques, and rolling motion. Participants analyze two cases: one with a frictionless surface and another with friction present. Key conclusions include that in Case 1, the center of the disk experiences zero acceleration while rotating clockwise, and in Case 2, the disk accelerates to the right and also rotates clockwise. The discussion emphasizes the importance of justifying answers to enhance understanding of the underlying physics principles.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with concepts of torque and rotational motion
  • Knowledge of static friction and its role in motion
  • Basic principles of forces acting on rigid bodies
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  • Explore the concept of torque in rotational dynamics
  • Study the effects of friction on rolling motion
  • Learn about the conservation of angular momentum in rigid bodies
  • Investigate practical applications of rolling motion in real-world scenarios
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Physics educators, students studying mechanics, and anyone interested in deepening their understanding of rotational dynamics and forces in motion.

  • #31
This is not a zero sum game. For a given impulse, the body does not acquire rotational kinetic energy at the expense of translational kinetic energy. The amount of rotational KE depends on the distance of the CM from the point of impact . The ensuing angular velocity about the CM is subject to angular momentum conservation just like the ensuing linear velocity is subject to linear momentum conservation. The two are independent of each other.
 
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  • #32
I personally don't think its irrational to be taken by surprise by this as a lay person (like me). It seems like you are getting something for nothing because "position" is often just arbitrary. I think, how can an arbitrary choice have such obvious consequences, and then you find out it does and it's a bit shocking. I guess the key here is that the position @kuruman is talking about isn't really arbitrary, its relative to a very special position in physics on an extended body, and that is what makes the difference.

This is even further off topic, but I remember thinking how a lever actually multiplies the force? Right away conservation of energy pops into your head, and you start reconciling forces and displacements. Then I thought: "But if the system is static there is no displacement, yet I still have a multiplied force?" It seems strange, and I'm not sure I still understand that, but you realize there are important consequences of position and it's not always obvious why...

I don't know where you are at in your education, but you probably have time to figure some of this stuff out. I wouldn't worry too much.
 
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  • #33
Does the final problem have to do with Newtons third law, where the net force from your foot is canceled by the force your butt exerts on the seat?

I showed the wife and kids this strangeness. They had fun! Thanks!
 
  • #34
kuruman said:
This is not a zero sum game. For a given impulse, the body does not acquire rotational kinetic energy at the expense of translational kinetic energy. The amount of rotational KE depends on the distance of the CM from the point of impact . The ensuing angular velocity about the CM is subject to angular momentum conservation just like the ensuing linear velocity is subject to linear momentum conservation. The two are independent of each other.

Let's take an example of a rod that weights 1kg, and has a length of 2 meters, ##M = 1##, ##L=2##, ##I_{cm}=\frac 1 {12} M L^2 = \frac 1 3## if a force of 10N is applied a distance ##R = 1## from the center of mass for 100ms, the change in angular momentum is ##\tau \Delta t = RF\Delta t = (1)(10)(.1) = 1##, the angular velocity is ##\dot \theta = \frac {L_{cm}} {I_{cm}} = (1)(3) = 3## radians per second. The change in linear momentum is ##F\Delta t = (10)(.1)=1##, so the velocity is ##\frac P M = 1## meters per second. If you apply the same force to the cm you will have no rotation, but you will have the same linear velocity. So in the first case:
$$KE = \frac 1 2 Mv^2 + \frac 1 2 I_{cm}{\dot \theta}^2 = \frac 1 2 + \frac 1 2 \frac 1 3 3^2 = 2$$In the second case$$KE = \frac 1 2 Mv^2 = \frac 1 2$$In this example we're not expending translating KE for rotational KE, but I'm wondering what the reasoning is for the result, we apply the same force at a different location and apparently we do more work with the same impulse? What's going on?
 
  • #35
Chenkel said:
does anyone know why there seems to be more energy in the body with the same impulse in the off center force example?
The answer has been given a number of times already [in another recent thread]

Energy goes as force times displacement. Momentum goes as force times time. The two need not be proportional. With an off-center hit there is less resistance at the point of impact, so more velocity at the point of impact, so more displacement at the point of impact, so more energy transferred for a given impulse.
 
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  • #36
jbriggs444 said:
The answer has been given a number of times already [in another recent thread]

Energy goes as force times displacement. Momentum goes as force times time. The two need not be proportional. With an off-center hit there is less resistance at the point of impact, so more velocity at the point of impact, so more displacement at the point of impact, so more energy transferred for a given impulse.
So I can take my constant impulse and potentially create a more kinetic energy from said impulse depending on how I apply it? I'm guessing the same impulse will create more energy if the distance traveled is larger, so that would take more effort on my part, the person applying the force. The puzzle is starting to come together. Thank you.
 
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  • #37
Chenkel said:
So I can take my constant impulse and potentially create a more kinetic energy from said impulse depending on how I apply it? I'm guessing the same impulse will create more energy if the distance traveled is larger, so that would take more effort on my part, the person applying the force. The puzzle is starting to come together. Thank you.

Same force, but applied to CM vs (almost at the) tip of the rod. The time of impact is also the same, hence same impulse. When force is applied to the tip of the rod, the displacement is longer, thus more work is done.
1657691679841.png
 
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  • #38
Chenkel said:
So I can take my constant impulse and potentially create a more kinetic energy from said impulse depending on how I apply it? I'm guessing the same impulse will create more energy if the distance traveled is larger, so that would take more effort on my part, the person applying the force. The puzzle is starting to come together. Thank you.
Simply put: Impulse is not energy. It is therefore not a given that a particular impulse should correspond to a particular energy.

The details have been discussed above.
 
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