Rotational work and forces like static friction and tension

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Discussion Overview

The discussion revolves around the concept of rotational work, particularly in the context of forces like static friction and tension. Participants explore the implications of the definition of rotational work and its application to scenarios involving rolling motion and rigid bodies.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the definition of rotational work, suggesting that any torque with an axial component should perform rotational work, using the example of a disk rolling down an incline where static friction generates torque.
  • Another participant clarifies that if the axis of rotation is at the point where friction acts, there is no torque and thus no work done by friction.
  • A later reply acknowledges the Wikipedia definition of rotational work as applicable to rotation about a fixed axis through the center of mass, while questioning why friction does not do rotational work despite exerting axial torque.
  • Some participants argue that while friction is necessary for rotation, it is not the source of work being done; rather, gravity is responsible for the work in the rolling disk scenario.
  • One participant introduces a different example involving a beam supported at two ends, questioning whether the remaining support does work as the beam falls and rotates.
  • Another participant notes that torque arises when a force's action point moves perpendicularly to the force, indicating that gravity does exert torque in the beam example.

Areas of Agreement / Disagreement

Participants express differing views on the role of friction and gravity in performing work during rotational motion. There is no consensus on whether friction does rotational work, as some argue it does not while others suggest it is involved in the process.

Contextual Notes

The discussion highlights the complexity of defining work in rotational systems, particularly regarding the choice of pivot points and the nature of forces involved. Participants reference specific conditions and definitions that may limit the applicability of their arguments.

Soren4
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I have a doubt regarding the definition of rotational work, which is as follows

W = \int \tau_z d \theta

Where \tau_z is the component of the torque parallel to the axis of rotation z.

My doubt concerns the fact that, looking at this definition, it seems that any torque which has an axial component and causes a rotation, do rotational work.

However, consider a problem of pure rotational motion (i.e. rolling with no slipping), for example a disk rolling down an inclined plane and take as pivot point for calculate torque the center of mass of the disk. The static friction force generates a torque which is totally axial and is the cause of the rotation of the disk (if there was no friction the disk would just slip). But the static friction is a classic example of a force that does not do work because it does not cause any displacement.

A similar situation is the one with rigid bodies similar to yo-yos, i.e. falling pulleys that carry a wire (on which they roll without slipping). Again, the tension of the rope exerts an axial torque and causes the rotation of the yo-yo, but it seems very strange to me that tension can do work.

Do these forces perform rotational work? I probably misunderstood the definition but I do not see what is wrong. Thanks in advance for your suggestions.
 
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You left out the fixed axis ...
Rolling example: if the axis is the point where the friction acts (the 'fixed axis'), there is no torque and no work.
yoyo example: if the axis is the point where the tension acts (the axis of rotation) there is torque from gravity, which is doing work.
(note that friction isn't required to keep a cylinder rolling, only to get it to roll)
 
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BvU said:
You left out the fixed axis ...
Rolling example: if the axis is the point where the friction acts (the 'fixed axis'), there is no torque and no work.
yoyo example: if the axis is the point where the tension acts (the axis of rotation) there is torque from gravity, which is doing work.
(note that friction isn't required to keep a cylinder rolling, only to get it to roll)

Thanks for the answer! Sorry if I expressed the condition of pure rotational motion incorrectly.

In the Wikipedia page it is claimed that the definition of rotational work is for a "rotation about a fixed axis through the center of mass". Now, considering the example of the disk on the incline, I'm totally ok with the fact that, if I consider the contact point of the disk with the incline to be the instantaneous axis of rotation, then static friction exerts zero torque while gravity does work, but, is there any reason why I cannot interpret the motion of the disk as a rotation about the center of mass, plus a traslational motion of the center of mass? If I do so, gravity still do ("traslational") work, but I don't see the reason why friction does no (rotational) work, according to the definition (it does exert a axial torque if the pivot point is in the center of mass). Am I missing something?
 
I don't think you are missing something. If you let something rotate, you also make use of friction. But it's you doing the work, not the friction.
 
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Thanks, forgive me but I do not get how I am doing work instead of friction, I mean I just let the disk roll down the incline, I do not exert any force on it
 
Soren4 said:
Thanks, forgive me but I do not get how I am doing work instead of friction, I mean I just let the disk roll down the incline, I do not exert any force on it
That was gravity doing the work.

I was referring to letting e.g. a ball spin: you need friction to do that,
 
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BvU said:
I don't think you are missing something. If you let something rotate, you also make use of friction. But it's you doing the work, not the friction.
BvU said:
That was gravity doing the work.
I was referring to letting e.g. a ball spin: you need friction to do that,

I hope I understood what you said (the fact that friction is not responsible by itself for the rotation, because it exists just if a force is exerted) but I still do not see why friction does no rotational work, just looking at the definition above, since fricition does exert an axial torque and that formula tells me that it means that friction does rotational work. Suppose to consider the motion of the disk as a combination of a traslational motion of CM and a rotation about the CM. Then if a force is exerted in the center of mass of the disk (like gravity), that force cannot exert torque, and I do not get how it can do the rotational work instead of friction
 
Other example: beam supported at two ends. One of the two supports disappears and the beam starts to fall and rotate. Does the other support do work ?

I admit I find it difficult to oppose your last paragraph. But you are not looking in an inertial frame and gravity does exert torque. Torque appears when moving an action point of a force in a direction perpendicular to the force. In this case gravitational force is moved sideways to directly above the support point. Torque and angular acceleration result.
 

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