Friction in rotational movement

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Discussion Overview

The discussion revolves around the role of friction in rotational movement, specifically in the context of a wheel rolling up and down an inclined plane. Participants explore the relationship between friction direction, angular acceleration, and the distinction between passive and active scenarios in rotational dynamics.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant describes a scenario where a wheel rolls down an incline, suggesting that the friction force aligns with the angular acceleration.
  • Another participant argues that if the wheel is actively being turned (e.g., by a motor), the angular acceleration may oppose the direction of friction, depending on the context.
  • A later reply emphasizes that static friction acts to prevent slipping and must create the necessary torque for angular acceleration, but this can vary based on external forces.
  • Some participants highlight the distinction between "passive" cases (where the wheel rolls down without external torque) and "active" cases (where torque is applied to move the wheel up the incline).
  • There is a suggestion that the understanding of friction's role may differ among participants, particularly regarding the definitions of passive and active scenarios.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between friction and angular acceleration, with some agreeing on the passive case while others contend that the active case introduces complexities that challenge this agreement. The discussion remains unresolved regarding the precise nature of friction's role in these scenarios.

Contextual Notes

Participants acknowledge that the definitions of passive and active cases may influence their understanding of friction's behavior, and there is an implication that additional external forces can complicate the dynamics involved.

Paloseco
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First, sorry for my bad english, it is a hard job for me.

I am an engineering student and I have found that something doesn´t match.

Imagine a cylinder, a wheel for example. Case 1) If it if it descends by a plane inclined because of its weight, the friction direction goes in the same way that the angular acceleration, Case 2) But imagine that you give a torque to this wheel to make it raise by the slope. In this case the angular acceleration goes in opposite that in case 1 (and the turn) but the friction force will go in the same direction that before. Is this right? Because some professors claim that the friction force goes always in the same direction that the angular acceleration, but I think that it deppends it the object is pasive (when you let it go downhill) or active (it makes the torque, like in a car wheel). I hope someone confirm me this, is very important for my investigation

Regards

Edited: you can try an applet in this page, it works pretty well:
http://www.edu.aytolacoruna.es/aula/fisica/teoria/A_Franco/solido/roz_rodadura/rozamiento.htm
 
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I THINK you are referring to the wheel turning faster as it goes down the ramp and slower as it goes up. (Otherwise, there is not necessarily any rotational acceleration.)

If there were no friction at all, the wheel could slide up or down the ramp with turning at all. The only force causing the wheel to turn faster (or slower) is the friction force (NOT gravity- that causes linear acceleration): F= ma so, yes, the friction force is in the same direction as the acceleration.

Notice that as the wheel is rolling down the ramp, the angular acceleration is directed back up the ramp, the same direction as the friction.

When the wheen is rolling up the ramp, the angular acceleration is directed down the ramp, again the same direction as the friction.

You say "but I think that it depends it the object is passive (when you let it go downhill) or active (it makes the torque, like in a car wheel)." so you may be thinking of the wheel applying force to go up, rather than a wheel simply rolling up the slope (and slowing as it goes). I think your "professors" are talking about the "passive" case that I am since in your "active" case, there might be know angular acceleration at all.
 
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Yes, my teachers are in the passive case, but they don´t understand it when i try to explain them the active case. :rolleyes:

When the wheel is rolling up the ramp, the angular acceleration is directed down the ramp, again the same direction as the friction
Yes, if it is passive, but if the object is active (like the wheel of a mountain bike) then, thinking of the wheel applying force to go up, in this case the angular acceleration will go in oppositte way to the friction force. The same case if you aply a torque to the wheel to force it to go up.

My question is, am I right or not? I am sure that I am, but I need it to be confirmed by someone else besides me
 
I'm not sure I understand the question, but I will offer these comments for situations involving rolling without slipping:

(1) If friction is the only torque-producing force on the wheel, then of course the friction must act so as to create the angular acceleration. If other torque-producing forces act, then (obviously) the net torque is what determines the acceleration.

(2) Static friction is a "passive" force, in that it will be the minimum it needs to be to prevent slipping, up to its limit ([itex]= \mu N[/itex]).

If you imagine a mountain bike accelerating on a flat surface (for simplicity), then the friction points in the same direction as the linear acceleration. (Friction is the only external horizontal force on the bike.) The friction exerts a torque on the wheel, but so does the biker. The net torque causes the angular acceleration.
 
Doc Al said:
If you imagine a mountain bike accelerating on a flat surface (for simplicity), then the friction points in the same direction as the linear acceleration.

That is what I tried to say, then I were not wrong. Thanks
 

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