Direction of friction in yo-yo where applied force is at top

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Homework Help Overview

The discussion revolves around determining the direction of friction for a yo-yo when a force is applied at the top tangent. Participants are exploring concepts related to Newton's laws of motion and rotational dynamics.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants are analyzing the net torque around different points of contact and questioning the assumptions made regarding the direction of friction. There is a discussion about the effects of choosing different axes for torque calculations.

Discussion Status

Some participants are seeking a more rigorous understanding of the frictional force direction, while others are clarifying the implications of the applied force on the motion of the yo-yo. There is an acknowledgment that the direction of friction may depend on the specific conditions of the problem, and multiple interpretations are being explored.

Contextual Notes

There is an emphasis on the need to solve the equations to determine the direction of friction accurately, with considerations for different geometries of the yo-yo affecting the outcome.

issacnewton
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Homework Statement


We have a yo-yo and the force ##F## which is the tension in the string and this is at the top tangent as shown in the figure attached with this problem. I want to figure out the direction of the friction at the point of contact.

Homework Equations


Newton's laws of motion and laws for rotational motion

The Attempt at a Solution


[/B]
Now I tried to see the net torque around the point of contact. Let's assume that the static friction force ##f##, is pointed in the same direction as ##F##, which is the right direction. So there are 3 forces acting at the point of contact. ##N, mg## and ##f##. So all of them will contribute zero torque around the point of contact. So only ##F## will contribute to the torque around the point of contact. And this is clockwise torque around this point of contact. Now consider the net torque around the point where ##F## is acting. Since the lines of action of ##N, mg## pass through this point, they will contribute zero torque around this point. ##F## will also not contribute to the net torque here since ##F## is acting at that point. So only ##f## will contribute to the net torque. And ##f## will cause a counter clockwise torque around this point. But this is not possible since we know from earlier analysis that the net torque has to be clockwise. So the direction of static friction force ##f## must be in the backward direction, so that the net torque will be clockwise.
But I know that in this problem, the friction force ##f##, has a forward direction (same direction as ##F##). So there must be something wrong in my reasoning.
So what is it ?

Thanks
 

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IssacNewton said:
Now consider the net torque around the point where F is acting.
Need to be careful in choice of axis. If you choose a non-inertial frame about a point which is not the mass centre you may get a wrong result.
IssacNewton said:
But this is not possible since we know from earlier analysis that the net torque has to be clockwise.
Torque is relative to a chosen axis, if you change axis you cannot assume the torque is the same way.
 
Ok, makes sense. I did not know that. I thought that if net torque is clock wise around one axis then it will be clock wise around any other axis. So, what is rigorous way to find the frictional force direction here ? I have seen the following explanation in this particular case. Due to the force ##F## at the top, the bottom will start sliding towards left and so there will be a momentary kinetic friction force in the forward direction. To prevent sliding, this forward kinetic friction force will become forward static friction force. This explanation is kind of convincing but I wonder if more rigorous argument could be made here.
 
IssacNewton said:
Due to the force F at the top, the bottom will start sliding towards left
That is not sufficiently obvious. Imagine this as an object floating in space. F will cause a translation to the right of the mass centre, and a clockwise rotation about the mass centre, but the direction of movement of the point diametrically opposite from F will depend on the ratio of the two.
 
So, how can we deduce that the static friction force is in the same direction as ##F## ? I don't think I clearly understood your point here.
 
IssacNewton said:
So, how can we deduce that the static friction force is in the same direction as ##F## ? I don't think I clearly understood your point here.
Just write out the equations and solve.

It will turn out that the direction will be in the F direction for a uniform solid cylinder. For a hollow cylindrical shell of zero thickness, I believe there would be no frictional force, and if you were to add a flange to that, projecting beyond the two forces, so that the moment of inertia exceeds mr2, then the frictional force will go the other way.
 
Ok, so we can not get the direction of friction before solving the equations ?
 
IssacNewton said:
Ok, so we can not get the direction of friction before solving the equations ?
That's my view.
 
Ok, thanks haruspex...
 

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