How to Determine if Friction Will Act?

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Discussion Overview

The discussion revolves around the mechanics of friction in a system of stacked boxes, specifically examining the conditions under which friction acts between the boxes when a force is applied to the middle box. Participants explore the implications of static friction, the role of normal forces, and the conditions for acceleration in the system.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that if the system is not accelerating, the friction force from the top box must be zero to prevent the top box from accelerating as a result of Newton's third law.
  • Others argue that without information about acceleration, one might assume there could be a friction force from the top box, regardless of the applied force.
  • A participant questions why all friction seems to come from the bottom box and not the top box, suggesting a possible connection to the normal force.
  • Another participant notes that when pushing the middle box, static friction between the middle and bottom boxes must be stronger than that between the middle and top boxes, due to differences in normal force.
  • Some participants discuss the idea that the top box does not need to exert friction if the middle box is not sliding relative to it, as the bottom box is holding the middle box in place.
  • There is a suggestion that gravity's direction may play a fundamental role in determining which box provides static friction in this scenario.

Areas of Agreement / Disagreement

Participants express differing views on the role of friction from the top box and the conditions under which it acts. There is no consensus on the necessity or behavior of friction in this context, indicating ongoing debate and exploration of the topic.

Contextual Notes

Participants acknowledge the dependence on assumptions about acceleration and the definitions of forces involved, but these remain unresolved within the discussion.

Acala
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Let's consider a system of three boxes stacked vertically, resting on the ground. There is friction acting between all surfaces involved.

I push on the middle box, but without enough force to move the system at all. If we are to analyze the middle box, we'll see a static friction force coming from the boxes both above and below it. The friction from the top box must equal zero, though, because if it were nonzero, the Newton's third law paired friction force from the middle box would cause the top box to accelerate.

My question is this: if we were not given the information that nothing in the system is accelerating, and rather simply given the information about the applied force and friction forces, how would we know that no friction were coming from the top box? Also, why is there no friction from this box in the first place?
 
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Hi Acala! :smile:
Acala said:
The friction from the top box must equal zero, though, because if it were nonzero, the Newton's third law paired friction force from the middle box would cause the top box to accelerate.

That's completely correct. :smile:
if we were not given the information that nothing in the system is accelerating, and rather simply given the information about the applied force and friction forces, how would we know that no friction were coming from the top box? Also, why is there no friction from this box in the first place?

I don't understand why you're asking. You obviously understand the F = ma principle applied to the top box. Everything in mechanics ultimately boils down to F = ma.

Why should there be friction if nobody's pushing the top box? :confused:
 
I mean that if we were given no information about the acceleration of the system, then we would have to assume that there would be a friction force from the top box, whatever value it may be. I say this because I calculated the friction force from the top box under the assumption that it was not accelerating.

I am wondering why all of the friction is coming from the bottom box in the first place; why is the top box not contributing friction and then just sliding off? Does it have something to do with the normal force?
 
Acala said:
… why is the top box not contributing friction and then just sliding off? Does it have something to do with the normal force?

there was friction from the top box when you started pushing …

but as you approached cruising speed, the acceleration reduced, and so did the friction,

and when you reached cruising speed, the acceleration was zero, and so was the friction :wink:
 
tiny-tim said:
Hi Acala! :smile:That's completely correct. :smile:I don't understand why you're asking. You obviously understand the F = ma principle applied to the top box. Everything in mechanics ultimately boils down to F = ma.

Why should there be friction if nobody's pushing the top box? :confused:

I think what the OP is asking is, if you push on the middle box, then you're trying to make two pairs of surfaces slide relative to each other. One pair happens to be the top of the middle box, and the bottom of the top box. So why isn't there static friction between the top and middle boxes in the case when you push, but not hard enough to make anything move?

I tried this with a stack of three books. I pushed on the middle one. If I didn't push hard enough, nothing happened.

If I pushed hard enough, static friction between the middle book and the bottom book was overcome, and the middle book started moving. The top book moved along with the middle book in this situation. So, clearly, in the situation where the middle book moves, there IS static friction between the middle book and the top book, because the middle one carries the top one along with it. Yet, in the case where nothing moved, there was clearly no static friction between the middle and top book, because this would lead to an unbalanced force on the top book. How do contact surfaces between the middle and top book "know" that no friction is necessary in the latter case?
 
Thinking about it some more, I think the answer is this:

In the case where you push on the middle box, but too weakly for anything to happen, it will always be true that static friction between the middle and bottom boxes is stronger than static friction between the top and middle boxes. The reason is that for the former case, the normal force is equal to the combined weight of the middle and top boxes. For the latter case, the normal force is only equal to the weight of the top box.

The middle box can't slide if the bottom one is holding it in place. And if the bottom one is holding it in place, the top one has no need to, since, from its "point of view" the middle box is not trying to slide relative to it.
 
Yes, cepheid's interpretation of my question was correct.

cepheid said:
The middle box can't slide if the bottom one is holding it in place. And if the bottom one is holding it in place, the top one has no need to, since, from its "point of view" the middle box is not trying to slide relative to it.

This does make sense, and it's quite insightful, but why, in that case, was the bottom box the first box that was called upon to provide the static friction? It seems that even if its maximum potential static friction force were lower, it could simply be overcome and the top box would be called upon to provide the friction.

Is there something more fundamental causing this? Perhaps, since gravity seems to be the force running this situation, it's because gravity points downward? And if that sounds reasonable, could it be (or has it been) generalized?
 

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