What Forces Are at Play to Prevent Slippage Between Two Accelerating Boxes?

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Homework Help Overview

The discussion revolves around a physics problem involving two boxes, where a smaller box rests on a larger box that is being accelerated horizontally. The focus is on understanding the forces at play that prevent the smaller box from slipping off the larger one, particularly the role of friction.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the applied force on the larger box and the frictional force that keeps the smaller box from slipping. Questions arise regarding the nature of friction and its dependence on normal force, as well as the conditions under which the boxes accelerate together.

Discussion Status

The discussion is active, with participants seeking clarification on the concepts of friction and normal force. Some guidance has been provided regarding the proportionality of frictional forces to normal forces, but there remains uncertainty about how horizontal forces influence these relationships.

Contextual Notes

Participants express confusion about the definitions and relationships between forces, particularly in the context of horizontal acceleration and its effect on normal force. There is an emphasis on understanding the conditions necessary for the smaller box to remain stationary relative to the larger box during acceleration.

zeion
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Top and bottom box force and motion question

Hello. This is my first time posting, I hope I have done everything correctly.



Homework Statement


A small box is resting on a larger box, which in turn sits on a table. When a horizontal force is applied to the larger box, both boxes accelerate together. The small box does not slip on the larger box.

1) What force causes the small box to accelerate horizontally?
2) If the acceleration of the pair of boxes has a magnitude of 2.5 m/s^2, determine the smallest coefficient of friction between the boxes that will prevent slippage.



The Attempt at a Solution



1)
Horizontal Fa on the lower box causes the top box to move, but Fa cannot > Fs between the two boxes or top will slip. But if Fs between two boxes is > than Fa then bottom cannot accelerate therefore top will not accelerate. Therefore Fa = Fs.
Fa causes the top box to move, but Fs between top and bottom causes top to not slip.

2)
\mu_s = \frac{F_s}{F_n}
It does not slip so F_A = F_s = ma
There is not vertical movement so F_n = mg
Therefore \mu_s = \frac{ma}{mg} = \frac{a}{g} = \frac{2.5m/s^2}{9.8m/s^2} = 0.25
\
 
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But if Fs between two boxes is > than Fa then bottom cannot accelerate therefore top will not accelerate.

Welcome to PF.

It's really enough to say that the force of friction is a maximum proportional to the normal force that reacts against horizontal forces. So long as the system is not accelerating the top box greater than the maximum frictional force available, then it won't move.
 
LowlyPion said:
Welcome to PF.

It's really enough to say that the force of friction is a maximum proportional to the normal force that reacts against horizontal forces. So long as the system is not accelerating the top box greater than the maximum frictional force available, then it won't move.

Hi. Thank you.
So the force of friction is never greater than the horizontal forces, it can only either be less or equal to them, is that right? I don't understand how horizontal forces affect Fn, I thought Fn was proportional to the perpendicular forces ie. gravity, which is proportional to the object's mass.
 
zeion said:
Hi. Thank you.
So the force of friction is never greater than the horizontal forces, it can only either be less or equal to them, is that right? I don't understand how horizontal forces affect Fn, I thought Fn was proportional to the perpendicular forces ie. gravity, which is proportional to the object's mass.

Fn is just that. Weight down and supporting force up.

Frictional forces are calculated on the basis that their magnitudes can be determined by a proportionality relationship with the normal forces.
 

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