Understanding Forces: Explaining maa and mbb in a Simple Example"

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Discussion Overview

The discussion revolves around understanding the forces acting on two blocks, A and B, in a physics problem involving applied forces, friction, and Newton's laws. Participants explore the definitions and roles of the forces maa and mbb, as well as the implications of these forces in the context of the problem.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question why mba is considered the reaction force and what exactly maa and mbb represent in the context of the problem.
  • One participant suggests that the force of A on B, denoted as FA→B, equals mba, which is normal to the surfaces between A and B, and relates this to the maximum static friction force.
  • Another participant emphasizes the need to apply the second law and draw a free body diagram to clarify the relationships between the forces acting on A and B.
  • There is a discussion about the distinction between the forces acting on A and B, with some participants asserting that F acts only on A, while others argue that A's interaction with B is also crucial.
  • Some participants propose that the forces acting on the system can be viewed in different ways, such as treating A and B as separate entities or as a single mass.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and roles of maa and mbb, with no consensus reached on their exact meanings or implications. The discussion remains unresolved regarding the interpretation of these forces.

Contextual Notes

Participants mention the need for a free body diagram and the application of Newton's second law, indicating that assumptions about the system's configuration and interactions may affect the analysis.

pluspolaritons
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Hi,

Please take a look at this figure:
Screenshot by Lightshot

There is a force that is applied so that block B will not fall under the influence of gravity.

I have set up the problem as:
F= (ma+mb)a

μR=mbg

where μ is the coefficient of friction and R is the reaction force.

Now my question is I can't figure out why mba is the reaction force.

What exactly is maa and mbb? Shouldn't maa be the force of block a on b? Then what about mbb? What is this force? The force direction should be pointing to the right side (since the applied force is to the right)? So it is as if mbb is acting on thin air?

I can't wrap my head around what is maa and mbb, please help.

Thanks.
 
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pluspolaritons said:
Hi,

Please take a look at this figure:
Screenshot by Lightshot

There is a force that is applied so that block B will not fall under the influence of gravity.

I have set up the problem as:
F= (ma+mb)a

μR=mbg

where μ is the coefficient of friction and R is the reaction force.

Now my question is I can't figure out why mba is the reaction force.
The 3rd law pair to the force of A on B is the equal and opposite force of B on A. But you do not really need to use the third law. This is a second law problem.

The force of A on B, FA→B = mba, which is normal to the surfaces between A and B. The maximum static friction force between B and A is the force normal to the surface between B and A multiplied by the co-efficient of static friction (μs).

Ffmax = μsFA→B = μsmba

In order for B not to fall, how must this maximum static friction force be in relation to mbg ?

AM
 
Thanks Andrew. I know the solution to this problem, but I need to know what is maa and mba. Why is the force of A on B equals to mba instead of maa? Then what is maa?
 
pluspolaritons said:
Thanks Andrew. I know the solution to this problem, but I need to know what is maa and mba. Why is the force of A on B equals to mba instead of maa? Then what is maa?

Draw a freebody diagram and apply the second law.

F = ma+ba = maa + mba

so: maa = F - mba

Examining the forces on A: there is F pushing A forward and the force from B on A (= -mba) which is in the opposite direction to F. Together they must sum to the net force on A which is necessarily maa (second law).

For B, there is only the force of A on B. This must be equal to mba (second law).

AM
 
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Andrew Mason said:
Draw a freebody diagram and apply the second law.

F = ma+ba = maa + mba

so: maa = F - mba

Examining the forces on A: there is F pushing A forward and the force from B on A (= -mba) which is in the opposite direction to F. Together they must sum to the net force on A which is necessarily maa (second law).

For B, there is only the force of A on B. This must be equal to mba (second law).

AM

Thanks, I think it's clearer now.

So, F only acts on A but not B right? This is because F is in direct contact with A but not B, correct? But since B is in direct contact with A, it will feel the force of A on B.
 
pluspolaritons said:
Thanks, I think it's clearer now.

So, F only acts on A but not B right? This is because F is in direct contact with A but not B, correct? But since B is in direct contact with A, it will feel the force of A on B.

You can divide the bodies any way you like. The forces that apply to all parts of A and B all originate with F: eg. without F, A could apply no force to B.

If you want to make a distinction between A and B, then you can say that F acts on A and A acts on B.

You could divide A into two parts and say that the left half of A applies a force to the right half of A so that the force applied by the left half of A causes the right half to accelerate.

Or you could make no distinction between bodies or parts of bodies treating A+B as a single mass and simply say that F applies a force to a mass A+B.

AM
 

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