Understanding Force Pairs in Accelerated Systems: Explained for Beginners

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Discussion Overview

The discussion revolves around the concept of force pairs in accelerated systems, particularly focusing on the dynamics of a hand holding a mass that is too heavy to support. Participants explore the differences in force interactions during static equilibrium versus acceleration, aiming to clarify the nature of these forces in a non-equilibrium context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant expresses confusion about how force pairs remain equal during acceleration, using the example of a hand holding a mass that is accelerating downwards.
  • Another participant suggests that the force of the mass on the hand is less than its weight (mg) because the hand is accelerating downwards, which affects the force interaction.
  • A participant seeks clarification on the relationship between the forces acting on the mass and the hand, noting that if the hand were in equilibrium, the force would equal mg, but this changes during acceleration.
  • There is a discussion about the forces acting on both the mass and the hand, with emphasis on how these forces differ when in motion compared to being stationary.
  • One participant points out that if both the hand and mass were in free fall, the forces between them would be zero, indicating a different state of interaction.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of the forces during acceleration, with ongoing questions about how these forces compare to those in static equilibrium. The discussion remains unresolved regarding the exact dynamics of force interactions in this scenario.

Contextual Notes

Participants express uncertainty about the conditions under which the forces change, particularly the assumptions related to acceleration and contact forces. The discussion highlights the complexity of force interactions in non-equilibrium situations.

kbm
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This is going to be a very elementary question, but I am having a hard time wrapping my head around it for whatever reason.

In static equilibrium, like a book on a table, I have no problem seeing that the force exerted on the table by the book is equal and opposite to the force exerted on the book by the table.

But when things are being accelerated I am having a hard time grasping how the force pairs are equal.

For example, if a hand is holding up a mass that is too heavy for the person to hold, then the mass and the hand will both be accelerated downwards. The forces acting on the mass would be the force of gravity, acting down, and the pushing force of the hand, acting up. The force of gravity is greater than the pushing force so there is a net force downwards.

How is it that the hand exerts an equal and opposite force on the mass?

The forces on the hand would be the weight of the mass, acting downwards, the force of gravity on the hand, acting downwards, and the pushing force of the arm on the hand, acting upwards.

The force of the mass on the hand is equal to the weight of the mass (mg), and the force of the hand on the mass is equal to the pushing force of the arm. But if these were equal, then the pushing force of the arm would equal the weight, or force of gravity, on the mass, an then there would be no net force downwards on the mass.

What am I getting confused?
 
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Welcome to PF!

Hi kbm! Welcome to PF! :smile:
kbm said:
The force of the mass on the hand is equal to the weight of the mass (mg) …

No, the force of the mass on the hand is less than mg (if you like, because the hand is accelerating away, so it isn't getting the full oomph from the mass), and the force of the hand on the mass is the same (less than mg), causing the mass to accelerate downwards.
 
Thanks for the reply.

Alright so just for clarification: If the hand was holding the mass up at equilibrium, then the force of the mass on the hand would be equal to mg, correct?

But because the hand is moving downwards, the force of the mass on the hand is <mg. So in an FBD the forces acting on the mass would be (mg) acting downwards and (<mg) acting upwards, so a net force down. Similarly, the forces on the hand would be (<mg) acting downwards, the weight of the hand acting down, and a push force acting upwards, which must be still LESS than (<mg).

Why though, if the hand and the mass are still in direct contact and accelerating down at the same rate, is the force of the mass on the hand LESS than it would be if they were both stationary?
 
kbm said:
Alright so just for clarification: If the hand was holding the mass up at equilibrium, then the force of the mass on the hand would be equal to mg, correct?

But because the hand is moving downwards, the force of the mass on the hand is <mg. So in an FBD the forces acting on the mass would be (mg) acting downwards and (<mg) acting upwards, so a net force down. Similarly, the forces on the hand would be (<mg) acting downwards, the weight of the hand acting down, and a push force acting upwards, which must be still LESS than (<mg).

Yes. :smile:
Why though, if the hand and the mass are still in direct contact and accelerating down at the same rate, is the force of the mass on the hand LESS than it would be if they were both stationary?

If they were free-falling, they would still be in direct contact and accelerating down at the same rate, but the forces between them would be zero, wouldn't they?

This is an intermediate stage.
 
Alright that makes sense. Thanks for the help.
 

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