Does the Normal contact force act through the centre of mass?

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Discussion Overview

The discussion revolves around the behavior of normal contact forces in relation to the center of mass (CoM) of stacked rectangular blocks when one block is pushed to the right. Participants explore whether the normal contact force acts through the CoM and the implications of torque in this scenario, with a focus on theoretical and conceptual aspects.

Discussion Character

  • Conceptual clarification
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants assert that the normal contact force does not always act through the center of mass, emphasizing that it is a general concept unrelated to the CoM.
  • Others propose that in specific cases, such as when the normal forces do not create net torque, the effective sum of these forces must pass through the center of mass.
  • One participant questions why the maximum displacement occurs when the weight acts through the pivot point, suggesting that beyond this point, the normal force cannot balance the torque due to weight, leading to potential rotation and loss of contact.
  • Another participant clarifies that the normal force is always perpendicular to the contact surface, which influences its relationship with the center of mass.
  • There is a discussion about how uniform gravity does not create torque around the CoM, and thus the supporting forces must also have zero torque around the CoM to prevent rotation.
  • Some participants note that similar dynamics occur even when the contact surfaces are not horizontal, with the top block rotating around the pivot point as it is pushed to the right.

Areas of Agreement / Disagreement

Participants express disagreement regarding the relationship between normal contact force and the center of mass, with no consensus reached on whether the normal force always acts through the CoM or only in specific cases. The discussion remains unresolved with multiple competing views presented.

Contextual Notes

Participants highlight the importance of torque and the conditions under which normal forces act, but do not resolve the mathematical implications or assumptions regarding the scenarios discussed.

phantomvommand
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TL;DR
Does the Normal contact force always act through the centre of mass?
Consider the following situation:

You have 1 rectangular block lying on a table, and an identical block is placed above the block on the table. Now, this new block is constantly pushed to the right, right before it topples off.

Consider the torque about an axis passing through the rightmost and topmost point (this point is labelled A) of the bottom block. I read somewhere that the maximum this new block can be pushed is to the point where it Weight acts through A. Does this mean Normal contact force also only acts through A at this point?

Thank you!
 
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phantomvommand said:
Does the Normal contact force always act through the centre of mass?
No. Normal contact force is a general concept that has nothing to do with the centre of mass per se.

phantomvommand said:
Consider the following situation:

You have 1 rectangular block lying on a table, and an identical block is placed above the block on the table. Now, this new block is constantly pushed to the right, right before it topples off.

Consider the torque about an axis passing through the rightmost and topmost point (this point is labelled A) of the bottom block. I read somewhere that the maximum this new block can be pushed is to the point where it Weight acts through A. Does this mean Normal contact force also only acts through A at this point?
Yes, in this special case, where the normal forces must not create any net torque, their effective sum has to pass through the center of mass.
 
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A.T. said:
No. Normal contact force is a general concept that has nothing to do with the centre of mass per se.Yes, in this special case, where the normal forces must not create any net torque, their effective sum has to pass through the center of mass.

I was really confused just now. Yes, it does not always go through the COM. Normal force is perpendicular to the contact surface, right?

In the situation I mentioned earlier, why is it that the maximum rightwards displacement is when Weight acts through the pivot point?

I suppose it is because when the Centre of Mass moves beyond the edge, normal contact force (acting perpendicular to the contact surface) can never balance the torque due to weight, resulting in rotation, loss of contact, and normal contact force = 0 eventually?
 
phantomvommand said:
Normal force is perpendicular to the contact surface, right?
Yes, that's all it means.

phantomvommand said:
I suppose it is because when the Centre of Mass moves beyond the edge, normal contact force (acting perpendicular to the contact surface) can never balance the torque due to weight, resulting in rotation, loss of contact, and normal contact force = 0 eventually?
I would put it like this: Uniform gravity doesn't create any torque around the CoM, so the torque around the CoM by the supporting froces must also be zero to prevent rotation. With all the contact surface on one side of the CoM, there is no possible distribution of a non-zero support froce, that would create zero torque around the CoM.
 
phantomvommand said:
I was really confused just now. Yes, it does not always go through the COM. Normal force is perpendicular to the contact surface, right?

In the situation I mentioned earlier, why is it that the maximum rightwards displacement is when Weight acts through the pivot point?

I suppose it is because when the Centre of Mass moves beyond the edge, normal contact force (acting perpendicular to the contact surface) can never balance the torque due to weight, resulting in rotation, loss of contact, and normal contact force = 0 eventually?
Same thing will happen in the case the surfaces of contact between both blocks are not horizontal.
Normal forces will have one direction and gravity force will have another, yet the top block will start rotating around point A clockwisely as soon as it has been pushed towards the right enough as to have more mass to the right than to the left of an imaginary vertical line that intersects point A.
 

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