Newtons 2nd law for non-rigid bodies

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SUMMARY

The discussion centers on the application of Newton's second law to a system of non-rigid bodies, specifically involving a disk and a bar connected by a spring. The key conclusion is that the center of mass (CM) of the system will not move to the right due to the absence of external forces acting in that direction. The participants agree that Newton's second law, expressed as F=Ma, applies to both rigid and non-rigid bodies, confirming that the disk will not remain in contact with the wall as it falls.

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  • Understanding of Newton's second law (F=Ma)
  • Knowledge of center of mass (CM) concepts
  • Familiarity with the dynamics of connected bodies
  • Basic principles of rotational motion
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aggie1293
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I have a question pertaining to the motion of the center of mass (CM) of several connected bodies.

Homework Statement



Here is a picture of the set-up (green surfaces are stationary):

U6uxxt8.png
The mass of the spring is zero.
The mass of the disk is M1.
The mass of the bar is M2.

There is a pin reaction at the union of the bar and the disk, so the disk is free to rotate.

QUESTION: Will the disk touch the stationary wall at t>0?

Homework Equations


F=Ma

The Attempt at a Solution

I believe no, the reason being thus:

First of all, assume that the disk will remain in contact with the wall as it falls. This would force the center of mass of the bar to move to the right, as in the picture below.

E7dYYDL.png


Since the CM of the disk does not horizontally and the CM of the bar moves to the right, the CM of the entire system also moves to the right. This is impossible because there is no force pushing any part of the system to the right.

GRsiZnZ.png
.

The orange arrows are the external forces acting on the body. Since there are no arrows pointing to the right (and the normal force can't be negative), there is no way for the CM of the system to move to the right.

Therefore, the assumption that the disk will remain on the wall is wrong. The disk will swing out as the reaction force of the bar resisting a change in it's inertia pushes it to the left. The reason I am asking this is because my professor and TA are adamant that the disk will roll down the surface of the wall. They say that Newton's second law is only applicable to rigid bodies.

Am I missing something here?
 
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More concisely stated, the question is this:

Does Newton's second law apply to a system of rigid bodies?
 
aggie1293 said:
More concisely stated, the question is this:

Does Newton's second law apply to a system of rigid bodies?
Of course it does. The net force on a system of bodies, rigid or not, determines the acceleration of the center of mass of the system. (Did your professor really say that it doesn't apply?)

Your reasoning above looks good to me.
 

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