Finding Acceleration of Ball on Paper

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SUMMARY

The discussion focuses on determining the acceleration of a ball resting on a piece of paper that is being pulled horizontally with acceleration 'a'. The key conclusion is that the ball experiences both translational and rotational motion due to the force exerted by the paper. The correct relationship for the ball's acceleration is derived as 'aball = 2apaper/5', indicating that the ball's acceleration is influenced by both the paper's acceleration and the ball's rotational dynamics. The analysis utilizes Newton's 2nd law and the concept of rolling without slipping to arrive at this conclusion.

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Homework Statement


I have a heavy ball on a piece of paper on the floor. The paper is grabbed and moved horizontally with acceleration a. What is the acceleration of the center of the ball? The ball is assumed to not slip with respect to the paper.


Homework Equations





The Attempt at a Solution


I'm not really sure how the acceleration is supposed to interact with the ball. A thought I've had is to say that the ball doesn't translate but rotates with angular acceleration a/R since it doesn't slip.
 
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boardbox said:
A thought I've had is to say that the ball doesn't translate but rotates with angular acceleration a/R since it doesn't slip.

*** Edited after reading Doc Al's Comment ***

That's almost it. See Doc Al's comment below.
 
Last edited:
boardbox said:
A thought I've had is to say that the ball doesn't translate but rotates with angular acceleration a/R since it doesn't slip.
Careful. The paper exerts a force on the ball, so the ball must translate as well as rotate. Both the ball and the surface (the paper) are accelerating, but at different rates. So you can't just assume that the angular acceleration is a/R.

Hint: Assume that the paper exerts some force F on the ball. Analyze the translational and rotational dynamics of the ball using Newton's 2nd law.
 
\SigmaFball = Fpaper = maball
\Sigmat = tpaper = I \alpha
t = r x F
\alpha = apaper/r

plug and chug

aball = 2apaper/5

does that get it about right?
 
Last edited:
boardbox said:
\SigmaFball = Fpaper = maball
OK.
\Sigmat = tpaper = I \alpha
t = r x F
OK.
\alpha = apaper/r
No. Alpha is the rotation about the center of mass--compare the acceleration of the paper with the acceleration of the center of mass.

(But you're on the right track!)
 
Last edited:
Would it be the sum of the two accelerations over the radius?

I think rolling without slipping is \omega = v/r so the acceleration version of that should just be the time derivative. If I have a a constant v on the paper and the ball I would expect to just sum them.
 
boardbox said:
Would it be the sum of the two accelerations over the radius?
What if the center of mass had the same acceleration as the paper? What would be the rotational acceleration of the ball in that case?
 
Zero?
You highlight sum. I'm wondering if you want magnitude of difference?
 
boardbox said:
Zero?
Exactly. If you just added them you'd get alpha = 2a/r, which doesn't make sense.
You highlight sum. I'm wondering if you want magnitude of difference?
What you need to find alpha is the relative acceleration of paper and ball divided by r.
 
  • #10
I see, makes sense. Thanks for the help.
 

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