Ball rolls without slipping in an accelerating car

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Homework Help Overview

The problem involves a bowling ball rolling without slipping in a horizontally accelerating subway car. Participants are exploring the relationship between the acceleration of the car and the acceleration of the ball, considering the effects of friction and torque.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the role of friction in generating torque on the ball and how it affects the ball's acceleration relative to the car's acceleration. There are attempts to set up equations relating the forces and accelerations involved, with some questioning the correctness of their calculations.

Discussion Status

Some participants have provided guidance on using the accelerated frame of reference to analyze the problem, while others are exploring different interpretations of the equations involved. There is an ongoing examination of the relationships between the various accelerations and forces, with no explicit consensus reached yet.

Contextual Notes

Participants are working under the assumption that the ball rolls without slipping and are considering the implications of this condition on the forces and torques at play. There is also a mention of the fictitious force in the accelerated frame, which adds complexity to the analysis.

astrocytosis
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Homework Statement


A bowling ball sits on the smooth floor of a subway car. If the car has a horizontal acceleration a, what is the acceleration of the ball? Assume that the ball rolls without slipping.

Homework Equations


torque = R x F = Iα
aball= Rα
Isphere = (2/5) MR2

The Attempt at a Solution


This seems like a simple problem but I'm struggling with it. If the ball is rolling without slipping, then there must be some friction force ƒ causing a torque on the ball equal to Rƒ = (2/5) MR2 * (aball/R). It's not on a ramp so the weight of the ball doesn't contribute to the torque. I guess I just can't figure out how to relate the acceleration of the car to all of this.

I had a thought that without friction, in the frame of the car, the ball would simply be accelerating at the same rate as the car, so the difference in acceleration must somehow be the result of friction. Friction here is ƒ = (2/5)Maball, so the difference in net force on the ball in the cases with and without friction is macar-maball=ƒ. But solving for the acceleration here does not get me the right answer so this reasoning must be flawed.

The correct answer according to the text is 2a/7. With my reasoning I get 5a/7.
 
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The approach is good, you have two equations with two unknowns. Apparently something went wrong in the calculations you didn’t show.
 
Macar-Maball = (2/5) Maball

M (mass of ball) cancels

acar=aball + (2/5) aball = (7/5) aball

So aball = (5/7) acar.

Am I missing something in this equation?
 
You can get the answer by doing the problem correctly in the accelerated frame. In that frame, there is a fictitious force ##F=m_{ball}~a_{car}## acting in a direction opposite to the actual acceleration of the car. This force generates a torque ##\tau## about the point of contact P. Write the torque equation ##\tau = I_P~\alpha_{ball}## where ##I_P## is the moment of inertia about point P, not the center of the ball. Solve the equation and the correct answer will plop out.
 
By the parallel axis theorem, IP = (2/5)MR2 + MR2 = (7/5)MR2

Then the torque is (7/5)MR2 *(aball/R) = R*F = RMcar

I'm still getting aball = 5acar/7 when I solve this equation, though.
 
Don't forget that the aball calculated this way is in the accelerated non-inertial frame. What is it in the inertial frame of the track?
 
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Oh I see... I just have to subtract the acceleration of the car then. Thanks!
 

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