Rotational Motion of a disk and a box

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The discussion revolves around a physics problem comparing the motion of a disk and a box of equal mass sliding down two inclines. The key point is that the disk is assumed to roll due to friction, while the box slides without friction. Participants express confusion about the role of friction and torque on the disk, emphasizing that without friction, the disk cannot roll. The solution involves applying Newton's second law to determine the linear acceleration of both objects down the incline. Ultimately, the problem aims to establish how much sooner the box reaches the bottom compared to the disk.
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Homework Statement



A disk and a box of equal mass are released from the top of two inclines both of which are a height h above the ground and make an angle θ to the horizontal. Let the radius of the disk be R. How much sooner does the box reach the bottom of the incline than the disk?
Express your answer in terms of some or all of the variables m, h, theta, and R, as well as the acceleration due to gravity g.

Homework Equations





The Attempt at a Solution



I am completely stumped. Please advice me on how to do this problem.

Thanks a ton for the help and advice!
 
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Is there friction? My guess is that they want you to assume friction for the disk (so it will roll) and no friction for the box.

Find the linear acceleration of each as they go down the incline. (Apply Newton's 2nd law to both. Be sure to include rotation for the disk.)
 
Thats the problem!

That's precisely the problem. We are asked to assume that there is no friction which is why I am confused as to what will cause the torque on the disk! Please advise.
 
If there's no friction, the disk will slide not roll.
 
Thanks for that. I'll keep that in mind and look into the problem again!
 
Despite the sloppy wording about "no friction", what I presume they want you to compare is the rolling of the disk versus the sliding of the box. The disk must have friction to roll, but the box should have none. I would solve the problem using that assumption.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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