Rotational Motion of a disc of mass

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Homework Help Overview

The discussion revolves around a problem involving the rotational motion of a disc with mass M and radius R, which is rolling down an incline while dragging another mass M. The participants are trying to determine the linear acceleration of the mass M, considering the forces acting on both the disc and the attached mass.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to relate the static friction force to the linear acceleration but struggles to define fs clearly. Some participants question the meaning of fs and its relation to gravitational and frictional forces. Others discuss the application of Newton's laws to both rotational and translational motion.

Discussion Status

The discussion is active, with participants exploring different interpretations of the static friction force and its implications for finding the linear acceleration. Some guidance has been offered regarding the relationship between acceleration and static friction, but there is no explicit consensus on the approach to take.

Contextual Notes

There is a noted confusion regarding the order of finding the linear acceleration and the frictional force, as well as a specific constraint mentioned by the teacher regarding the definition of fs.

PhysicsNewb
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I'm stuck on a miniquestion in my HW that is hindering the entire problem, so here it is.

A disc of mass M, radius R, Icm =1/2MR^2 is rolling down an incline dragging a mass M attached with a light rod to a bearing at the center of the disc. The friction coefficients are the same for both masses, us and uk.

Determine the linear acceleration of the mass M.

Well, this question seems easy, and I ended up with 2fs/M = a.
But I need to find out what fs is to simplify my answer, and I can't figure out how.
 
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I don't see how anyone can tell you what fs IS if you don't tell us what it MEANS. I might guess, since it is "f", that it is a force and then guess that "s" means directed along the incline, but I'm still not sure whether it is the force of gravity along the incline or the retarding force due to friction.

If it is gravitational force, then it is -2Mgsin(θ) where θ is the angle the incline makes with the horizontal. (Notice the 2. Gravity pulls on both masses.)

If it is the friction force then it is μMgcos(θ) where Mgcos(θ) is the force normal to the plane due to the weight of the second mass. The disk is rolling so there is no sliding friction.
 
I'm sorry I should have been clearer. fs is the frictional force, except on my paper my teacher said that fs does not equal uMGcos(theta), which is the source of my problem. He says fs equals 1/2Ma, which is where I got a = 2fs/M from.

Sum of the torques = I(angular acceleration)
fsR = 1/2MR^2(a/R)
fs = 1/2Ma
 
Last edited:
PhysicsNewb said:
He says fs equals 1/2Ma, which is where I got a = 2fs/M from.
That comes from applying Newton's 2nd law to the rotational motion of the cylinder. ([itex]\tau = I \alpha[/itex]) Now apply Newton's 2nd law to the translational motion of the entire system.
 
Okay, here is the source of my confusion about this problem. First it says find the linear acceleration of mass M, then the following question asks me to find the frictional force acting on the disc. But don't I need to find the frictional force before I find the acceleration?
 
PhysicsNewb said:
But don't I need to find the frictional force before I find the acceleration?
No. In fact, the only way you can find the static friction on the disc is to find the acceleration, since it depends on the acceleration. Try it!

(Static friction is a "passive" force--it can adjust to be whatever it needs to be up to a maximum value.)
 

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