Net Torque / Rotational Dynamics Pulley System help

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Homework Help Overview

The problem involves a uniform solid cylinder and a disk-shaped pulley system, where a block is suspended from a string attached to the cylinder. The objective is to determine the acceleration of the block after the system is released from rest, using principles of rotational dynamics and torque.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the application of Newton's second law and torque equations for the block, cylinder, and pulley. There are attempts to verify the correctness of the equations set up for each component of the system. Questions arise regarding the forces acting on the cylinder and the role of friction in the torque calculations.

Discussion Status

Some participants have provided feedback on the original poster's equations, indicating which parts are correct and which need reconsideration. There is an ongoing exploration of the relationships between the forces and torques, with participants questioning assumptions about the forces involved.

Contextual Notes

There is a noted confusion regarding the expected form of the answer, as one participant mentions an unexpected numerical result that does not align with the requirement to express the answer in terms of the variables M and R.

elsternj
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Homework Statement


A uniform, solid cylinder with mass M and radius 2R rests on a horizontal tabletop. A string is attached by a yoke to a frictionless axle through the center of the cylinder so that the cylinder can rotate about the axle. The string runs over a disk-shaped pulley with mass M and radius R that is mounted on a frictionless axle through its center. A block of mass M is suspended from the free end of the string (the figure ). The string doesn't slip over the pulley surface, and the cylinder rolls without slipping on the tabletop.

Find the magnitude of the acceleration of the block after the system is released from rest.
Express your answer in terms of the variables M, R, and appropriate constants

YF-10-62.jpg

Homework Equations


\sumF=ma
\sum\tau = I\alpha
I = md2

The Attempt at a Solution


Let's take downward to be positive

For the block:
\sumF=ma
mg - T1 = ma

For the cylinder:
Rotational:
\sum\tau = I\alpha
T22R = 1/2m(2R)2\alpha

Translational:
T2 - f = ma

For the Pulley:
T1R-T2R = I\alpha

Okay so I am fairly new to understanding torque. First I want to know if my equations are correct and if I am including everything. I'm having trouble moving on from here also. Any insight would be greatly appreciated.
 
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elsternj said:
For the block:
\sumF=ma
mg - T1 = ma
Looks good.

For the cylinder:
Rotational:
\sum\tau = I\alpha
T22R = 1/2m(2R)2\alpha
No. The tension T2 does not exert a torque about the cylinder's center of mass. What force does?

Translational:
T2 - f = ma
Good.

For the Pulley:
T1R-T2R = I\alpha
Good. You'll need to express I in terms of M and R, of course.
 
No. The tension T2 does not exert a torque about the cylinder's center of mass. What force does?

Ah, I see it doesn't exert a torque because it is actually attached to the point of rotation, right?
So... friction? -f(2R) = 1/2m(2R)2\alpha ?

So oddly enough the answer to this question is 3.27 which kind of confuses me because I was expecting it to have to be in terms of M and R like it asks and we don't have any numbers for our variables. But... i'll worry about that when I get to there I suppose.
 
elsternj said:
Ah, I see it doesn't exert a torque because it is actually attached to the point of rotation, right?
So... friction? -f(2R) = 1/2m(2R)2\alpha ?
Exactly. (Get rid of that minus sign, though.)

So oddly enough the answer to this question is 3.27 which kind of confuses me because I was expecting it to have to be in terms of M and R like it asks and we don't have any numbers for our variables. But... i'll worry about that when I get to there I suppose.
Solve it and see for yourself. It's quite possible that those M's and R's end up canceling. :wink:
 

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