Mastering Physics: Acceleration of a Pulley

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Homework Help Overview

The problem involves a uniform solid cylinder with a string wrapped around it, connected to a block. The goal is to find the angular acceleration of the cylinder as the block descends, with both the cylinder and block having mass m. The context includes the application of Newton's laws and rotational dynamics.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the equations used to relate tension, angular acceleration, and forces acting on the system. There are attempts to derive the angular acceleration and questions about the validity of certain steps in the algebraic manipulation.

Discussion Status

Some participants have provided guidance on re-evaluating the algebraic steps taken in the original poster's attempt. There is an ongoing exploration of the relationships between tension, torque, and the forces acting on the block and cylinder. Multiple interpretations of the equations are being discussed without a clear consensus on the correct approach.

Contextual Notes

Participants are questioning the assumptions made in the derivation of the equations, particularly regarding the forces acting on the block and the cylinder. There is also mention of alternative methods, such as using energy considerations, to verify results.

danielhep
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Homework Statement


A string is wrapped around a uniform solid cylinder of radius r, as shown in (Figure 1) . The cylinder can rotate freely about its axis. The loose end of the string is attached to a block. The block and cylinder each have mass m.
Find the magnitude α of the angular acceleration of the cylinder as the block descends.
upload_2017-4-15_19-12-53.png


Homework Equations


F=ma=mg-T
Torque=Iα=-Tr
a=-rα
I=mr2/2

The Attempt at a Solution


I use these three equations to eliminate T and solve for α.

m(-rα)=mg-T
-1/2mr=T
-mrα=mg+1/2mr
-α=g/r+1/2
α=-1/2-g/r

I tried this answer however it was wrong.

Mastering says the correct answer is
α = 2g/3r

I'm really not sure where this comes from, so any help would be great! I need to understand where I went wrong.
 
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danielhep said:
-1/2mr=T
Where did this come from? It doesn't look right.

Edit: Okay, now I see what you did. You were equating Iα to -Tr, then substituting I = mr2/2 for I. You should work through that algebra again and I think you'll find your problem.
 
TomHart said:
Where did this come from? It doesn't look right.

Edit: Okay, now I see what you did. You were equating Iα to -Tr, then substituting I = mr2/2 for I. You should work through that algebra again and I think you'll find your problem.
I dropped the g. Thank you so much! I found the correct answer.
 
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why is Iα = -Tr. Shouldn't the force acting on it be mg since T (from cylinder to block) - T (from block to cylinder) -mg = mg? Or shouldn't it be mg - T, which is what we defined the net force as above.
 
qdnwedowlnd said:
why is Iα = -Tr. Shouldn't the force acting on it be mg since T (from cylinder to block) - T (from block to cylinder) -mg = mg? Or shouldn't it be mg - T, which is what we defined the net force as above.
It won't just be mg as that would assume that there is no acceleration of the mass.

The pulley experiences a torque just due to the Tension, so that is why I\ddot{\theta} = Tr (or with a minus sign if you choose to define in other direction), and then the other terms come into play when we substitute our expression that we get from Newton's 2nd law on the mass.

Note: you can also solve this by energy and differentiate to get \ddot{\theta} to check your answer.

Hope that helps.
 
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