How to Solve Atwood's Problem with a Massive Pulley?

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Homework Help Overview

The discussion revolves around Atwood's machine, specifically analyzing the dynamics of two masses connected by a rope over a pulley with a given moment of inertia. Participants are exploring how to determine the accelerations of the blocks and the angular acceleration of the pulley using different approaches, including Newton's laws and conservation of energy.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to solve the problem using conservation of energy and expresses uncertainty about applying Newton's laws. They also seek confirmation of their calculated acceleration.
  • Another participant provides a set of equations derived from Newton's laws, suggesting a method to eliminate tensions and derive an expression for acceleration.
  • Further discussion arises regarding the implications of assuming a massless pulley and whether this leads to equal tensions in the rope.

Discussion Status

Participants are actively engaging with different methods to approach the problem. Some guidance has been offered regarding the correctness of the original poster's answer using the Newton's laws approach. There is an ongoing exploration of the implications of a massless pulley on tension in the system.

Contextual Notes

Participants are navigating the complexities of the problem, including the effects of the pulley's mass and moment of inertia on the dynamics of the system. The original poster expresses a desire for verification of their calculations and understanding of the underlying principles.

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Homework Statement



In the Atwood's machine shown below the masses of the blocks are ma = 3kg and mb = 2kg. The moment of inertia of this frictionless pulley about its axis is Ic = .6 kg m2 and its radius is Rc = .2m. Note that there is no slipping between the rope and the pulley.

Find the accelerations of the blocks and the angular acceleration of the pulley

http://commons.wikimedia.org/wiki/File:Atwoodmachine.gif
this is the closest diagram i could find... the distance of the right block (I'll name it block 2 and the left block 1) above the ground is h.

I thought of two ways to do this problem, but I wanted to try and use Newton's laws.
I solved it using conservation of energy:
EPot f - EPot i + Kfinal - Kinitial = 0
so we know that:

Kinitial = 0 (since its not moving yet)
EPot f = m1(g)(h)
EPot i = m2(g)(h)
Kfinal = (1/2)m2v2 + (1/2)m1v2 + (1/2) Iw2

then using vf2= vi2+2ah
again vii = 0, so we can now replace every vf2 by 2ah

at this point you have:
m1(g)(h) - m2(g)(h) + (1/2)(ma)(2ah) + (1/2)(m1)(2ah) + (1/2)(I)(2ah/R2)

Now cancel out all the h's and get:
m1(g) - m2(g) + (1/2)(ma)(2a) + (1/2)(m1)(2a) + (1/2)(I)(2a/R2)

After solving for a I got a = .49 m/s2 of the blocks (I'm not concerned with the angular acceleration right now)

I think my answer is right but..
Is there any way to use Newton's Laws... Maybe use the following?
m2(g) - T2 = m2(a)
T1 - m1(g) = m1(a)
Or does this only apply for massless pulleys?
I tried using it, and I get a different Answer... Also if someone could check my answer itd be nice
 
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M1g - T1 = M1a
T2 - M1g = M2a
torque (t) = T1R - T2R = Ia/r

eliminate T1,T2

M1g -M2g - (T1-T2) = (M1 + M2)a

T1 - T2 = Ia/r^2

M1g - M2g - Ia/r^2 = (M1 + M2)a

a = (M1 - M2)g/(M1 + M2 + I/r^2 )

massles pulley implies I = 0

your answer 0.49 is correct using this approach
 
resaypi said:
M1g - T1 = M1a
T2 - M1g = M2a
torque (t) = T1R - T2R = Ia/r

eliminate T1,T2

M1g -M2g - (T1-T2) = (M1 + M2)a

T1 - T2 = Ia/r^2

M1g - M2g - Ia/r^2 = (M1 + M2)a

a = (M1 - M2)g/(M1 + M2 + I/r^2 )

massles pulley implies I = 0

your answer 0.49 is correct using this approach

Thanks for the help, I get it now... Just another question though... When we consider the pulley to massless does it mean that the tensions are equal? Since T1-T2=Ia/r2 Or am I jumping to a false conclusion? Thanks again
 
True, if we consider the pulley massless T1 = T2. The difference is due to the fact that there is a friction force that turns the pulley.
 

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