General Atwood system with moment of inertia

AI Thread Summary
The discussion revolves around a project on Lagrangian mechanics, specifically the challenge of converting Lagrangian solutions to Newtonian format. The user is struggling with the signs in their equations for acceleration, particularly when comparing results from both methods. They derive an expression for acceleration that differs in sign from the Lagrangian result, leading to confusion regarding the moment of inertia's role. The user identifies a potential issue with the negative moment of inertia in their final equation, questioning how to justify this discrepancy. Clarification is sought on the correct formulation of tension and its impact on the angular acceleration equation.
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Homework Statement



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I have taken this image from http://farside.ph.utexas.edu/teaching/336k/lectures/node79.html

Hello, I am currently doing a project on Lagrangian mechanics. As part of my project, it was advised that I should redo each of the problems done using the Lagrangian method in the Newtonian format.

So essentially I am requesting help on determining the acceleration of the system

Homework Equations



F=m\ddot{x}

τ=Iα

τ=FR

The Attempt at a Solution



I am getting increasingly confused especially when the signs don't match :(
(a = radius of the pulley, not acceleration)
(acceleration is denoted as \ddot{x}

m_{1}\ddot{x_{1}}=T_{1}-m_{1}g
m_{2}\ddot{x_{2}}=T_{2}-m_{2}g

τ=Iα
τ=(T_{1}-T_{2})a

Tangential acceleration of the pulley is the same as the acceleration of the mass, assuming that there is absolute grip of the rope to the pulley.

\ddot{x}=αa

However we can see that

\ddot{x_{1}}=-\ddot{x_{2}}

Therefore,

m_{1}\ddot{x_{1}}=T_{1}-m_{1}g
m_{2}\ddot{x_{1}}=m_{2}g-T_{2}

and,

α=(T_{1}-T_{2})a/I
\ddot{x}=(T_{1}-T_{2})a^{2}/I

Adding the first 2 equations

m_{1}\ddot{x_{1}}+m_{2}\ddot{x_{1}}=T_{1}-T_{2}+m_{2}g-m_{1}g

Replacing the Tensions

m_{1}\ddot{x_{1}}+m_{2}\ddot{x_{1}}=\ddot{x}I/a^{2}+m_{2}g-m_{1}g

Finally rearranging it

(m_{1}+m_{2}-I/a^{2})\ddot{x_{1}}=(m_{2}-m_{1})g

\ddot{x_{1}}=\frac{(m_{2}-m_{1})g}{(m_{1}+m_{2}-I/a^{2})}

The signs are everywhere and completely different to the derivation obtained through the Lagrangian method. :I Can anyone explain what my issue is?

EDIT: Included the solution obtained via Lagrangian method

\ddot{x_{1}}=\frac{(m_{1}-m{2})g}{m_{1}+m_{2}+I/a^{2})}
 
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The minus sign difference in the numerator is not a problem but the minus sign in the detonator of your solution is a problem, the inertia of the pulley should have a plus sign, its inertia tends to reduce the acceleration of the system.
 
Thanks for your reply Spinnor,

I agree the problem is within the negative moment of Inertia in the final acceleration equation.

However, I can't seem to find a reason to justify it. (Doing so would somehow need to make the initial F=T-mg equation negative or somehow justify T_2 - T_1 instead of T_1 - T_2 for the angular acc. equation)
 
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