General Atwood system with moment of inertia

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SUMMARY

The discussion focuses on resolving discrepancies in the acceleration equations derived from Lagrangian mechanics versus Newtonian mechanics for a system involving a pulley with moment of inertia. The user presents their equations, including F = m\ddot{x} and τ = Iα, and expresses confusion over sign differences in the results. The final derived equation for acceleration, \ddot{x_{1}} = \frac{(m_{2}-m_{1})g}{(m_{1}+m_{2}-I/a^{2})}, contrasts with the Lagrangian result, highlighting a critical misunderstanding regarding the treatment of moment of inertia in the context of acceleration. The user seeks clarification on the negative sign in their equation.

PREREQUISITES
  • Understanding of Lagrangian mechanics and its application in classical mechanics.
  • Familiarity with Newton's laws of motion, particularly F = m\ddot{x}.
  • Knowledge of rotational dynamics, including torque and moment of inertia.
  • Ability to manipulate and solve differential equations related to motion.
NEXT STEPS
  • Study the derivation of acceleration in systems with pulleys using both Lagrangian and Newtonian methods.
  • Learn about the implications of moment of inertia on system dynamics in classical mechanics.
  • Explore the concept of tension in ropes and its effects on angular acceleration.
  • Investigate common pitfalls in sign conventions when transitioning between Lagrangian and Newtonian frameworks.
USEFUL FOR

Students and professionals in physics, particularly those studying classical mechanics, engineers working on mechanical systems involving pulleys, and anyone interested in the application of Lagrangian mechanics to real-world problems.

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Homework Statement



img1622.png


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)
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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