Moment of inertia where mass and torque are at a different positions

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Discussion Overview

The discussion revolves around the concept of moment of inertia, particularly in scenarios where mass and torque are applied at different positions relative to a pivot point. Participants explore the implications of this separation on the validity of the moment of inertia formula, its derivations, and the underlying physics principles.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express concern that the two different positions of mass and torque in the moment of inertia formula (I=mr²) complicate its application when they do not coincide.
  • Others argue that the derivation of moment of inertia models the rigid body as a collection of point masses, suggesting that applying force at a different location does not align with the assumptions of the model.
  • Several participants highlight that the moment of inertia for a point particle is given by I=mr², but for non-point bodies, it can be more complex, involving a volume integral that accounts for mass density and geometry.
  • One participant mentions that the moment of inertia depends on the axis of rotation and the distribution of mass, indicating that different configurations can yield different moments of inertia.
  • There is a discussion about the relationship between torque and work, with some participants asserting that the moment of inertia is influenced by both concepts, while others maintain that the derivation is strictly based on Newton's second law.
  • A later reply provides a detailed derivation of angular momentum and torque in rigid body dynamics, emphasizing that all points in the rigid body experience the same angular motion, which may not require the concept of work for understanding the moment of inertia.

Areas of Agreement / Disagreement

Participants generally do not reach a consensus, as multiple competing views remain regarding the implications of applying force at different locations and the relationship between torque, work, and moment of inertia.

Contextual Notes

Limitations include the assumptions made in the derivation of moment of inertia, the dependence on the chosen axis of rotation, and the complexity introduced by real-world factors such as the mass of levers or other systems involved.

  • #61
sophiecentaur said:
If you replace torque and MI by Force and Mass, you will see how nonsensical that statement appears. You seem to be determined to fit the Science to your personal intuition. That ain't going to work. It has to be the other way round.
I told OP 2-3 times that the moment of inertia doesn't depend where we apply the torque and how big/small is the torque, but I refrain myself of doing it over and over again. OP chooses perplexed examples (like that of cars with smaller/bigger wheels, or that with the plank and the point mass) where a change in torque comes simultaneously with a change in moment of inertia and that gives OP the false impression that the moment of inertia depends on the torque.
 
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  • #62
chananyag said:
Hope I got it right
You did not. What is the force on each mass? Also, please use units when you write down numbers.
 
  • #63
sophiecentaur said:
If you replace torque and MI by Force and Mass, you will see how nonsensical that statement appears. You seem to be determined to fit the Science to your personal intuition. That ain't going to work. It has to be the other way round.
My original understanding was that τ=Iα should only apply where the torque and mass are at the same position - unless the moment of inertia changes. My mistake was that it was F=ma, not τ=Iα, which doesn't directly apply when the force and mass at different positions. You can repeat ad nauseam that my conclusion is wrong, but it’s far more helpful if you can explain why by pointing out the false premises. Actually #2 did so, but in a hand-waving way so I didn’t really get what they were saying. It took me a while to pinpoint my original mistake, but I think I got there.

I think your accusation is unfair. My original question was mathematical one, not based on intuition, although I did discuss intuition in the thread (perhaps more than I should have).
 
  • #64
Delta2 said:
I told OP 2-3 times that the moment of inertia doesn't depend where we apply the torque and how big/small is the torque, but I refrain myself of doing it over and over again.
I'm afraid telling isn't enough. You need to explain. I admit I was a bit stubborn, and I apologise for that, but those who explained to me why I was wrong and what my missteps were got further than those who just asserted I was wrong.

I also had a lot of other misunderstandings on the subject, which came clear as we went along.
 
  • #65
chananyag said:
I'm afraid telling isn't enough. You need to explain. I admit I was a bit stubborn, and I apologise for that, but those who explained to me why I was wrong and what my missteps were got further than those who just asserted I was wrong.

I also had a lot of other misunderstandings on the subject, which came clear as we went along.
I tried to explain, I gave the general formula the MoI and from that it seems that MoI doesn't depend on Torque , torque doesn't appear anywhere in that formula. It depends on where we put the axis of rotation though and how is the mass density distribution around the axis of rotation. You choose perplexed examples where the changes in the two aforementioned quantities come together with a change in torque (like the example of car with bigger/smaller wheels) and that gives you the false impression that the MoI depends on torque.

@kuruman and others might find your examples interesting and try to explain you in detail where you get wrong, I am afraid I just don't find them so interesting. My area of expertise is not classical mechanics anyway.

And yes you are stubborn especially on trying to fit science to your personal intuition as @sophiecentaur very successfully said.
 
  • #66
Delta2 said:
where a change in torque comes simultaneously with a change in moment of inertia
chananyag said:
My mistake was that it was F=ma, not τ=Iα, which doesn't directly apply when the force and mass at different positions.
chananyag said:
You need to explain. I admit I was a bit stubborn,
Actually, no one 'needs' to explain. Those are not the terms of PF interchanges. You are the one with the 'need' and all PF can do is to state the facts and, perhaps, explain away popular misconceptions. You will appreciate that your reactions all seem like a last ditch stand to maintain that you are actually right. This is hard to deal with.
My suggestion is, again, to apply the logic that applies with F = ma and to get the causal relationship in the right direction. Let me try this: A given point mass cannot be altered but the MI of an object varies with the axis you choose. The minimum MI is when the axis is through the CM. (If you are familiar with basic statistics, the Standard Deviation is equivalent to the MI) MI about other axes increases (and the SD of a distribution is minimal about the mean and increases from side to side). So we have the same object which is harder to rotate if you want it to rotate about a point that's not the CM because the MI has increased. So MI is a property of the object (as with Mass) but it depends on the reference axis. That makes total sense when you think about it.
If you want to give a certain value of angular acceleration to an object then the Torque required will depend on which axis you want to rotate it about.
I am labouring this point because I think it is what your problem is all about. Cause and Effect...
 
  • #67
kuruman said:
You did not. What is the force on each mass? Also, please use units when you write down numbers.
Here’s my calculation for #56:

1. Net torque is [(20kg)(9.8m/s^2) × (2.5m)] – [(5kg) (9.8m/s^2) × (5m)] = 490Nm -245Nm = 245Nm
2. The common acceleration is α = τ/I = 245Nm/[(20kg)(6.25m)] + (5kg)(25m)] = 245Nm/250kg m^2 = 0.98 rad/s^2
3. The COM is at 1m from the pivot. The tangential acceleration should then be 0.98 m/s^2
4. The force on the COM is (25Kg)(0.98m/s^2) =245N
5. The tangential acceleration of the left mass is (0.98 rad/s^2)(2.5m) = 2.45m/s^2. The force on the left mass is therefore (20kg)(2.45m/s^2) = 49N
6. The tangential acceleration of the right mass is (0.98 rad/s^2)(5m) = 4.9 m/s^2. The force on the right mass is therefore (5kg)(4.9 m/s^2) = 24.5N

I think I have a better grasp on the issues now, and have cleared up my initial misunderstandings. Thanks all for your help and patience! It took a while, but I learned a lot.
 
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  • #68
chananyag said:
Here’s my calculation for #56:

1. Net torque is [(20kg)(9.8m/s^2) × (2.5m)] – [(5kg) (9.8m/s^2) × (5m)] = 490Nm -245Nm = 245Nm
2. The common acceleration is α = τ/I = 245Nm/[(20kg)(6.25m)] + (5kg)(25m)] = 245Nm/250kg m^2 = 0.98 rad/s^2
3. The COM is at 1m from the pivot. The tangential acceleration should then be 0.98 m/s^2
4. The force on the COM is (25Kg)(0.98m/s^2) =245N
5. The tangential acceleration of the left mass is (0.98 rad/s^2)(2.5m) = 2.45m/s^2. The force on the left mass is therefore (20kg)(2.45m/s^2) = 49N
6. The tangential acceleration of the right mass is (0.98 rad/s^2)(5m) = 4.9 m/s^2. The force on the right mass is therefore (5kg)(4.9 m/s^2) = 24.5N

I think I have a better grasp on the issues now, and have cleared up my initial misunderstandings. Thanks all for your help and patience! It took a while, but I learned a lot.
All that is correct. i am happy that you have a better grasp now.
 
  • #69
What I can see is that OP has not replied to anyone in the thread after posting his/her question.
 
  • #70
chananyag said:
I think I have a better grasp on the issues now, and have cleared up my initial misunderstandings. Thanks all for your help and patience! It took a while, but I learned a lot.
That's great; well done.
Now you are convinced that the 'theory' gives a 'convincing' answer, the next step is to see it working in symbolic (algebraic) form. That half page of numbers would all change if you used a slightly different set of conditions, moreover, when you use numbers, they lose their identity when you multiply them together and a final numerical answer doesn't tell you how it arrived. The algebra stays the same for all the numbers - you know what I mean.
So now you should look at the formulae and try to see the 'forms' without the numbers - like where there are squared values or divisions etc. etc. and see how that all goes to give the answer. You should find that your grasp improves further.
 
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