I Newton's second law for rotations

AI Thread Summary
The discussion revolves around understanding Newton's second law for rotations and the conditions necessary to initiate the rotation of a homogeneous bar. The original poster mistakenly overlooked the law of inertia and sought clarification on the force required to overcome the moment of inertia while the bar is in static equilibrium. Participants emphasized that any net force can cause movement and rotation in the absence of resisting forces, highlighting the relationship between linear and angular motion. Additionally, there was confusion regarding the interpretation of an attached image, with suggestions that the development of equations appeared coherent despite initial misunderstandings. The conversation underscores the importance of recognizing torque and forces acting through the center of mass in rotational dynamics.
pedrovisk
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What is the minimum force to start rotation in a bar?
EDIT: I forgot about Second Newton's law for rotations and this led to a mistake. Anyway, thanks for the people who answered it and remembered me about law of inertia.

I was thinking about how to "make" things to move without rotate the object, then i tried to calculate the minimum force to start a homogeneous bar to rotate in a x axis. I attached a link.
Could someone check if my answer is correct?

 
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:welcome:

What force is resisting rotation?
 
PeroK said:
:welcome:

What force is resisting rotation?
Hi! The bar is at static equilibrium. What I meant with this force F is what "push" I need to do in order to "win" the moment of inertia.
 
pedrovisk said:
Hi! The bar is at static equilibrium. What I meant with this force F is what "push" I need to do in order to "win" the moment of inertia.
I don't know what "win" means in this context. In the absence of a resisting force, any force (no matter how small) will move and rotate the bar.
 
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It is like asking what force is required to make an object accelerate when there is no resisting force. F = ma tells you that any net force will result in an acceleration, just as ##T = I\alpha## tells you any net torque will result in an angular acceleration.
 
Orodruin said:
It is like asking what force is required to make an object accelerate when there is no resisting force. F = ma tells you that any net force will result in an acceleration, just as ##T = I\alpha## tells you any net torque will result in an angular acceleration.
Can't believe i forgot about this. Basic Newton's first law for rotations.

I think I was confused when I was trying to rotate a bar like that. I probably just forgot about the friction.

Anyway, now I'm curious. Is there any meaning for the pic I attached?
 
PeroK said:
I don't know what "win" means in this context. In the absence of a resisting force, any force (no matter how small) will move and rotate the bar.
Thanks, you are absolutely right. I was having trouble to understand rotations as a extension of Newton's laws.

Asking the same question I did to Orodruin, what is a possible interpretation for the pic? Did it have a meaning or I should just torn it apart the paper and throw it to the trash? The development of the equations looks so smooth.
 
pedrovisk said:
Thanks, you are absolutely right. I was having trouble to understand rotations as a extension of Newton's laws.

Asking the same question I did to Orodruin, what is a possible interpretation for the pic? Did it have a meaning or I should just torn it apart the paper and throw it to the trash? The development of the equations looks so smooth.
You have a torque of ##F\frac l 2##. Somehow you have an opposing torque of ##\frac{mlg}{4}##.
 
PS gravity acts through the centre of the bar, so it should not produce a torque on the bar about its centre.
 
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pedrovisk said:
I was thinking about how to "make" things to move without rotate the object,
Apply all force through the center of mass, otherwise make sure that the torques cancel.
 
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