Does Newton's Third law apply to torque/rotation?

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The discussion revolves around the application of Newton's Third Law (N3L) to torque, particularly in systems involving gears of different sizes. It is clarified that while equal and opposite forces can create equal and opposite torques, this only holds true when the forces act at the same radius from the same pivot point. In the case of gears, the differing diameters lead to unequal torques, which is a fundamental aspect of their mechanical advantage. The conversation emphasizes that N3L applies to the interaction at the contact point between the gears, but the torques around different axes cannot be directly equated. Ultimately, the participants agree that while internal torques in a system must sum to zero, this does not imply that every individual torque has an equal and opposite counterpart.
  • #31
alkaspeltzar said:
Dale, i agree. If i pick Gear A axis and sum the torques about A, they do sum to zero. But that doesn't mean there is a N3L for torque does it? IF so, if gear B in my example has 50 inches pounds on it, where does its equal and opposite torque get applied?
Let's say you were teaching a junior student about Newton's laws and they would not accept that force had a direction. They kept talking about force as a magnitude only. And, no matter how many times you told them that force was a vector and had a magnitiude and direction, they just kept repeating the same mistake by considering only the magnitude of all the forces.

What would you do?

Because, really, as far as persuading you that a torque is always relative to a point, I'm out of ideas. Sorry. Your stubbornness has defeated me.
 
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  • #32
russ_watters said:
As I said above, it's your problem and you need to specify what's in it. You specified two equal/opposite torques for A, but you didn't for B. So you tell us. Is gear B connected to a shaft that has an applied torque?
[edit] Oh; you said there's a motor at B. The motor provides the other torque.

Here is the problem. A is the driver gear. It has a motor providing 10 inch lbs to it. B is the driven gear.

I see a 10 lb force acting at B, which is 5 away. THat is 50 inch lbs. Let's assume B is a wheel touching the ground
1611684157411.png
 
  • #33
alkaspeltzar said:
Here is the problem. A is the driver gear. It has a motor providing 10 inch lbs to it. B is the driven gear.
That's a different drawing and description from what you provided before. So just remove my edit: you need to tell us what gear B is connected to. A shaft? A wheel touching the ground? What? In order for the torques to sum to zero, there needs to be a second torque on gear B, opposing the torque applied by gear A.
 
  • #34
alkaspeltzar said:
Here is the problem. A is the driver gear. It has a motor providing 10 inch lbs to it. B is the driven gear.

1611684157411-png.png

You have 2 torque interactions here, and the N3 applies to each of them, when taken around the same point :

torque_by_MOTOR_on_A = -torque_by_A_on_MOTOR
torque_by_B_on_A = -torque_by_A_on_B
 
  • #35
alkaspeltzar said:
If i pick Gear A axis and sum the torques about A, they do sum to zero. But that doesn't mean there is a N3L for torque does it?
Yes, it does.

The point of N3 is the conservation of momentum. The point of the torque version is the conservation of angular momentum. Angular momentum requires the specification of one single axis about which all angular momenta are measured. That is just how angular momentum works.
 
  • #36
russ_watters said:
That's a different drawing and description from what you provided before. So just remove my edit: you need to tell us what gear B is connected to. A shaft? A wheel touching the ground? What? In order for the torques to sum to zero, there needs to be a second torque on gear B, opposing the torque applied by gear A.

Russ, i have edited my picture to show A is connected to a Motor, on the ground. And B is a wheel touching the ground.
1611684526215.png
 
  • #37
alkaspeltzar said:
Russ, i have edited my picture to show A is connected to a Motor, on the ground. And B is a wheel touching the ground.
View attachment 276893
So, the ground a applies a torque around B, equal and opposite of what gear A applies.
 
  • #38
alkaspeltzar said:
Russ, i have edited my picture to show A is connected to a Motor, on the ground. And B is a wheel touching the ground.

1611684526215-png.png

If there are no horizontal forces between B and ground, it's still the same:

When taken around the same point:

torque_by_MOTOR_on_A = -torque_by_A_on_MOTOR
torque_by_B_on_A = -torque_by_A_on_B

Otherwise there is also:

torque_by_GROUND_on_B = -torque_by_B_on_GROUND
 
Last edited:
  • #39
A.T. said:
torque_by_B_on_A = -torque_by_A_on_B

NO

The vector torque is an axial vector. To uniquely define a torque on an extended body one must specify the axis (or equivalently the point of application) of the torque. Within this definition a strong form of Newton's 3rd Law Rotational applies: there is an equal and opposite torque at the same point of application (or along the exact same axis equivalently) from the torquee to the torquer.
The equivalent Newtons Law for forces also tacitly assumes the line of action of the forces is coincident.

The case listed above is not correctly analyzed by the Newton 3rd rotational law because the axes are not coincident.
 
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  • #40
hutchphd said:
NO

The vector torque is an axial vector. To uniquely define a torque on an extended body one must specify the axis (or equivalently the point of application) of the torque. Within this definition a strong form of Newton's 3rd Law Rotational applies: there is an equal and opposite torque at the same point of application (or along the exact same axis equivalently) from the torquee to the torquer.
The equivalent Newtons Law for forces also tacitly assumes the line of action of the forces is coincident.

The case listed above is not correctly analyzed by the Newton 3rd rotational law because the axes are not coincident.
So I asked that at the beginning of my post. N3l for torques only applies if the forces are inline and act at the same point, THerfore same radius.

So with these gears, yes Ang. Momentum must still be conserved, but I cannot say there is a n3l for torques
 
  • #41
hutchphd said:
... because the axes are not coincident.
I have explicitly specified this in all previous posts :
A.T. said:
..., when taken around the same point
except in the last update one you quoted. Will add it now.
 
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  • #42
alkaspeltzar said:
So I asked that at the beginning of my post. N3l for torques only applies if the forces are inline and act at the same point, THerfore same radius.

So with these gears, yes Ang. Momentum must still be conserved, but I cannot say there is a n3l for torques
Picard.jpg
 
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  • #43
alkaspeltzar said:
So I asked that at the beginning of my post. N3l for torques only applies if the forces are inline and act at the same point, THerfore same radius.
"Therefore same radius" is not true. You seem to be applying Newtons 3rd law to any torques that are equal and I have no idea what your question is at this point.
Would you care to try again?
 
  • #44
alkaspeltzar said:
...but I cannot say there is a n3l for torques
How would a N3L for torques look like to you?
 
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  • #45
A.T. said:
How would a N3L for torques look like to you?
I have been asking where does the 50 inch lbs torque about B get balanced out.
 
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  • #46
alkaspeltzar said:
I have been asking where does the 50 inch lbs torque about B get balanced out.
I agree with this, but what happens to the torque about B. Do we ignore it since it's not relative to axis A?
torque_by_MOTOR_on_A = -torque_by_A_on_MOTOR
torque_by_B_on_A = -torque_by_A_on_B

Otherwise there is also:

torque_by_GROUND_on_B = -torque_by_B_on_GROUND
 
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  • #47
alkaspeltzar said:
I agree with this, but what happens to the torque about B. Do we ignore it since it's not relative to axis A?
torque_by_MOTOR_on_A = -torque_by_A_on_MOTOR
torque_by_B_on_A = -torque_by_A_on_B

Otherwise there is also:

torque_by_GROUND_on_B = -torque_by_B_on_GROUND
I think I'm understand. I cannot compare torque at B since we have to maintain being consistent with A right? That's what I am looking to confirm.

So we look at torques about A and only A, everything balances correct?

Perok that's what I'm trying to get. I am really trying. Not trying to be pig headed
 
  • #48
alkaspeltzar said:
I have been asking where does the 50 inch lbs torque about B get balanced out.
What does "balancing out" have to do with N3L? It seems like you confusing N2L and N3L. Make sure you understand the difference between them for forces, before going into torques.
 
  • #49
A.T. said:
What does "balancing out" have to do with N3L? It seems like you confusing N2L and N3L. Make sure you understand the difference between them for forces, before going into torques.

What I am asking is where does the the 50inch lbs torque have its equal pair?

Below what you stated makes perfect snese. Not arguing this at all. But shouldn't there be an equal torque somewhere for the 50 inch lbs, and if no, why?If there are no horizontal forces between B and ground, it's still the same:

When taken around the same point:

torque_by_MOTOR_on_A = -torque_by_A_on_MOTOR
torque_by_B_on_A = -torque_by_A_on_B

Otherwise there is also:

torque_by_GROUND_on_B = -torque_by_B_on_GROUND
 
  • #50
alkaspeltzar said:
What I am asking is where does the the 50inch lbs torque have its equal pair?
Here:
torque_by_GROUND_on_B = -torque_by_A_on_B = 50
 
  • #51
russ_watters said:
Here:
torque_by_GROUND_on_B = -torque_by_A_on_B = 50

So the ground applies a horizontal force of 10lbs at the 5 inches about B. This is opposite and equal to the torque by A on B, about B. ANd if you consider gear B, these are the opposite and equal torques for it. Its like Gear A is now acting similar to the ground, and therefore the N3L balance.

Right?
 
  • #52
alkaspeltzar said:
So the ground applies a horizontal force of 10lbs at the 5 inches about B. This is opposite and equal to the torque by A on B, about B. ANd if you consider gear B, these are the opposite and equal torques for it. Its like Gear A is now acting similar to the ground, and therefore the N3L balance.

Right?
Sounds about right, yes.
 
  • #53
russ_watters said:
Sounds about right, yes.

THank you

I think i see what is going on here. In the end, torque is dependent on the point of rotation and everything about it, like summing the moments has to be done around the same axis. However, because of conservation of ang momentum, and N3L, it all has to balance one way or another.

This example probably was bad as i didn't start with good unknowns, but in the end i see it all. Makes me understand why in many cases we don't have to care about all the reactions because we identify our system to make life easier.

Thanks again
 
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  • #54
alkaspeltzar said:
So the ground applies a horizontal force of 10lbs at the 5 inches about B. This is opposite and equal to the torque by A on B, about B. ANd if you consider gear B, these are the opposite and equal torques for it. Its like Gear A is now acting similar to the ground, and therefore the N3L balance.

Right?
Wrong. The torque_by_A_on_B and the torque_by_GROUND_on_B are not a N3L pair. This is not N3L, but a N2L balance. You are still confusing the laws you are applying.
 
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  • #55
A.T. said:
Wrong. The torque_by_A_on_B and the torque_by_GROUND_on_B are not a N3L pair. This is not N3L, but a N2L balance. You are still confusing the laws you are applying.
Probably be clearer if you drew it out as I asked nicely but since I have tried and still getting it wrong I guess I just won't care. Your replys are short but leave a lot to be explained to someone trying to learn
 
  • #56
alkaspeltzar said:
Probably be clearer if you drew it out as I asked nicely ...
I have given you all the N3L pairs, for all your diagrams. Nowhere in there are torque_by_A_on_B and torque_by_GROUND_on_B a N3L pair.
 
  • #57
Dale said:
Yes, it does.

The point of N3 is the conservation of momentum. The point of the torque version is the conservation of angular momentum. Angular momentum requires the specification of one single axis about which all angular momenta are measured. That is just how angular momentum works.
Dale, can we talk or expalin where the n3l pair is for the torque B has on it? I get the point about being around a single axis, but do I just ignore what is happening to hear B
 
  • #58
A.T. said:
I have given you all the N3L pairs, for all your diagrams. Nowhere in there are torque_by_A_on_B and torque_by_GROUND_on_B a N3L pair.
I asked though what about gear B, do we just ignore the torque about B as it is around an axis not related to the problem?
 
  • #59
alkaspeltzar said:
Dale, can we talk or expalin where the n3l pair is for the torque B has on it? I get the point about being around a single axis, but do I just ignore what is happening to hear B
No, you don't ignore what is happening to gear B. You must include all torques on all objects in the system. But you must fix the axis of interest. Which axis do you want to know if there is torque about? Then you calculate all torques about that point.
 
  • #60
alkaspeltzar said:
I asked though what about gear B, do we just ignore the torque about B as it is around an axis not related to the problem?
"About B" makes no sense. Do you mean about the center of B? You can use any point, as long it's the same for both torques of an N3L pair.
 

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