What is the relationship between T2 and T1 in torque propagation?

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    Propagation Torque
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Discussion Overview

The discussion revolves around the relationship between torque T1 and torque T2 in a system involving a horizontal rod and its associated forces and moments. Participants explore the implications of arm length, the application of torque, and the effects of deformation on the system. The conversation includes theoretical considerations and calculations related to torque propagation.

Discussion Character

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

Main Points Raised

  • Some participants question how T2 is influenced by T1 and suggest that the length of the arm on the right may be a critical factor.
  • Others argue that the way T1 is generated does not affect T2, as T1 could arise from various sources.
  • Several participants express uncertainty about the forces acting on the rod and the implications of deformation due to torque.
  • One participant proposes a theory involving angular acceleration and inertia, suggesting that both perspectives (left pivot and appendage) yield the same angular acceleration.
  • Another participant emphasizes the need for clarity on how torque T1 is applied to fully understand its relationship with T2.
  • Some calculations are presented, indicating that different arm lengths yield different results for T2, depending on how T1 is applied.
  • Participants discuss the rigidity of the joint and its impact on torque calculations, with some suggesting that the direction of the appendage arm may not matter.
  • One participant introduces the concept of gyroscopic couple reaction as a source of torque in their specific investigation.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between T1 and T2, the relevance of arm length, and the effects of torque application. The discussion remains unresolved, with no consensus reached on several key points.

Contextual Notes

Participants highlight the potential underspecification of the problem, noting that additional information about the application of torque T1 is necessary for a complete analysis. There are also discussions about the assumptions involved in calculations and the implications of deformation on the system.

24forChromium
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True or false.jpg

See image. If T_1 and L is known, what is T_2? (T_2 is caused by T_1)
 
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24forChromium said:
View attachment 88293
See image. If T_1 and L is known, what is T_2? (T_2 is caused by T_1)

Can you draw a free body diagram (FBD) for the horizontal rod?

And if the rod does not move, what can you say about the sum of the forces and moments on the rod?

What changes if the horizontal rod can deform due to the applied torque?
 
I think there may be a missing piece of information, which is the length of the arm on the right of the diagram.

According to my calculations, ##T_2## depends on ##\frac{h}{L}## where ##h## is the length of the arm.

But I'm not brilliant with torques, so that may be wrong.
 
andrewkirk said:
I think there may be a missing piece of information, which is the length of the arm on the right of the diagram.

I think it is irrelevant, because the arm length on the right will only effect the torque T_1 if T_1 is generated by forces acting on those arms, but T_1 could be generated in many other ways, and I don't think the way T_1 is generated matters to T_2.
 
berkeman said:
Can you draw a free body diagram (FBD) for the horizontal rod?

And if the rod does not move, what can you say about the sum of the forces and moments on the rod?

What changes if the horizontal rod can deform due to the applied torque?
I don't think I can, because I don't know what kind of forces will be acting on it if those forces are generated by a torque on the other end. The rod should move, but if you are asking about the moment in time where is hasn't beginning moving yet, then I would say the sum of the forces acting on the whole system is equal to the torque acting on the appendage, at least that would be what's logical to me. About deformation, I think that would just make things more complicated and I don't think I need that, because I am investigating a real case of such a system, I think the effect of the deformation would be unmeasureably small.
 
24forChromium said:
I don't think I can, because I don't know what kind of forces will be acting on it if those forces are generated by a torque on the other end. The rod should move, but if you are asking about the moment in time where is hasn't beginning moving yet, then I would say the sum of the forces acting on the whole system is equal to the torque acting on the appendage, at least that would be what's logical to me. About deformation, I think that would just make things more complicated and I don't think I need that, because I am investigating a real case of such a system, I think the effect of the deformation would be unmeasureably small.

Is only a torque applied to the left end of the horizontal arm? How is the torque applied?
 
My current theory goes like this:

Rotation is relative, seen from the left pivot, a torque is accelerating the appendage in the counterclockwise (C.C.) direction; seen from the fixed joint, a torque is acting around the fixed joint and accelerating the left pivot as well as the horizontal rod in the C.C. direction, even though this is not true when the fact that the left pivot is fixed on the ground when the ground is taken into consideration. However, the angualr acceleration perceived by both points should be the same in magnitude.

From the perspective of the left pivot, a torque is accelerating the system with an angualr inertia that is the sum of the angular inertia of the pivot itself and the angular inertia of the appendage at a radius of L away. Or: α = (I_pivot + I_appendage_L) /T

From the perspective of the appendage, a torque is accelerating the system with an angualr inertia that is the sum of the angular inertia of the appendage itself and the angular inertia of the body at a radius of L away. Or: α = (I_pivot_L + I_appendage) /T

Because α is the same for both, (I_pivot + I_appendage_L) /T = (I_pivot_L + I_appendage) /T
 
24forChromium said:
I think it is irrelevant, because the arm length on the right will only effect the torque T_1 if T_1 is generated by forces acting on those arms, but T_1 could be generated in many other ways, and I don't think the way T_1 is generated matters to T_2.
I think it does matter, because a torque needs to arise from a force applied to some body.

Consider the cases where the arm has length L from tip to square joint and where it has length 2L, and the torque ##T_1## arises from a force applied at one tip of the arm. According to my calcs we get different answers for ##T_2## in the two cases.
 
berkeman said:
Is only a torque applied to the left end of the horizontal arm? How is the torque applied?
yes, only a torque is applied on the left and it is applied by gyroscopic reaction in the case that I am investigating.
 
  • #10
andrewkirk said:
I think it does matter, because a torque needs to arise from a force applied to some body.

Consider the cases where the arm has length L from tip to square joint and where it has length 2L, and the torque ##T_1## arises from a force applied at one tip of the arm. According to my calcs we get different answers for ##T_2## in the two cases.
That sounds like it may be true, let's say the arm length on the appendage is D, can you show me how T_2 can be calculated?
 
  • #11
This is the way I'm thinking about it: Since the joint is rigid, it doesn't matter whether the arm points down as shown, or sideways as a continuation of the horizontal strut. The latter is easier to work with, so let's consider that. The torque T1 is equivalent to a force T1/D at the end of the arm. We then use the length D+L to convert that to a torque around the pivot.
 
  • #12
andrewkirk said:
This is the way I'm thinking about it: Since the joint is rigid, it doesn't matter whether the arm points down as shown, or sideways as a continuation of the horizontal strut. The latter is easier to work with, so let's consider that. The torque T1 is equivalent to a force T1/D at the end of the arm. We then use the length D+L to convert that to a torque around the pivot.
so, you are saying that T_2 = (T_1 / D) * (D + L) am I right?
 
  • #13
andrewkirk said:
This is the way I'm thinking about it: Since the joint is rigid, it doesn't matter whether the arm points down as shown, or sideways as a continuation of the horizontal strut. The latter is easier to work with, so let's consider that. The torque T1 is equivalent to a force T1/D at the end of the arm. We then use the length D+L to convert that to a torque around the pivot.
I don't believe that's right, if the direction of the appendage arm does not matter and the force is always tangential to the right joint, then it should be equally correct to have the arm pointing to the left, overlapping parts of the body, and have a force point down from the arm and accelerating the whole system clockwise, which is the opposite of what happens.
 
  • #14
24forChromium said:
I don't believe that's right, if the direction of the appendage arm does not matter and the force is always tangential to the right joint, then it should be equally correct to have the arm pointing to the left, overlapping parts of the body, and have a force point down from the arm and accelerating the whole system clockwise, which is the opposite of what happens.
Good point. I hadn't thought of that. Oh well, there goes that theory.

This nudges me towards the view that the problem is underspecified. We need to know how or where (or both) the torque T1 is applied.
 
  • #15
There are a lot of possibilities, in my specific investigation, the torque T1 is produced by a phenomenon known as (at least I call it) Gyroscopic couple reaction. It's super complicated, by essentially it says that if a gyroscope is spinning and precessing at the same time, the gyroscope will generate a torque in a direction that is perpendicular to both of those rotations, the equation is T = ω*L. I still don't believe that the way a torque is applied matters, I still think that the variable arm length can be compensated by variable tangential force, but if you like, we can put numbers into all of those variables.
Here is the numbers in my experiment:
Body length - L: 0.6m
arm length - D (in this case the radius of the disk): 0.3m
torque - T1 (at one point in time): 75N*m
 
  • #16
It is not possible to calculate given the information provided. You need to know the motion of the structure (especially angular acceleration, but maybe also angular velocity). Then you can solve for the unknown torque.

Also, are you assuming the rod is massless and rigid?
 
Last edited:
  • #17
DaleSpam said:
It is not possible to calculate given the information provided. You need to know the motion of the structure (especially angular acceleration, but maybe also angular velocity). Then you can solve for the unknown torque.

Also, are you assuming the rod is massless and rigid?
You can add one such variable if you wish, then express T2 in terms of the other variables.
 

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