Where's the torque when you retract your arms on a spinning chair?

[DocZaius]

If you spin on a chair with your arms and legs out and then pull them in, your rotation accelerates. What torque is responsible for that acceleration? It seems to me all the movement is towards the axis of rotation and should not be responsible for any torque. In fact, take an idealized body that can reduce its radius with movements entirely towards the axis of rotation. Where does the torque come from?

I know that the moment of inertia has changed, and from that point of view it makes sense that the angular velocity would increase. I was just trying to look at it from a free body diagram perspective.

 

[rcgldr]

The path that your arms take when being retracted is a inwards spiral. Part of that force is in the direction of travel of that spiral path, so the speed of your arms increases. In order to keep your arms orientation constant relative to yourself and the chair, you need to apply a torque, coexistant with an equal and opposing torque from your arms that increases your rate of rotation. Image of an example spiral path showing the line perpendicular to the path, and the radial line that is not perpendicular to the path.

 

[DocZaius]

Thank you very much!

 

[Cleonis]

If you spin on a chair with your arms and legs out and then pull them in, your rotation accelerates. What torque is responsible for that acceleration?

As Jeff reid points out with his diagram:
The trajectory of your feet and fists is an inward spiral. The general case is contraction of a rotating system. At each point in time a rotating system will contract when the actual centripetal force is larger than the required centripetal force. Over the course of the contraction the centripetal force is doing https://www.physicsforums.com/library.php?do=view_item&itemid=75".

If a trajectory is circular then the centripetal force is not doing work. When the trajectory is a spiral then the work that is being done is causing rotational acceleration.

Peculiarly, quite a few authors write statements such as: "The person on the chair starts rotating faster because his moment of inertia decreases." I believe that line of reasoning violates causality. The causal factor is the centripetal force. During contraction the centripetal force causes angular acceleration. The contracted system has a smaller moment of inertia.

Cleonis

 

[rcgldr]

The centripetal force only does work when there's a component of force in the direction of the spiral path. In the case of a object pulled by a string that wraps around a post, the path is an involute of circle, and no work is done because the force is always perpendicular to the spiral path. Angular momentum doesn't appear to be conserved, until you take into account that a torque force is applied to the post, imparting a angular acceleration to whatever the post is attached to (like the earth, in which case the angular acceleration is tiny), in which case angular momentum is conserved again when you include whatever the post is attached to as part of a closed system.

 

[diazona]

If you spin on a chair with your arms and legs out and then pull them in, your rotation accelerates. What torque is responsible for that acceleration? It seems to me all the movement is towards the axis of rotation and should not be responsible for any torque. In fact, take an idealized body that can reduce its radius with movements entirely towards the axis of rotation. Where does the torque come from?

I know that the moment of inertia has changed, and from that point of view it makes sense that the angular velocity would increase. I was just trying to look at it from a free body diagram perspective.

There is no torque, in the ideal case. As the idealized body reduces its radius, its moment of inertia decreases and you would observe its angular velocity \vec{\omega} increasing in such a way as to keep the angular momentum \vec{L} = \mathbf{I}\vec{\omega} constant. And since
\vec{\tau} = \frac{\mathrm{d}\vec{L}}{\mathrm{d}t}
if the angular momentum stays constant, there is no torque.

There would, of course, be internal forces involved. But the moments of all those forces about the axis of rotation would cancel out, so that the net torque involved is zero.

 

[Cleonis]

In the case of a object pulled by a string that wraps around a post, the path is an involute of circle, and no work is done because the force is always perpendicular to the spiral path.

Indeed you point out an important difference.

The simplest case is a circumnavigating mass subject to pull from a massless cord, causing it to spiral inward. If the force is at all times a central force then:
- The centripetal force is doing work
- Angular momentum of the circumnavigating object is conserved.
- As the rotating system contracts the tangential velocity increases all the time.

In the case of the cord wrapping around a post:
- Pull of the cord on the object is at all times perpendicular to the velocity: the force is not doing work.
- Angular momentum of the circumnavigating object is not conserved
- The tangential velocity stays the same.


Cleonis

 

[D H]

f a trajectory is circular then the centripetal force is not doing work. When the trajectory is a spiral then the work that is being done is causing rotational acceleration.

No.

Peculiarly, quite a few authors write statements such as: "The person on the chair starts rotating faster because his moment of inertia decreases." I believe that line of reasoning violates causality.

Quite a few authors say that because they are correct.

Can you lift yourself by your bootstraps? No. The reason is because pulling on your bootstraps is an internal force. An external force is required to change your momentum. Similarly, an external torque is required to change your angular momentum. In the ideal case, a person on a frictionless spinning chair, flailing ones arms about (or pulling them in) does not result in an external torque.

Look at the rotational equation of motion:

\frac{D\vec L}{dt} = \frac{d}{dt}\left(\mathbf I \vec {\omega}\right) = \vec{\tau}

No torque is required to change the angular velocity. In fact, if there is zero torque (as it is in the ideal case), angular velocity *must* increase to keep the angular momentum constant when the moment of inertia is decreasing.

The causal factor is the centripetal force.

A causal factor is indeed needed to change the moment of inertia. Work is being done here! However, it is mistaken to think of this as necessitating a torque. Torque is change in angular momentum, not angular velocity. The kinetic energy of the system is

T = \frac 1 2 \left(\vec L \cdot \vec {\omega}\right)

Differentiating wrt time,

\frac {dT}{dt} = \frac 1 2<br /> \left(\frac{d\vec L}{dt}\cdot \vec{\omega}<br /> + \vec L \cdot \frac{d\vec{\omega}}{dt}\right)

With no external torque, this reduces to

\frac {dT}{dt} = \frac 1 2 \vec L \cdot \frac{d\vec{\omega}}{dt}


In the simple freshman physics case of rotation about an eigenaxis of the system, angular momentum is parallel to angular velocity and angular acceleration. The above vector equations become scalar equations.

\aligned<br /> \dot{\omega} &amp;= -\,\frac{\dot I}{I} \omega \\<br /> \dot T &amp;= \frac 1 2 \dot I \omega^2<br /> \endaligned

Work must be being done to accomplish that increase in kinetic energy. Just because work is being done does not mean that a torque must exist.

 

[rcgldr]

torque

In this particular case, internal torques are required to increase the angular momentum of the persons body and chair that are not moving "inwards", and to decrease the angular momentum of the arms and hands that are moving "inwards". The overall angular momentum of this system is preserved, but the components of this system experience internal torques and changes in angular momentum.

 

[D H]

Let's reduce this to the simplest case, Jeff. Consider a massless rod rotating about its axis. The ends of the rod are connected to some massive structure via frictionless couplings. Two point masses are connected to the rod by equal length flexible massless strings. The strings are connected to the rod via a pair of tiny frictionless pulleys. A motor controls the length of the strings. The entire system is in empty space; no gravity.

The rod+masses subsystem is set into rotation and the masses are slowly pulled toward the rod. There is no external torque on this subsystem. Because the forces needed to draw the masses inward are purely radial, there are no internal torques, either. Yet the angular velocity still increases.

 

[rcgldr]

Let's reduce this to the simplest case, Jeff. Consider a massless rod rotating about its axis. The rod+masses subsystem is set into rotation and the masses are slowly pulled toward the rod. Because the forces needed to draw the masses inward are purely radial, there are no internal torques, either. Yet the angular velocity still increases.

I agree, I was only pointing out the case where the rod is not massless, with the analogy of the person and chair being the rod with mass. The first diagram I posted would be similar to the case of the massless rod, all of the mass is in the moving object, and I'm assuming a massless string.

 

[Cleonis]

Peculiarly, quite a few authors write statements such as: "The person on the chair starts rotating faster because his moment of inertia decreases." I believe that line of reasoning violates causality.

In the ideal case, a person on a frictionless spinning chair, flailing ones arms about (or pulling them in) does not result in an external torque.

Obviously I agree there is no external torque.
In my replies in this thread I have not mentioned torque; your disagreement is not with me.

As Jeff Reid points out, in the case of a person on a swiveling chair you can opt to track the torso and the limbs separately, and then there are internal torques to evaluate.

Cleonis

 

[D H]

I agree, I was only pointing out the case where the rod is not massless, with the analogy of the person and chair being the rod with mass. The first diagram I posted would be similar to the case of the massless rod, all of the mass is in the moving object, and I'm assuming a massless string.

Whether the rod is massless is irrelevant. It just makes the calculation of the inertia tensor a bit simpler. Let's go back to that post.

The path that your arms take when being retracted is a inwards spiral. Part of that force is in the direction of travel of that spiral path, so the speed of your arms increases.

This does not necessarily mean a torque is exerted. Think of it in terms of a comet orbiting the Sun. Comets have highly elliptical orbits. The force is only normal to the ellipse at the apsides. Yet there is no torque on the comet. Gravitation is a central force.

Image of an example spiral path showing the line perpendicular to the path, and the radial line that is not perpendicular to the path.

Torque is \vec r \times \vec F. It has nothing to do per se with velocity, which (locally) defines the path being followed.

The centripetal force only does work when there's a component of force in the direction of the spiral path.

This is correct. Work is a different concept than torque. Work must be performed to decrease the moment of inertia of a constant mass spinning object. Just because work is being performed does not mean a torque is being applied.

 

[blitz.km]

Peculiarly, quite a few authors write statements such as: "The person on the chair starts rotating faster because his moment of inertia decreases." I believe that line of reasoning violates causality. The causal factor is the centripetal force. During contraction the centripetal force causes angular acceleration. The contracted system has a smaller moment of inertia.

Cleonis

I am sure I can justify what many authors write.

The angular momentum can be conserved because we do not have any external force on the system.

Angular momentum= I.w
I: Moment of inertia
w: Angular velocity

As the person folds his hands, the moment of inertia decreases.. because now more mass is concentrated near the axis of rotation.
As the angular momentum has to remain constant, the angular velocity increases.

 

[Cleonis]

As the angular momentum has to remain constant, the angular velocity increases.

My perspective is tracing causality.
My demand is that the sequence must be tracable from cause to effect.

Now, in the case of reasoning like "the angular momentum has to remain constant", the metaphor is vague. What is the cause?

Of course the calculation that is based on conservation of angular momentum will produce the correct result. But the original poster is asking why the person in the chair starts spinning faster. The request is to help understand.

Instead of using conservation of angular momentum you can calculate the increase in angular velocity by evaluating how much work the centripetal force is doing. By looking at the direction of velocity and the direction of force one gets a visceral understanding of what physics is taking place.

 

[D H]

Why is the concept of work, which does not work without the concept of conservation of energy, more fundamental than conservation of angular momentum?

 

[Cleonis]

Why is the concept of work, which does not work without the concept of conservation of energy, more fundamental than conservation of angular momentum?

I have made no statements about one principle being "more fundamental" than another; your disagreement is not with me.

Work deals with energy conversion; as a force is causing acceleration one form of energy is converted to another form. Work is associated with proceeding in time from cause to effect. Conservation of angular momentum on the other hand, is strongly associated with spatial symmetry.

In the end it all converges: it is possible to derive conservation of angular momentum from the work/energy-theorem, but in doing so one of the postulates is symmetry of the laws of dynamics for all oriëntations in space.

 

[DocZaius]

I think that the reason I have trouble understanding how this system could have had an angular acceleration applied to it without an external torque is that this corresponding situation is different in the linear case.

It seems that linearly, a mass cannot simply change its value as the moment of inertia does here. If it does, it does so by ejecting matter and we treat the resulting bodies seperately (but we remember they were together when considering conservation of linear momentum).

So linearly, if I see the whole body having undergone linear acceleration, it is safe to say that an external force was applied to it, while rotationally that is not necessarily the case (the whole body could have changed its moment of inertia entirely internally (say that 3 times fast)).

Let me know if/how I am wrong!

 

[blitz.km]

Now, in the case of reasoning like "the angular momentum has to remain constant", the metaphor is vague. What is the cause?

Well, can you explain this:
"An object would have constant linear momentum until we apply an external force on it."
Even this must be vague, because according to you we can not apply this to solve any query.

 

[A.T.]

Work deals with energy conversion; as a force is causing acceleration one form of energy is converted to another form. Work is associated with proceeding in time from cause to effect. Conservation of angular momentum on the other hand, is strongly associated with spatial symmetry.

I still don't get why a force is a better "cause" than conservation of angular momentum.

Both are just assumptions based on experience. We assume that there is a force, if we see acceleration. And we assume that angular momentum is conserved. Isn't it just that we are more used to say "a force caused something"?

 

[Cleonis]

I still don't get why a force is a better "cause" than conservation of angular momentum.

Both are just assumptions based on experience. We assume that there is a force, if we see acceleration. And we assume that angular momentum is conserved. Isn't it just that we are more used to say "a force caused something"?

Linear momentum is the product of two input factors, inertial mass and velocity. Angular momentum is the product of three input factors, inertial mass, velocity and radial distance.

In a geometrical representation:
Linear momentum is proportional to a line: in the absence of a force an object in motion covers equal distances in equal intervals of time.
Angular momentum is proportional to an area: in the absence of a torque the trajectory of an object sweeps out equal areas in equal intervals of time.

Compared to linear momentum angular momentum is a compound entity.

That said, it's only in Newtonian dynamics that the distinction is clear. I'm aware that in relativistic physics and quantum physics it's a different story.

 

[Andy Resnick]

If you spin on a chair with your arms and legs out and then pull them in, your rotation accelerates. What torque is responsible for that acceleration? It seems to me all the movement is towards the axis of rotation and should not be responsible for any torque. In fact, take an idealized body that can reduce its radius with movements entirely towards the axis of rotation. Where does the torque come from?

I know that the moment of inertia has changed, and from that point of view it makes sense that the angular velocity would increase. I was just trying to look at it from a free body diagram perspective.

This is a tricky problem; more tricky than it appears. The Feynman Lectures discusses this in section 19-8. As it turns out, the 'missing' force is the Coriolus force.

 

[A.T.]

This is a tricky problem; more tricky than it appears. The Feynman Lectures discusses this in section 19-8. As it turns out, the 'missing' force is the Coriolis force.

The Coriolis force can be blamed in frame that initially co-rotates with you. But in the inertial frame there is only the centripetal force.

 

[Andy Resnick]

Rotating frames are not inertial frames.

 

[Cleonis]

This is a tricky problem; more tricky than it appears. The Feynman Lectures discusses this in section 19-8. As it turns out, the 'missing' force is the Coriolus force.

Working with a centrifugal term and a Coriolis term in the equation of motion is useful in the following kind of setup: A overall system that is rotating at a constant angular velocity, with a particular object (or multiple objects) having a velocity relativity to that system.

Now the case of a person on a swivel chair, rotating, retracting arms and legs. Then there is no overall system with a constant angular velocity. There just the one chair and the angular acceleration of that chair


Now, in engineering the expression 'Coriolis effect' has the following meaning: If you have a rotating part, and it moves closer to the axis of rotation, then it's angular velocity will increase. For instance, helicopter blades bend up all the time, and bending up moves the mass closer to the axis of rotation. You can get buildup of catastrophic vibration. Another example is the operating principle of a Coriolis flow meter.

In the past decades in physics the meaning of the word 'Coriolis' has shifted. It used to be the same meaning as in engineering, but it has moved away from that. What Feynman is referring to is the engineers definition of Coriolis effect.

The work of Gustave Gaspard Coriolis dealt with engineering. Coriolis was the one who introduced the concept of mechanical work. Coriolis was interested in the question of how much usable energy can be obtained from a waterwheel, that was the kind of rotation he was interested in. It was through engineering that the expression 'Coriolis effect' first entered science.

 

[A.T.]

Rotating frames are not inertial frames.

Exactly. And the Coriolis force exists only in rotating frames but not in in inertial frames. If you want to explain something from an inertial frame, you cannot use the Coriolis force.

Now the case of a person on a swivel chair, rotating, retracting arms and legs. Then there is no overall system with a constant angular velocity. There just the one chair and the angular acceleration of that chair

You can still define a rotating frame of reference, that has a constant angular velocity equal to the chair's initial angular velocity. So initially the chair is at rest in that frame, and then when the masses start moving radially they are accelerated tangentially by the Coriolis force.

What Feynman is referring to is the engineers definition of Coriolis effect.

Is this text available online?

 

[DocZaius]

So just to make sure that what I took from this thread is right...let me know if the following statement is correct.

"Linearly, a system cannot increase the velocity of its center of mass entirely through internal forces. However, rotationally a system can increase the angular velocity of its center of mass entirely through internal forces."

I realize using center of mass for the angular velocity case might be unescessary but I wanted to be explicit.