# The force of angular momentum

1. Apr 25, 2014

### bobie

We read everywhere that a spinning wheel, a gyroscope, offers resistence to change the plane of rotation.
Suppose a gyroscope has angular momentum L = 10 J*s:

What force F must we apply, what work W is needed to rotate the spinning plane by 2π?
- do we need to know only L or do we need to know r?
I suppose also:
- the work required is the same in every direction, and that
- the amount of work don is proportional to the angle of rotation, 90° = W/4
Is that correct?

2. Apr 25, 2014

### Simon Bridge

Hint: Conservation of angular momentum.

Note: if the system ends up in the same state it started in, without friction or other losses, then no net work was done on the system.

It is not as simple as applying a force to rotate the gyroscope - you need a constant torque to maintain the gyroscope at the new angle. Remove the force and the gyroscope falls back to it's original orientation.
So I think you need to do more reading on how rotating systems work so that you can refine your questions.
http://www.cleonis.nl/physics/phys256/gyroscope_physics.php
More generally:
http://faculty.ifmo.ru/butikov/Applets/Precession.html

3. Apr 25, 2014

### bobie

I couldn't watch the applet because I do not have Java, it seems really interesting, but,
Before I start getting deeper into the issue, please clarify these basic concepts:

- why is conservation relevant to this issue? we are not applying any torque to the spin , not changing the radius of the spinning wheel, right?, we are only changing the orientation of the spinning plane.
If we push the gyroscope in any direction (change its position) we must do the usual work (Ke) we would do if it were not spinning Ke = mv2/m
- if we tilt the gyroscope (changing its orientation) when it is not spinning, we must do some work w , if we repeat that while it is spinning, even if there were no extra resistence we must still do the work w, plus (if any) some extra resistence w1 caused offered by angular momentum L, for a total (w+w1) = W.
The fact that the gyroscope returns to the original position (that's amazing, is that in the applet ordo you know any video showing this phenomenon?) shouldn't affect that, the same as when we pull a spring, we do some work, even if the spring returns to the original position.
What is wrong in these beliefs?
Thanks a lot, Simon

Last edited: Apr 25, 2014
4. Apr 25, 2014

### BruceW

we are not applying torque to change the magnitude of angular momentum. But we are changing the direction of angular momentum. This still requires a torque. Angular momentum is a conserved vector, just like linear momentum. So it is not enough to just consider the magnitude of these vectors.

As an analogy to conservation of linear momentum, if we have an object moving in a circle at constant speed, the magnitude of linear momentum doesn't change, but the direction of linear momentum does change, so we still must supply a centripetal force to keep the object moving in a circle.

5. Apr 25, 2014

### bobie

So , I thought, a force/some work is needed to change the direction of the spinning plane. How do I calculate this force/work?

6. Apr 25, 2014

### jbriggs444

It takes no torque to maintain a gyroscope at a particular angle. It will not "fall back" to its original orientation. Conservation of angular momentum assures us that this is true.

The force applied to cause a gyroscope to precess to a new rotation plane is at right angles to the resulting deflection at the point of application. It requires no work.

7. Apr 25, 2014

### bobie

Why precess?
Suppose we have a flywheel weighing 1 ton with two . If I grab the axle and rotate it by 90° do I do work? If the wheel is spinning do I do the same amount of work or more? does the wheel precess?does it bounce back?

Thanks

Last edited: Apr 25, 2014
8. Apr 25, 2014

### jbriggs444

It is easier to demonstrate with a bicycle wheel rather than with a 1 ton flywheel.

Take an ordinary bicycle wheel, removed from the bicycle and give it a spin. Hold it by the axle, one end in your right hand and one in your left (with the treads of the tire spinning downward in the rough neighborhood of your nose).

Now push up with your left hand and down with your right. This applies a clockwise torque to the bicycle wheel. Over time, this will naturally impart clockwise angular momentum. In order to have a clockwise angular momentum, the spinning bicycle wheel will twist in your hands. The axle end in your left hand will twist toward you. The axle end in your right hand will twist away from you. The treads will be coming down somewhat to the right of your nose and you will be looking at a bicycle wheel which has turned so that its rotation is slightly clockwise.

This effect is called precession.

Note that you applied an upward force with your left hand. But the resulting movement was at right angles -- toward you. You applied a downward force with your right hand. But the resulting movement was at right angles -- away from you. In both cases, the force and the displacement were at right angles from one another. That means that no work was done.

If you stop applying the torque with your two hands, the bicycle wheel will keep spinning on its new axis. It will not "remember" its original orientation. It will not try to twist back to that orientation.

Last edited: Apr 25, 2014
9. Apr 25, 2014

### A.T.

To rotate the spin-axis (S) by 90° around an axis (R) you have to apply a net external torque around an axis (T), which is perpendicular to both S & R. The instantaneous net angular velocity vector (ω) is somewhere in the plane spanned by S & R. So the applied torque T and ω are perpendicular, and no work is done.

10. Apr 25, 2014

### bobie

That is what I am trying to say: I resist the twist and keep my left hand up and right hand down allowing the wheel to change only in that direction. Is it clear now?
What is the work I have done? I surely applied a force, didn't I?
The wheel will stay that way or if I release my force it will move in any direction?

Last edited: Apr 25, 2014
11. Apr 25, 2014

### bobie

You mean that if the wheel weighs 10 tons I can rotate it with my little finger? and the wheel (if there's no friction) will rotate at any speed with no effort on my side? I can make it rotate at 100 rps?

12. Apr 25, 2014

### jbriggs444

If you resist the twist then you are now pushing away with your left hand and pulling toward you with your right. This is a clockwise torque as viewed from above. The wheel will twist against this torque and will precess to obtain clockwise angular momentum as viewed from above.

The result is that the wheel will now precess in the direction you originally tried to get it to move. Your left hand will rise, your right hand will fall and the treads coming down near your nose will be moving diagonally downward from your upper right to your lower left.

But you did not need to lift up with your left hand and down with your right to make this happen. That force was irrelevant. What was relevant was the outward push from your left hand and the inward pull from your right. But those forces were at right angles to the upward movement of the axle end in your left hand and the downward movement of the axle end in your right. So no work was done.

13. Apr 25, 2014

### A.T.

Your effort has little to do with mechanical work done. Holding up a 100kg weight does no work, but it is quite an effort for a human.

14. Apr 25, 2014

### jbriggs444

You can rotate it through any angle you like with as little torque as you care to apply. Though it may take a long time.

The less torque you apply, the slower the rate of precession. If you want to precess a 10 ton wheel moving at 10,000 rps so that the axis of rotation itself rotates at 100 rps, that will take vastly more torque than you can apply with your little finger.

15. Apr 25, 2014

### bobie

I might do no work, but I am applying a force equal and opposite to gravity, right?
That's why I enquired aboutF/W, force/work.
If there is a 10 ton flywheel must I apply a force to make it rotate at 1 rps? and if I want it to rotate at 10 rps? Do you think I can make it rotate at 100 rps?
Now, whatever your answers, if that wheel is spinning does it make any difference?
That is what I would like to know
Thanks, everybody

Last edited: Apr 25, 2014
16. Apr 25, 2014

### bobie

I haven't been clear enough:
I lift my left hand, lower my right and resist any twist, precession, force .... etc....that oppose my move, in any direction, and leave it like that.
Even if you say there is no work done, what force do I exert? no force at all?

17. Apr 25, 2014

### Staff: Mentor

If you actually change the orientation of the spin, you're doing work because you're applying torque across an angle, and that does work just as applying a force across a distance does. Indeed, it's fairly easy to derive the formula for the work done by a torque from the the old classic $W=Fd$ (and I strongly suggest that you try doing that as an exercise).

But first you have to understand how torque relates to changes of the direction of spin as well as the rate of spin. That came up in your other angular momentum thread: https://www.physicsforums.com/showpost.php?p=4728955&postcount=14

18. Apr 25, 2014

### jbriggs444

Right.

But force and work are different things. Work is defined (in freshman physics) as the product of force applied time distance moved in the direction of the applied force.

Yes, whether it is spinning makes a difference.

If the flywheel is not spinning and if it has frictionless bearings, you can make it spin at any rate you like with as little force as you like. You just have to apply that force for a long enough time. It is actually a "torque" that you need to apply. Any force that is not applied right at the axis of rotation will have an associated torque.

If the flywheel is spinning and you want to change its axis of rotation then the situation is different. If the flywheel spin rate is much faster than the desired precession rate then the rules of gyroscopes in freshman physics apply. To a first approximation, the precession rate that you get is proportional to the applied torque and inversely proportional to the angular momentum that the gyroscope possesses by virtue of its spin rate.

The area that freshman physics does not cover is when the desired precession rate is not very small compared to the existing spin rate. As I understand it, you need tensors to deal properly with rotational mechanics in that regime.

Last edited: Apr 25, 2014
19. Apr 25, 2014

### jbriggs444

To a first approximation in the case of high spin rates and low precession rates, if you apply a torque, the resulting precession is at right angles to the applied torque. No work is done.

If the applied torque changes the rotation rate of the spin... then work is done.

20. Apr 25, 2014

### bobie

Now, that really baffles me:
suppose we have a wheel (m, r)on frictionless gimbals (http://en.wikipedia.org/wiki/File:Gyroscope_operation.gif)
If we want to spin the wheel on its plane xy, we must apply a force/ give it momentum/Ke/work which depends on the speed of rotation: rps/v/ω. If instead of the wheel we have two balls (m= .5 kg) at the ends of a diameter (1 m) , and v is 10 m/sec, then we know we must give the 'wheel' 50J of Ke and L is 25J*s
You are saying that I can rotate the same wheel on a normal plane , give it same speed and a roughly similar Ke, with almost no force applied?
Now suppose the wheel is spinning on its plane at 10/π rps, and we make it rotate at the same speed on a normal plane, what force have we applied, what is the Ke in that direction?

Now, coming back to my first question, suppose I grab the 2 golden axles (in the .gif) in my hands, rotate it by 90° in any direction and keep it like that,
- what work have I done?
- what happens if, after a while, I let go of them?

Thanks a lot for your Kind help

Last edited: Apr 25, 2014