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09 Precession (3b)

Aim

To show how a rotating wheel reacts to an applied torque.

Subjects

Diagram

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Figure 1:.

Equipment

Presentation

The bicycle wheel with handles is vertically mounted on a rotating platform in such a way that one handle is fixed in a hinged clamp and the other handle rests on a support (see diagram). The bicycle wheel is made fast spinning.

Now the rotating platform is slowly turned round by hand, trying both directions of rotation. In one direction of rotation, the spinning bicycle wheel will lift its free handle upwards from the support.

As soon as you stop speeding up the rotating platform, the lifting of the spinning bicycle wheel will stop also.

Leaving the spinning bicycle wheel to itself now, it slowly comes down, and the rotating platform speeds up.

Explanation

The spinning bicycle wheel has an angular momentum of I1ω0I_{1} \omega_{0}. Rotating the platform, introduces a torque TT. This torque tends to change I1ω0I_{1} \omega_{0}, so I1ωbI_{1} \omega_{b} moves into the direction of TT. So, when TT is pointing upward, I1ω0I_{1} \omega_{0} moves upward: the bicycle wheel handle lifts itself from the support. (See Figure 2a.)

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Figure 2:.

While the platform is freely rotating, gravitational torque mgsm g s is acting (see Figure 2b). In Figure 2b this torque is pointing out to the reader. I1ω0I_{1} \omega_{0} moves into the direction of mgsm g s, keeping the platform rotating (precession). In this process, increases because the bicyclewheel is coming down. Since ωp=mgsI0ω0,ωp\omega_{p}=\frac{m g s}{I_{0} \omega_{0}}, \omega_{p} increases due to ss becoming larger (and also a little due to ω0\omega_{0} becoming smaller).

Remarks

Sources