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02 Boomerang Ball (1)

Aim

To explain the very peculiar behavior of a bouncing superball.

Subjects

Diagram

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Figure 1:.

Equipment

Safety

Presentation

The superball is thrown under the table as shown in the Diagram. Surprisingly it bounces back to the pitcher! How is this possible?

Explanation

As an introduction to an explanation a basketball is rolled over the floor, hitting the wall and rolling back to you. But in this rolling back it is also bouncing up and down. Confronting your students with the question “where originates this vertical momentum?” will lead them (I hope) to the answer: “the impulse of the friction force while the ball touches the vertical wall”.

As a second introduction to an explanation the basketball is thrown as shown in Figure 2A.

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Figure 2:.

(Also see the demonstration [“Throwing a basketball”](../1K1005 Throwing a Basketball/1K1005.md)). The ball is thrown without rotation, but after bouncing it rotates (the lines on the basketball make this rotation very well visible). The cause for this rotation is the torque M\vec{M}, due to the friction force Fr:(M=r×Fr)\vec{F}_{r}:\left(\vec{M}=\vec{r} \times \vec{F}_{r}\right) (see Figure 2B). Fr\vec{F}_{r}, that acts during a certain time Δt\Delta t, also causes a decrease of the momentum ( Δph)\left.\Delta p_{h}\right) in the horizontal direction of the moving ball ( Δph=0ΔtFRdt\Delta \stackrel{\rightharpoonup}{p}_{h}=\int_{0}^{\Delta t} \vec{F}_{R} d t ). The result is that, after hitting the floor, the ball not only rotates but also rises at a steeper angle than it had in its approach. (See Figure 2C; pvp_{v} only reverses its direction and does not change its magnitude; suppose the bounce completely elastic). Figure 3 shows the ball on hitting the bottom-side of the table-top. Observing the movement of the ball’s surface with respect to the bottom-side of the tabletop makes clear that the friction force is (again) directed to the left.

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Figure 3:.

Due to this horizontal impulse, php_{h} even changes direction and bouncing from the bottom side, the ball even moves to the left. (The clockwise rotation will be slowed down, stopped or even reversed, because on hitting the bottom-side of the tabletop Mˉ\bar{M} is directed in the opposite direction.)

Depending on the value of php_{h} now, CD in Figure 3 could be a possible line of movement. Explaining line DE (towards the pitcher) will be easy when you suppose a counterclockwise rotation in the path CD, because then the friction force on hitting the floor is directed again to the left increasing the horizontal component of the ball’s velocity to the left! (see Figure 3B)

Remarks

Sources