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183_notes:angular_motivation [2021/05/08 18:46] – [Catching a Ball] stumptyl | 183_notes:angular_motivation [2021/05/31 15:47] (current) – [An Observation You Can't Fully Explain] stumptyl | ||
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{{youtube> | {{youtube> | ||
+ | //This video is primarily used for visual learning. No audio is within this demonstration video.// | ||
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- | This is an inelastic collision. You have read how to [[183_notes: | ||
- | | + | **This is an inelastic collision.** You have read how to [[183_notes: |
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Δ→psys=→FextΔt | Δ→psys=→FextΔt | ||
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With estimates of the velocity and mass of the ball as well as the collision time, you can determine the frictional force that the floor exerts on the stool. | With estimates of the velocity and mass of the ball as well as the collision time, you can determine the frictional force that the floor exerts on the stool. | ||
- | * The collision is inelastic, so the kinetic energy of this system is not conserved, which is fairly obvious. Initially the system has kinetic energy (the ball is moving) and in the final state it does not. The system' | + | * The collision is inelastic, so the kinetic energy of this system is not conserved, which is fairly obvious. Initially, the system has kinetic energy (the ball is moving) and in the final state, it does not. The system' |
ΔEsys=Wsurr+Q | ΔEsys=Wsurr+Q | ||
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{{youtube> | {{youtube> | ||
+ | //This video is primarily used for visual learning. No audio is within this demonstration video.// | ||
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Now, when the ball is caught, the person in the stool begins to rotate. There are a few other observations that you can make (depending on how much friction is in the bearings): | Now, when the ball is caught, the person in the stool begins to rotate. There are a few other observations that you can make (depending on how much friction is in the bearings): |