Question regarding centripetal force

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Discussion Overview

The discussion revolves around the physics of centripetal force as experienced on a ride like the Gravitron, particularly focusing on the motion of a rider if the walls of the ride were to suddenly disappear. Participants explore the implications of forces and momentum in circular motion.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant describes the centripetal force exerted by the ride's walls and questions why, if that force is present, they would not move directly away from the center if the walls disappeared.
  • Another participant clarifies that if the wall disappears, the force goes to zero, leaving the rider's linear momentum, which is tangent to the circular path, dictating their motion.
  • A different viewpoint emphasizes that while a rider is pushed inward by the wall, their momentum is tangential, and they will continue in that direction once the force is removed.
  • Some participants argue about the interpretation of being 'flung outwards,' suggesting that while the path may appear radial, it is influenced by the rider's tangential momentum.
  • One participant introduces the concept of reference frames, explaining that from the rotating ride's perspective, the rider drops radially outward, while from a ground observer's perspective, the motion is tangential.
  • Another participant reiterates the conservation of both linear and angular momentum, noting that the moment arm for momentum calculations remains relevant regardless of the rider's distance from the center.
  • There is a discussion about the angular difference between radial and tangential lines at the point of release, highlighting the complexity of interpreting motion in this scenario.

Areas of Agreement / Disagreement

Participants express differing views on the nature of motion after the walls disappear, with some emphasizing tangential motion and others discussing radial aspects. The discussion remains unresolved, with multiple competing interpretations present.

Contextual Notes

Participants reference concepts such as linear and angular momentum, centripetal force, and the effects of different reference frames, but the discussion does not resolve the implications of these concepts in the context of the ride.

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Hi just have a basic question. Just went to the local fair yesterday and road the Gravitron ride. The ride that sucks you to the walls. I became curious on the physics that cause you to get stuck to the wall so I have been researching centripetal force. Now it seems that the seats are exerting a force on me directly towards the center of a circle. I also understand that if hypothetically all of a sudden the walls disappeared on the ride I would move perpendicular to the force (tangental to the point on the circle). To me this makes little sense as I always thought I would move in a straight line directly in the opposite direction of the center of the circle. IF you have a force pushing you towards the center wouldn't that mean you would fly away from the center in a straight line assuming the walls suddenly disappeared. Please clarify this? Thank you.
 
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If the wall behind you suddenly disappears, then the force it is exerting on you goes to zero as well. That leaves you with the linear momentum (and angular momentum) that you had just before the wall disappeared. That linear momentum was tangent to the circular path you were traveling, so that is the direction you will fly off the (disintegrated) ride. There will likely be a rough landing!
 
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A basic law of motion is that you will move in a straight line if there are no forces on you. While you are in the ride, you feel the force on your back pushing you in radially, but your momentum is sideways (tangential). Momentum is conserved--force is not. When the walls disappear, it doesn't matter where the force used to be. It matters what your current momentum is. You will continue that trajectory until you hit something.
 
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People love to state that you are not 'flung outwards' in such circumstances. But it is not totally untrue because your path takes you ever further from the centre of rotation and, as the distance increases, the path becomes more an more approximately radial `(at least parallel to a radius).
 
There is a sense in which you do, in fact, fly directly away from the center of the ride. It's all about reference frames.

Suppose that instead of the wall completely disappearing, a hatch opens up that is big enough for you to fall through. From the point of view of the rotating ride, you will begin to drop radially outward. If you switch to the ground point of view, both you and the hatch will be moving tangentially. The hatch will accelerate radially inward away from you. Both descriptions are correct. You could continue to look straight through the hatch and see the hub of the ride. At least for a moment or two.

If you continue to maintain the viewpoint of the rotating ride, your trajectory would begin to be curved by Coriolis force, receding backwards compared to the rotating ride. If you continue to maintain the viewpoint of a ground observer, the hatch, of course, does not accelerate in a straight line but continues its circular motion while you move in a straight line. Both descriptions are correct. Either way you would lose sight of the hub of the ride. Your position would no longer fall on a line drawn radially outward from hub through hatch.
 
sophiecentaur said:
People love to state that you are not 'flung outwards' in such circumstances. But it is not totally untrue because your path takes you ever further from the centre of rotation and, as the distance increases, the path becomes more an more approximately radial `(at least parallel to a radius).

I think that this misses the point in that both linear and angular momentum are conserved, and the relevant moment arm for the "moment of momentum" calculation remains the radius of the rid, no matter how far the rider is thrown.
 
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Dr.D said:
I think that this misses the point in that both linear and angular momentum are conserved, and the relevant moment arm for the "moment of momentum" calculation remains the radius of the rid, no matter how far the rider is thrown.
I agree. But the difference becomes less and less - if you are considering the angle between the radial line to the projectile and the tangential line. The emphasis always seems to be in the effect at the point of release, where that anglular difference is 90 degrees and that really does conflict with what we often experience.
 

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