Ye Olde Acceleration: Angular Speed, Deceleration, & More

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Discussion Overview

The discussion revolves around the dynamics of a ball being spun on a string by a motor, focusing on concepts of angular speed, angular acceleration, and the transition to free fall when the motor is turned off. Participants explore the effects of centripetal force, gravitational force, and the implications of different environments, such as space.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant asserts that while a motor spins a ball at constant speed, there is centripetal acceleration but no angular acceleration.
  • Another participant agrees and adds that turning off the motor results in negative angular acceleration, leading to deceleration of the ball.
  • Concerns are raised about the conditions under which the ball will begin to fall, with one participant suggesting that friction will reduce the ball's speed immediately.
  • A participant introduces a scenario in microgravity, proposing that the ball would wind up around the shaft instead of falling, depending on its properties.
  • Another participant questions the immediate effect of turning off the motor, referencing centripetal force and its relationship to gravitational force, and seeks a method to calculate the time until the centripetal force is less than gravitational force.
  • One participant compares the situation to a ball rolling inside a hemisphere, suggesting a connection between speed and height, and prompts further exploration of the relevant formula.

Areas of Agreement / Disagreement

Participants express differing views on the immediate effects of turning off the motor and the conditions under which the ball will fall. There is no consensus on the calculations needed to determine the timing of the transition from centripetal to gravitational dominance.

Contextual Notes

Participants reference various forces and conditions without resolving the mathematical relationships or assumptions involved in their claims. The discussion remains open to interpretation and further exploration.

Who May Find This Useful

Individuals interested in dynamics, angular motion, and the effects of forces in different environments may find this discussion relevant.

a.mlw.walker
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hi,

if a motor spins a ball on a string round and round and a constant speed, there is an acceleration towards the centre, but no angular acceleration, just angular speed right?

but if you now turn the motor off, the balls angular acceleration will now go negative, and the ball will decelerate. at what point does the ball fall. how do you calculate how long it will take and at what speed the ball will fall at? because this is separate from its centrepetal acc yes?
 
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Hi a.mlw.walker! :smile:
a.mlw.walker said:
if a motor spins a ball on a string round and round and a constant speed, there is an acceleration towards the centre, but no angular acceleration, just angular speed right?

Yes!
but if you now turn the motor off, the balls angular acceleration will now go negative, and the ball will decelerate. at what point does the ball fall. how do you calculate how long it will take and at what speed the ball will fall at? because this is separate from its centrepetal acc yes?

Friction will gradually reduce the speed of the ball, and therefore its angular velocity (as you say, the angular acceleration will now go negative), and this will start immediately.

What is supporting the ball (apart from the string)? If nothing is, then the ball will immediately start to go lower (on the surface of an imaginary sphere). But it won't actually "fall". :smile:
 
If this were to be done in space, though, with no air and microgravity, the effect would be different. In that case, stopping the motor would just cause the tether line to wind up around the shaft and draw the ball in until it hit centre. Then, depending upon the properties of the ball, it would possibly rebound and unwind just to wind up again in the opposite direction. Eventually, the losses due to collision with the centre would overcome the ability to unwind again.
At least, I think that's how it would go.
 
well, yeah ok fine i didnt mention it for the example but if you want, the shaft has an arm on it and the string is attached to that so it can't "wind up"...

are you sure that effect is happening immediately, because with centrepetal force f=mv*v)/r

when this force gets below the force gravity has on the ball then the ball will begin to spiral down - but its only spiraling down because of a forward momentum, until the point where centreptal force is lower than the gravitational force, it will continue to spin on the same radius.

my question is how to work out how long after you turn the motor off, to when centreptal force is lower than gravitational force... it must be to do with the angular accelration but can't work out how to do it...
 
a.mlw.walker said:
… are you sure that effect is happening immediately, because with centrepetal force f=mv²)/r ...

Hi a.mlw.walker! :smile:

(copy the ², and anything else you want, for future use)

This is exactly the same as a ball rolling round the inside of a hemisphere.

Its height depends precisely on its speed.

Reduce the speed slightly, and that must reduce the height slightly … it does happen immediately.

So … on a sphere … what do you think is the formula connecting the speed with the height? :smile:
 

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