Why does rotating a ball on a string faster makes it horizontal

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Discussion Overview

The discussion centers on the dynamics of a ball being rotated on a string and the observed phenomenon of the ball's orientation becoming more horizontal as its speed increases. Participants explore the forces involved, including tension, gravity, and the concept of centrifugal force, while examining the implications of angular velocity on the system's behavior.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that as the speed of the ball increases, it appears to become more horizontal, questioning the role of centripetal and centrifugal forces.
  • Another participant clarifies that centrifugal force is not present in this context, emphasizing that the tension in the string has both radial and vertical components, with gravity acting only vertically.
  • It is proposed that the vertical component of tension must equal the gravitational force, while the horizontal component provides the necessary centripetal force, leading to a more horizontal orientation of the string as speed increases.
  • A participant checks their understanding of the forces involved, expressing confusion about how increasing angular velocity affects the angle of the string and the tension required to counteract gravity.
  • Another participant agrees that if the angle increases, the vertical component of tension would decrease, suggesting that infinite tension would be required to reach a 90-degree angle.
  • There is a discussion about the nature of centrifugal force, with one participant asserting it is an apparent force due to inertia, while another explains that it is not relevant for an observer not rotating with the ball.

Areas of Agreement / Disagreement

Participants express differing views on the existence and relevance of centrifugal force, with some arguing it is merely an apparent force while others question its absence in the analysis. The discussion remains unresolved regarding the implications of increasing angular velocity on the system's dynamics.

Contextual Notes

Participants reference the need for a balance of forces and the implications of changing angular velocity on tension and angle, but do not resolve the mathematical relationships or assumptions underlying these dynamics.

musik132
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Hi suppose i had a ball on string and started to rotate it in a circle around my hand. When i increase the speed of the ball it becomes more and more horizontal.
The only forces i can think of at play is centripetal and centrifugal forces and the force exerted by my hand and gravity. Is somehow the centripetal force's vertical component greater than the centrifugal's or is it something else?
 
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Actually - as you are looking at it, there is no centrifugal force.
There is the tension in the string which has radial and vertical components, and gravity, which is only vertical.

The vertical component of the tension has to be equal to gravity.
The horizontal component has to be the centripetal force.
The centripetal force is related to the angular velocity of the ball ... so what is happening is that to go faster the ball need more centripetal force - but only the same lift against gravity to hold it up. Since both these forces come from the same place (the tension in the string) then the string gets more horizontal.

It can never get completely horizontal though.--------------------
From the POV of an ant-physicist on the ball, there is a gravity force pointing down and a centrifugal force pointing horizontally to it. There is also a tension force in the string which exactly balances the other two. The the string were at 45deg then the centrifugal force would be equal to the gravity force ... the faster the ball goes, the bigger the centrifugal force and so the bigger the horizontal component of the tension has to be to balance it... so the angle has to be less than 45deg.
 
Last edited:
so just to check my thinking:
Ft = tension Fg = gravity Fc = centripetal
Ftcosθ = Fg and Fc=mrω^2=Ftsinθ
If ω increases the angle must go up but if the angle goes up doesn't Ftcosθ become less which would mean an increase in tension in order to counteract gravity? So an increase in ω changes both Ft and sinθ

and why isn't there a centrifugal force?
there is a "apparent outward force that draws a rotating body away from the center of rotation. It is caused by the inertia of the body as the body's path is continually redirected" wikipedia
 
musik132 said:
If ω increases the angle must go up but if the angle goes up doesn't Ftcosθ become less which would mean an increase in tension in order to counteract gravity?

Indeed. To reach 90 degrees ω and the tension would need to be infinite.
 
musik132 said:
and why isn't there a centrifugal force?
there is a "apparent outward force that draws a rotating body away from the center of rotation. It is caused by the inertia of the body as the body's path is continually redirected" wikipedia
That's exactly it - it is only an apparent force. The reference you used also explains.

It did not belong in your initial description because "you" doing the observing are not rotating with the ball. No reason for you to have an inertial correction. You do feel the ball pull back on the string but recall - you are providing the applied force to the center. This is an unbalanced force resulting in acceleration towards the center which you see as circular motion.

The ant in my description has a different POV. He sees no centripetal forces, but it does make sense to talk about his experience in terms of the centrifugal pseudoforce.

In Newtonian physics, the appearance of a pseudoforce in your physics is a clue that you are in an accelerating reference frame.
 

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