Tetherball wrapping around a pole

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Homework Help Overview

The discussion revolves around a tetherball scenario where the ball is kicked with an initial velocity and wraps around a pole. The problem involves analyzing the dynamics of the tetherball, specifically focusing on the relationship between the length of the string, angular velocity, and linear velocity, while neglecting external forces like gravity and air resistance.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to set up a differential equation to describe the length of the string over time and seeks to analyze angular and linear velocities without relying on conservation of angular momentum. Some participants suggest alternative approaches, such as expressing the length of the string as a function of time rather than using differential equations.

Discussion Status

Participants are exploring various methods to express tangential and angular velocities in relation to the number of revolutions made. There is a recognition that the linear velocity remains constant, while angular momentum is not conserved due to the torque from the tension in the string. Multiple interpretations of the problem are being discussed, with no explicit consensus reached.

Contextual Notes

The original poster notes that they may have omitted necessary information for a complete analysis, which could affect the discussion. Additionally, the problem is framed as a non-homework scenario, indicating a more exploratory approach to the physics involved.

opticaltempest
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Hello,

I am trying to analyze the following situation:

A tetherball is kicked with velocity of v meters per second at time t=0 seconds. The length of the string attaching the tetherball to the pole is l meters. The radius of the pole is r. Assume no gravity and no air resistance so that the ball wraps around the pole in the plane in which it is initially kicked. In other words, when the ball makes one complete revolution around the pole the length of the string is reduced by 2\pi r.

1. I would like to set up a differential equation that describes the length of the string at any time t.

2. My ultimate goal is to analyze the angular velocity and linear velocity at any time when the ball is wrapping inward towards the pole without using the conservation of angular momentum.

This isn't a homework problem so I might have left out information needed to complete the problem.

I am having trouble on all approaches. Any help will be greatly appreciated.
 
Last edited:
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I don't think you need to use any DiffEq for this. Just write an equation for the length of string versus time, and use that to express he position of the ball mass versus time...
 
I think I see how to express tangential velocity and angular velocity in terms of how many revolutions were made.

How would I express the tangential velocity and angular velocity in terms of time?

From the relationship between tangential velocity v_{t} and
angular velocity \omega

v_{t}=r\omega

Where r, in our case, would be the length of the string.

The length of the string l at any revolution is

l=l-2\pi r \gamma

Where \gamma is the number of revolutions.

The tangential velocity is then

v_{t}=(l-2\pi r \gamma)\omega

and

\large \omega = \frac{v_{t}}{l-2\pi r \gamma}
 
Last edited:
You have probably forgoten about this post by now. I have been recently looking at this problem. The magnitude of the linear velocity is constant. Angular momentum as it is not conserved in this system. If you let the centre of the pole be a fulcrum then there is a torque due to the tension in the string which decreases the angular momentum as it wraps around.

So to do the problem you let the velocity stay constant and energy is conserved. angular velocity will increase and angular momentum will decrease.
 

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