Solving Forces Acting on a Swinging Gymnast

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Homework Help Overview

The problem involves a gymnast swinging on a horizontal bar, where the objective is to determine the force she must exert on the bar at the bottom of her swing. The discussion centers around the application of mechanical energy conservation and centripetal force calculations.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to calculate the mechanical energy at the top of the swing and uses it to find the tangential velocity at the bottom. Some participants question the accuracy of the energy calculations, particularly regarding the value of gravitational acceleration used.

Discussion Status

Participants are actively discussing the calculations presented, with some noting discrepancies in the total energy values. There is an ongoing exploration of how different values for gravitational acceleration affect the results, but no consensus has been reached regarding the correct approach or final answer.

Contextual Notes

There is mention of differing values for gravitational acceleration (g=9.8 m/s² vs. g=10 m/s²), which may influence the energy calculations and the resulting force determination. The original poster expresses uncertainty about their calculations in relation to the book's answer.

danago
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A 40kg gymnast is swinging on a horizontal bar. Her center of mass is 1.2m from the bar, and right at the top of the circle she is traveling in, her body has a speed of 1m/s.

What force must she hold onto the bar with right at the bottom of the swing if she is to continue swinging?


Well first thing i did was calculate the mechanical energy in the system right at the top of the swing.

[tex] \begin{array}{c}<br /> E_M = E_k + E_p \\ <br /> = \frac{{mv^2 }}{2} + mgh \\ <br /> = 980J \\ <br /> \end{array}[/tex]

Since energy is conserved, i used this to calculate the tangental velocity at the bottom of the swing.

[tex] \begin{array}{l}<br /> 980 = 20v^2 \\ <br /> v = 7ms^{ - 1} \\ <br /> \end{array}[/tex]

Using this, i can calculate the centripetal force (net force).

[tex] \begin{array}{c}<br /> F_c = \frac{{mv^2 }}{r} \\ <br /> = 1633.\overline {33} \\ <br /> \end{array}[/tex]

At the bottom of the swing, the force she holds on with and the weight force act in opposite directions, and i can say that:

[tex] \begin{array}{c}<br /> \sum F = F - mg \\ <br /> F = \sum F + mg \\ <br /> = 2033.\overline {33} \\ <br /> \end{array}[/tex]

The answer the book gives is different however. I am not really sure what i have done wrong. Any help?

Thanks,
Dan.
 
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The total energy is off by 20J.
 
neutrino said:
The total energy is off by 20J.

If i use g=9.8ms-2, i get a total energy of 960.8J, but the book is using g=10. Is that the 20J difference youre talking about? Or have i missed something else?
 
anyone have any input?
 

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