Solving for Potential Energy of Hanging String: Integrals and Equations

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Homework Help Overview

The discussion revolves around calculating the potential energy of a hanging string with mass m and length L, positioned over the edge of a table. Participants explore the implications of defining potential energy in relation to the height of the string segments below the table.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss defining potential energy for small mass elements and consider using mass density for integration. Questions arise regarding the integration limits and the implications of uniform mass density.

Discussion Status

The conversation includes attempts to derive the potential energy through integration, with some participants suggesting alternative methods involving the center of mass. There is ongoing exploration of how to handle the variable length of the string and the limits of integration.

Contextual Notes

Participants note the absence of explicit information about the length L in the original problem statement, raising questions about its necessity for the calculations.

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Homework Statement


This is actually just a minor part of a larger problem - I need to find the potential energy of a string of mass m and length L that is hanging over the edge of a table.


Homework Equations





The Attempt at a Solution


If we define V = 0 at the level of the talbe, then the potential energy of a mass element dm below the able is given by V = -gydm where y is the height of dm below the table. But here I blank - how can I use this to find the total potential energy o hte cord?
 
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What about thinking in terms of a mass density \delta so the potential of a string segment of length dy is -\deltaydy and integrating with respect to y?
 
I'm not sure I follow

the liear mass density would be m/L assuming that it is uniform, but how can I turn that into the integral?
 
KBriggs said:
I'm not sure I follow

the liear mass density would be m/L assuming that it is uniform, but how can I turn that into the integral?

For each segment dy of cable that is hanging over the edge a distance y it's potential is -\delta y\,dy. You have to add all these up, which you do by integrating with appropriate y limits.
 
So we get:

\int_0^y(\frac{-mg}{L}y)dy = \frac{-mg}{2L}y^2

Is that right, assuming that a length y is hanging over the edge?


The only problem is that I am not explicitly given L in the question, so I am not sure if I can use it. Is there a way to get the potential of a string of mass m hanging a distance y over the edge of a table without using the length? I can't think of anything.
 
y is the variable. You don't want it in the upper limit. If h is the length of the cable hanging over the edge your integral would go from 0 to h.
 
Alright - if you replace y by h in the above, is it correct? ^_^
 
It looks OK to me.
 
Thanks :)

Now that it's done, I see you can get the same thing without the integral by using the centre of mass of the part of the cord that is hanging over the edge.
 

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