Solving the Puzzling Physics Problem: Chain Falling Off Table

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Homework Help Overview

The problem involves a uniform chain of length L that begins to fall off a frictionless table, with one link hanging over the edge. The original poster seeks to determine the vertical acceleration of the chain at a given moment, denoted by x, which represents the amount of chain that has fallen. The discussion revolves around the application of conservation of energy and Newton's second law to analyze the motion of the chain.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the use of conservation of energy and differential equations to analyze the problem. There are questions about the correctness of the initial energy equation and whether the problem can be approached using Newton's second law. Some participants suggest simplifying the analysis by focusing on forces acting on the chain.

Discussion Status

There is an ongoing exploration of different methods to solve the problem, with participants providing feedback on each other's equations and suggesting corrections. Some guidance has been offered regarding taking derivatives and simplifying expressions, but no consensus has been reached on a single approach.

Contextual Notes

Participants note that the choice of potential energy reference level could simplify the problem, and there is discussion about the assumptions made regarding the chain's motion and the forces involved.

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I have this question which is confusing as it should be harder than it appears...

A uniform chain of length [tex]L[/tex] lays on a frictionless table top. Suppose one link just hangs over the table's edge so that the chain begins to fall.

Let [tex]x[/tex] be the amount of chain that has fallen. What is the chains vertical acceleration at this instant.

I started off trying to use conservation of energy
(with the zero potential line being a distance [tex]L[/tex] below the table top).

I went with

[tex]mgL = (L - x)mgL + xmg\left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2[/tex]

which led to

[tex]v^2 = gx^2 + 2gL(1 - L)[/tex]

Now firstly I am not sure if this is correct. If it is then what is my next step?

Secondly, I started thinking is the problem maybe a pretty simple differential equation from Newtons second law?

Or can it be done both ways?
 
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No Name Required said:
I went with

[tex]mgL = (L - x)mgL + xmg\left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2[/tex]
Realize that your units don't match--you have an extra L floating around in two of your right side terms. Redo this.

Also realize that you are assuming that the chain is laid out in a straight line so that it moves with a single speed. (Sounds like a good assumption.)
Now firstly I am not sure if this is correct. If it is then what is my next step?
It's wrong, as noted. But once you get the correct expression for v, just take a derivative.

Secondly, I started thinking is the problem maybe a pretty simple differential equation from Newtons second law?
Sure. Just consider the forces acting on the chain.

Or can it be done both ways?
Absolutely!
 
At your right hand side, you may want to replace the m by the density m/L in the first and second term, otherwise the equation seems cool

and your way is not the best way(easiest way) to attack this problem. try to find the force directly.. (the only force here is gravity) and the acceleration is F/m

the force should be depend on time F=F(t), but the problem is asking you to solve F(x), therefore, you don't need do solve the differential equation
 
Ah rite k, thankyou :smile:

It should correctly be

[tex]mgL = (L - x)mg + xmg\left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2[/tex] yes?

If this is right, you say take the derivative... Is this with respect to t?
(in order to get [tex]\frac{dv}{dt}[/tex])

If this is so i found

[tex]\frac{dv}{dt} = \frac{g - gL + xg}{\sqrt{2xg - 2xgl +x^2g}}\frac{dx}{dt}[/tex]

This looks wrong except for the fact that [tex]\frac{dx}{dt} = v[/tex] i suppose...

Ill look further into the differential equation solution.
 
No Name Required said:
It should correctly be

[tex]mgL = (L - x)mg + xmg\left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2[/tex] yes?
Getting closer--now only one term is wrong. :smile:
It should look like this:
[tex]mgL = (L - x)mg + xmg(L - \frac{1}{2}x)/L + \frac{1}{2}mv^2[/tex]

You'll find that this expression simplifies nicely, giving you a simple expression for v as a function of x.

If this is right, you say take the derivative... Is this with respect to t?
(in order to get [tex]\frac{dv}{dt}[/tex])
That is correct.

If this is so i found

[tex]\frac{dv}{dt} = \frac{g - gL + xg}{\sqrt{2xg - 2xgl +x^2g}}\frac{dx}{dt}[/tex]
Wrong, for reasons stated above. Once you get the correct expression for v, taking the derivative will give you the acceleration.

This looks wrong except for the fact that [tex]\frac{dx}{dt} = v[/tex] i suppose...
Yes, you will need to use this fact.

Ill look further into the differential equation solution.
Don't give up on the above solution. Once you get the right initial expression, the answer comes easy.

But definitely do it using Newton's 2nd law also. Don't worry about differential equations... all you need is F = ma.

Of course, you'll get the same answer. :wink:
 
take the derivative of the WHOLE THING, the algebra will much much simpler...

[tex]\frac{d}{dt} [mgL] = \frac{d}{dt} [(L - x)mg + xmg/L \left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2][/tex]

because of the chain rule, ALL (non-zero) TERMS has a v... therefore, you can cancel the v by dividing the whole equation by v...
and you will get dv/dt as a function of x only...(which is what your original problem asking you to do)

BTW, why don't u apply F=ma directly... obviously, F= mgx/L and a=mx/L...
 
Just a note. Problem would have been much simplified if the tabel top was used as the zero potantial level.
 
Gamma said:
Problem would have been much simplified if the tabel top was used as the zero potantial level.
This is true! (That's how I would do it. :smile:) But regardless of zero level, the expression simplifies immediately.
 
Thankyou!

Ah yes, all is clear now :smile:
Thankyou all very much for your help. Its much appreciated.
 

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