Finding time taken to fall off table

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SUMMARY

The time required for a uniform chain of length L to fall off a smooth table, with part of its length b initially hanging over the edge, is given by the formula t = √(L/g) arccosh(L/b). This conclusion is derived using either Newton's second law or conservation of energy principles. The discussion emphasizes the need to integrate potential energy when applying conservation of energy to solve the problem. The acceleration of the chain increases as the length b increases, complicating the dynamics of the situation.

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Homework Statement


A uniform chain of length L lies on a smooth table with part of its length b initially hanging over the edge. Show that the time required for it to fall off the table when released from rest is given by

t = √(L/g) arccosh (L/b)


Homework Equations


http://img10.imageshack.us/img10/2203/integral.png


The Attempt at a Solution


Not sure how to begin, since the acceleration of the chain keeps increasing as b increases. b is in turn related to the acceleration of the chain.
 
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Welcome to PF!

Hi Arctic! Welcome to PF! :smile:

(have a square-root: √ and try using the X2 tag just above the Reply box :wink:)
Arctic said:
A uniform chain of length L lies on a smooth table with part of its length b initially hanging over the edge. Show that the time required for it to fall off the table when released from rest is given by

t = (L/g)^0.5 arccosh (L/b)

Either use good ol' Newton's second law, or (slightly quicker, since it gives you a first-order equation :wink:) simply use conservation of energy. :smile:

(But if you use conservation of energy, don't forget you have to integrate to find the PE)
 
Using conservation of energy I get:

eq.latex?Initial%20PE%20=%20mg[(\frac{L}{2})(\frac{L-b}{L})+(\frac{L-b}{2})(\frac{b}{L})].gif

This is by breaking the chain into 2 parts: the part of length L-b lying on the table and the part b over the edge. I also take PE = 0 at height L/2 below the table to simplify calculations later

When the chain has fallen off the table, PE = 0 (since its center of gravity is at L/2 below the table) and
eq.latex?PE%20=%200.5mv^{2}=%20mg[(\frac{L}{2})(\frac{L-b}{L})+(\frac{L-b}{2})(\frac{b}{L})].gif


eq.latex?\Leftrightarrow%20v^{2}=%20g[(L-b)+(\frac{b(L-b)}{L})]=g(L-b)(1+\frac{b}{L}).gif

Not sure how to continue from here, assuming this is right that is.

As for Newton's 2nd law..
F=ma
mgb/L = ma
a = gb/L
dv/dt = gb/L
d2b/dt2 = gb/L
dt2 = d2b L/gb

Again, I am stuck here
 

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  • eq.latex?Initial%20PE%20=%20mg[(\frac{L}{2})(\frac{L-b}{L})+(\frac{L-b}{2})(\frac{b}{L})].gif
    eq.latex?Initial%20PE%20=%20mg[(\frac{L}{2})(\frac{L-b}{L})+(\frac{L-b}{2})(\frac{b}{L})].gif
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