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I have this question which is confusing as it should be harder than it appears...
A uniform chain of length L lays on a frictionless table top. Suppose one link just hangs over the table's edge so that the chain begins to fall.
Let x 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 L below the table top).
I went with
mgL = (L - x)mgL + xmg\left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2
which led to
v^2 = gx^2 + 2gL(1 - L)
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?
A uniform chain of length L lays on a frictionless table top. Suppose one link just hangs over the table's edge so that the chain begins to fall.
Let x 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 L below the table top).
I went with
mgL = (L - x)mgL + xmg\left(L - \frac{1}{2}x\right) + \frac{1}{2}mv^2
which led to
v^2 = gx^2 + 2gL(1 - L)
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?