How can I find the acceleration and position of a chain overhanging a table?

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In summary, the conversation discusses the problem of finding the acceleration of a chain as it falls off a table. The solution is found using energy conservation or by solving a differential equation. The final solution is given as x = \frac {L}{2} \cosh \left( \sqrt {\frac {g}{2L}} t\right).
  • #1
hola
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A chain of length 2d and mass 2m is placed over a frictionless table such that half of the rope is on the table; the other half dangling, and it is just starting to accelerate. Find its acceleration as a function of time.

I couldn't get this one.

I tried net force = ma
(m+d)g = 2ma; where d represents the mass of the part of the chain that has slipped. But I can't get it in terms of t. Any help?
 
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  • #2
If I understood correctly the only thing falling is the chain like this:
[" ******
---------* ||
--------|* \/
--------|* "]
* = chain
and the "arrow" is the direction that it is falling.
Hint: all mass falls with the same acceleration(on earth).
 
  • #3
I know, but I can't solve for a in terms of t.
 
  • #4
If there's no friction then the acceleration is constant (same a for every t);
 
  • #5
As more of the chain is sliding off the table, the remaining chain will experience a larger force pulling it off teh table. Acceleration is not constant
 
  • #6
Yes there will be a larger FORCE pulling it of the table but there will also be more mass to pull. Since F=ma the more massive the body is the more force you need to accelerate it. you can also see this mathematicly:
F=ma , in this case the force is mg so:
mg = ma /m
g=a
As you can see, the mass is irrelevant since the more mass you add to the force (mg) the more you need to accelerate it (ma) so the masses cancel out. If there was friction then it would be different cause you'd have more force to overcome the friction and then you'd speed up.
 
  • #7
daniel_i_l said:
If there's no friction then the acceleration is constant (same a for every t);

No, the acceleration is not constant. If x is the length of chain hanging over the edge then the acceleration is

[tex]\frac {gx}{2L}[/tex]

The force acting on the chain is the weight of the hanging chain but it's the entire chain that is being accelerated.
 
  • #8
You totally right, I was only looking at the mass hanging over the end:(
 
  • #9
Were you able to solve this? I tried solving it but I can't. I set up a few relationships, but I think this problem requires some calculus and I'm really weak with that. Can someone help further please?
 
  • #10
The solution works out to [itex]x = \frac {L}{2} \cosh \left( \sqrt {\frac {g}{2L}} t\right)[/itex].
 
  • #11
how did you do it?
 
  • #12
There are two ways to do it. The easier way is to write down an equation expressing energy conservation. It relates the speed of the mass to the length of overhanging mass. Once you have that, solve for v and, since v = dx/dt you can integrate to find x(t).

The other way is to start with the second derivative of x equals gx/2L. It's a little messier but if you're into differential equations you should be able to handle it.
 

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