Chain sliding off the edge of a table

AI Thread Summary
The discussion centers on a physics problem involving a chain sliding off a table, focusing on static and kinetic friction. Participants explore how to analyze the forces acting on the chain, particularly the balance between gravitational force and frictional force as portions of the chain hang off the edge. The equilibrium condition is established, showing that the chain will slide if at least 3.00m hangs over the edge, with calculations involving mass ratios and friction coefficients. For determining the speed of the chain as it leaves the table, energy methods are suggested, emphasizing the transformation of potential energy to kinetic energy while accounting for work done against kinetic friction. The conversation highlights the importance of understanding the dynamics of the chain's motion and the forces involved.
gaborfk
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A uniform chain of length 8.00m initially lies stretched out on a horizontal table.

a)
If the coefficient of static friction between the chain and the table is 0.600, show that the chain will begin to slide off the table if at least 3.00m of it hangs over the edge of the table.

b)
Determine the speed of the chain as all of it leaves the table, given that the coefficient of the kinetic friction between the chain and the table is 0.400.

I do not have a clue on how to draw up an FBD and start working on the problem. I kind of think it has to do with partial derivatives since the length of the chain, its mass hanging off the edge and its speed and acceleration varies with time.

Can someone please, help me out to get started by giving a direction or a generic setup which I can start to work with.

Thank you in advance!
 
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Treat the chain as having two segments: one piece on top of the table, the other hanging. What are the forces on each?
 
The first one is just setting the friction force equal to the force of gravity. The second one is trickier, however. We know that F_f = \mu mg and that F_g=mg but the m's are changing over time. Let m=m_f+m_g to denote the portion of the mass being affected by friction and gravity, respectively. The net force acting on the chain is then F_g-F_f = m_g g - \mu m_f g = m a. I may have stopped my explanation too early so tell me if you need me to extend it a little further. Perhaps someone knows a less complicated way as well.
 
Does either have any tension forces acting on it?

If not the 5m segment has a negative F(friction) and it equals to the gravity acting on the 3m segment.

Is this correct?

-F(friction)=-F(gravity)

0=F(friction)-F(gravity) (equlibrium, chain does not slide if ratio is 5/3)

Also, how do I account for the length of the chain segments in the force equation since I do not have the density to calculate the mass? Do I just use ratios?

Thank you
 
Thank you for your reply. Yes, that would be great if you could expend on it a bit.

Thanks
 
gaborfk said:
Does either have any tension forces acting on it?
They better--or else how can the weight of the hanging piece affect the piece on the table? In equilibrium, the tension at the top of the hanging piece will equal its weight. And that tension exerts a force on the tabled piece tending to pull it towards the edge.

If not the 5m segment has a negative F(friction) and it equals to the gravity acting on the 3m segment.

Is this correct?

-F(friction)=-F(gravity)

0=F(friction)-F(gravity) (equlibrium, chain does not slide if ratio is 5/3)
Essentially correct, but how would you get the answer if it wasn't given? (See below.)

Also, how do I account for the length of the chain segments in the force equation since I do not have the density to calculate the mass? Do I just use ratios?
The way I'd do it is to call the hanging length "x". Its mass is then (M/L)x, where M is the mass of the chain and L the length of the chain. You'll find that M drops out.

To solve the first part, write the mass of the tabled piece and hanging piece using the above trick. Then set up your equilibrium equation and solve for x.
 
Here is how I solved the first part:

m=ro*x

Where x is the length of the chain

So m1=5ro, m2=3ro

Equation

F(gravity)-F(friction)=0
m2g-mu*m1g=0
(9.8)(3)ro-(9.8)(5)(0.6)ro=0
Since the g*ro will drop off we are left with 3-(5*0.6)=0 and that is true!

Now onto the second part...

Can you please start me out on how to get the V out of the above equations? Do I work backwards from F=ma, then solve for a, substitute dv/dt and do a partial derivative??

Thank you
 
gaborfk said:
Can you please start me out on how to get the V out of the above equations? Do I work backwards from F=ma, then solve for a, substitute dv/dt and do a partial derivative??
Sounds like a lot of work to me! :smile: To find the speed of the chain, I would use energy methods. An interesting problem!
 
Can you please get me started on the energy method? I understand that the chain as it slides down has both kinetic and potential energy. Do I start with the chain hanging as initial condition and just as it passed the edge of the table as the final condition and use Ui+Ki+W=Uf+Kf? How would I account for the Friction Force? Static or Kinetic?
 
  • #10
Yes, I would start at the point it begins to fall. As you know, it has an initial potential energy, and ends up with some kinetic energy. Along the way it transforms some of its mechanical energy to friction. The challenge is to figure out the work done against friction. (And you must use kinetic friction--otherwise no displacement and no work! :smile: ) Hint: the chain is stretched out for a reason.
 
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