Analyzing the Fall of a Chain: Problem 103 of 200 Puzzling Physics Problems

Click For Summary

Homework Help Overview

The problem involves analyzing the dynamics of a chain falling off a table, focusing on the forces acting on the chain and the implications of its lack of rigidity. It falls under the subject area of classical mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the forces acting on the chain as it falls, including gravitational force and normal force upon contact with the ground. Questions arise regarding the transition from the chain's motion to free fall and the implications of its non-rigid nature.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the forces involved and the behavior of the chain as it interacts with the ground. Some guidance has been provided regarding the nature of forces and energy dissipation, but no consensus has been reached.

Contextual Notes

Participants are considering the assumptions made about the chain's rigidity and the effects of acceleration during its fall. There is also a mention of the textbook's perspective on the problem, which may differ from the participants' interpretations.

phantomvommand
Messages
287
Reaction score
39
Homework Statement
A chain of length 1m is loosely coiled close to a hole in a table of height 1m. One end of the chain is pulled a little way through the hole and then released. After what times will the 2 ends of the chain reach the floor?
Relevant Equations
F = dp/dt
Kinematics equations
My attempt:

At first, only a small part of the chain has fallen through. Let that part have mass m, speed v, and length x. Suppose the chain has a mass per unit length of u.

To accelerate a small length of chain on the table to speed v, Force needed = v dm/dt = v (dm/dx) * (dx/dt) = uv^2.
Force acting on on the chain due to gravity = uxg
Net force = uxa

uxg - uv^2 = uxa
a = g - v^2/x.

Noting v^2 = 0 + 2ax,
a = g/3.

Very first part of the chain takes time t = sqrt(2L/a) = sqrt(6L/g) = 0.78s. (L = 1m = height of table)
When the first part touches the ground, the velocity of the chain is v = at = sqrt(2Lg/3) = 2.56m/s

My Equation for last joint of chain to reach the floor: L = vt + 1/2 (g/3)t^2
Textbook's Equation for last joint of chain to reach the floor: L = vt + 1/2 (g)t^2

The textbook claims that once the first joint touches the floor, the chain is in free fall. Why is that so? Isn't there an upwards force from the ground on the chain, which acts to decelerate each joint of the chain hitting the ground to 0 velocity? Thus, shouldn't there still remain the upward force due to changing mass?

An extension: If height of table > chain, is the following analysis correct:
- Acceleration for when the last joint of the chain leaves the table is the same as above. (a = g/3)
- As the chain falls through space (as L > length of chain), it's acceleration is g (free fall).
- Upon the first joint touching the floor, its acceleration = g/3.

FYI: This is problem 103 of 200 Puzzling Physics Problems
 
Physics news on Phys.org
phantomvommand said:
The textbook claims that once the first joint touches the floor, the chain is in free fall. Why is that so? Isn't there an upwards force from the ground on the chain, which acts to decelerate each joint of the chain hitting the ground to 0 velocity? Thus, shouldn't there still remain the upward force due to changing mass?
The normal force stops the chain as it touches the ground, after that it's balanced by the downward gravitational force of the chain lying on the ground. The lack of rigidity of the chain is important here.
 
  • Like
Likes   Reactions: phantomvommand
PeroK said:
The normal force stops the chain as it touches the ground, after that it's balanced by the downward gravitational force of the chain lying on the ground. The lack of rigidity of the chain is important here.

Thanks for the help. I am not sure if I understood you correctly, but this is what I gathered:
The net force acting to slow down the chain is negligible, because the chain is allowed to "crumble" due to its lack of rigidity.
 
phantomvommand said:
Thanks for the help. I am not sure if I understood you correctly, but this is what I gathered:
The net force acting to slow down the chain is negligible, because the chain is allowed to "crumble" due to its lack of rigidity.
The net force is not negligible: it slows the chain from its maximum speed to rest on the surface.
 
  • Like
Likes   Reactions: phantomvommand
PeroK said:
The net force is not negligible: it slows the chain from its maximum speed to rest on the surface.
Then why would the rest of the chain that is still falling through air be at "free fall", if there is a force acting on the bottom of the chain to slow it down? Did you mean the force acting on the chain on the floor is not transmitted to the falling chain, due to the chain's lack of rigidity? If so, how does the non-rigid chain dissipate the force? Thank you very much for your help.
 
phantomvommand said:
Then why would the rest of the chain that is still falling through air be at "free fall", if there is a force acting on the bottom of the chain to slow it down? Did you mean the force acting on the chain on the floor is not transmitted to the falling chain, due to the chain's lack of rigidity? If so, how does the non-rigid chain dissipate the force?
A force doesn't dissipate. Energy dissipates. A force is transmitted. The chain may transmit a force in one direction only. Think of two masses joined by a light string. The first mass may pull the second in one direction only, but cannot push it in the opposite direction via the string.

The force on the ground briefly exceeds gravity (enough to bring a falling link to rest) and then is balanced by gravity. The mass of chain on the ground is effectively dissociated from the mass of falling chain. If the chain were rigid that would not be so.
 
  • Like
Likes   Reactions: phantomvommand
PeroK said:
A force doesn't dissipate. Energy dissipates. A force is transmitted. The chain may transmit a force in one direction only. Think of two masses joined by a light string. The first mass may pull the second in one direction only, but cannot push it in the opposite direction via the string.

The force on the ground briefly exceeds gravity (enough to bring a falling link to rest) and then is balanced by gravity. The mass of chain on the ground is effectively dissociated from the mass of falling chain. If the chain were rigid that would not be so.

Thank you for the detailed explanation. This has cleared everything up.
 
  • Like
Likes   Reactions: PeroK
phantomvommand said:
Noting v^2 = 0 + 2ax,
You should not assume acceleration is constant.
The general solution of the ODE is ##2gx^3=3x^2v^2+c##.
In the present case, when t=0, x=0 and v=0, leading to the equation you obtained.
 
  • Like
Likes   Reactions: phantomvommand

Similar threads

  • · Replies 100 ·
4
Replies
100
Views
7K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 45 ·
2
Replies
45
Views
4K
  • · Replies 2 ·
Replies
2
Views
3K