Solving the Problem of an Infinite Chain Slipping Down a Table

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Homework Help Overview

The problem involves a chain of infinite length slipping down a table without friction, with the goal of determining the position of the tip of the chain over time. The subject area includes dynamics and the application of Lagrangian mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss various approaches, including Newton's equations and Lagrangian mechanics. Questions arise regarding the application of the Euler–Lagrange equations and the implications of the chain's infinite length on its mass and motion.

Discussion Status

Participants are exploring different methods to model the problem, with some providing guidance on using conservation of energy and Lagrangian mechanics. There is an ongoing examination of assumptions related to the infinite length of the chain and its physical implications.

Contextual Notes

There is a mention of potential confusion regarding the infinite mass of the chain and how that affects its motion. The discussion also reflects on the need for a clear reference point for potential energy.

johnson12
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Hello all, I'm having trouble with the following problem:

Pb: A chain with constant density and infinite length is slipping down from the table without friction. Determine the position of the tip of the chain at time t.

I know there are a few ways to approaching this problem, namely from Newtons equations, or lagranges equations, but I am quite rusty with this, so any suggestions would help a lot, thanks.
 
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Hi,

do you know the Euler–Lagrange equations ?
You have to find an expression for the potential and kinetic energy,
the difference is the Lagrange-function. Put this function in the Langrange equations
and you get a second order diff.-equation.

kind regards
 
Hi johnson12! :smile:

Infinite length? … presumably only in one direction? :wink:

Use conservation of energy.
 
are you referring to this equation:

\frac{\partial L}{\partial x_{i}} - \frac{d}{dt}\frac{\partial L}{\partial \dot{x_{i}}} = 0, i=1,2,3

where L = T - U is the lagrange function,

how can I use this to model my problem?
(ps. I am apologize if my physics is wrong, unfortunately I am a math major).
 
johnson12 said:
are you referring to this equation:

\frac{\partial L}{\partial x_{i}} - \frac{d}{dt}\frac{\partial L}{\partial \dot{x_{i}}} = 0, i=1,2,3

where L = T - U is the lagrange function,

how can I use this to model my problem?
(ps. I am apologize if my physics is wrong, unfortunately I am a math major).

Yes, but we need only one variable x_1 = y for example. Now you have to find an expression
for the kinetic energy T which is simple and for the potential energy U which is simple
as well. U depends of course at your point of reference. Make a sketch.
 
I get that T(\dot{x}) = \frac{1}{2}m \dot{x}^{2}
U(x) = mgx,

\frac{\partial L}{\partial x}= - m g
\frac{d}{dt} \frac{\partial L}{\partial \dot{x}}= m\ddot{x}
Lagranges equation implies m\ddot{x} + mg = 0

but I'm a little confused, if the chain is of infinite length, would it then have infinite mass?

so how can the chain move?
 

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