What Are the Equilibrium Points of a Pendulum System with an Elastic Force?

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Homework Help Overview

The discussion revolves around finding the equilibrium points of a pendulum system that includes an elastic force acting on a moving particle along a rod. The setup involves a fixed point O, a mass m attached to a rod, and another mass m that is influenced by an elastic force.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the Lagrangian formulation of the system and express confusion regarding the equations of motion derived from it. There are attempts to identify equilibrium conditions based on the second derivatives being zero.

Discussion Status

Some participants have pointed out potential issues with the Lagrangian, particularly regarding the gravitational potential energy and its dependence on the variable X. Others have raised questions about the correctness of the Lagrangian and the expected equilibrium conditions.

Contextual Notes

There is a mention of a discrepancy in the potential energy terms used in the Lagrangian, specifically regarding the elastic force and gravitational potential energy setup. Participants are exploring the implications of these differences on the equilibrium points.

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Homework Statement


A long light inflexible rod is free to rotate in a vertical plane about a fixed point O. A particle of mass m
is fixed to the rod at a point P a distance ℓ from O. A second particle of mass m is free to move along the rod, and is attracted to the point O by an elastic force of strength k.

Find any equilibrium points. (You may assume the rod is sufficiently long that the moving particle does not reach either end of the rod).

Homework Equations


The potential due to the elastic force is ##V = kx^2##

The Attempt at a Solution


Let ##X## be the distance of the second particle from the origin O. Then the Lagrangian I got is
##L = \frac{1}{2}m[\dot{X}^2 + (X^2 +l^2)\dot{\theta}^2] - mg[X(1-cos\theta) +l(1-cos\theta)] - kX^2##
This gives the equations of motion for ##X(t)## and ##\theta (t)## as
##\ddot{X} = X(\dot{\theta}^2 - 2k) -g(1-cos\theta)##
##\ddot{\theta}(X^2+l^2) + 2\dot{X}\dot{\theta} = -gsin\theta(X + l)##.

Equilibrium points occur when the second derivatives are both zero, so I have to solve
##0 = X(\dot{\theta^2} - 2k) -g(1-cos\theta)##
##2\dot{X}\dot{\theta} = -gsin\theta(X + l)##
And now I'm lost. If I try to solve these I will end up with the fixed points ##X## and ##\theta## as functions of ##t##, which doesn't seem right to me.

Any help would be appreciated, maybe the Lagrangian I got is incorrect.
 
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m has disappeared from the equations of motion

I would expect an equilibrium at ##\dot X =0,\ \dot\theta = 0,\ \theta = 0, X = {mg\over 2k}##, so there must be something with ##L##. And sure enough: for ##\theta=0## V doesn't depend on X !
 
Hi there, I am also struggling on this question? I get the same Lagrangian except the potential of the spring is 1/2*k*x^2. Can anyone explain why this L is wrong?
 
As BvU hinted: the gravitational potential energy of the second mass is not correctly set up in the Lagrangian. For the special case where θ = 0, the gravitational PE of the second mass should certainly depend on the variable X. But in the Lagrangian in post #1, this is not so.

You need to be careful about where you are defining zero gravitational PE for the two masses.
 

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