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

AI Thread Summary
The discussion focuses on finding equilibrium points in a pendulum system with an elastic force. The Lagrangian derived for the system is questioned, particularly regarding the gravitational potential energy of the moving mass, which is not correctly represented. Participants highlight that the gravitational potential energy should depend on the variable X, especially when θ equals zero. There is confusion about the equations of motion derived from the Lagrangian, leading to concerns about the disappearance of mass in the equations. Accurate setup of the gravitational potential energy is crucial for solving the equilibrium conditions effectively.
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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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