Effective potential of a particle sliding on an inclined rod

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SUMMARY

The discussion centers on a point mass sliding along a rigid rod fixed at the origin, forming an angle α with the z-axis and rotating with a constant angular velocity ω. The system has one degree of freedom, represented by the distance r from the origin to the mass. The Lagrangian is derived as L = (1/2)m[˙r² + r²ω²sin²α] - mgrcosα, leading to the Lagrange equation &ddot;r - rω²sin²α + gcosα = 0. The effective potential must be derived from this Lagrangian to analyze equilibrium positions and their stability.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with angular motion and effective potential concepts
  • Knowledge of differential equations
  • Basic principles of classical mechanics, including kinetic and potential energy
NEXT STEPS
  • Derive the effective potential from the given Lagrangian
  • Analyze equilibrium positions by differentiating the effective potential
  • Determine stability by applying the second derivative test on the effective potential
  • Explore the implications of angular velocity on the motion of the mass
USEFUL FOR

This discussion is beneficial for students and professionals in physics, particularly those studying classical mechanics, Lagrangian dynamics, and rotational motion analysis.

Dixanadu
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Homework Statement



Hey guys,

Here is the question:

A pointlike mass m can slide along a rigid rod of length l and negligible mass. One extremity of the rod is fixed at the origin O of an inertial system (x,y,z), and the rod forms a constant angle α with the z-axis. The rod rotates about the z-axis with constant angular velocity ω. Gravity acts in the negative z-direction.

(i) How many degrees of freedom does the system have?

(ii) Write down the Lagrangian and the Lagrange equations.

(ii) Recast the system as a 1-dimensional motion in an effective potential. Find an expression for the effective potential and determine the equilibrium positions as well as their stability

Homework Equations


T=1/2mv^{2}
Lagrangian: L = T - V
Lagrange Equation: \frac{d}{dt}\frac{\partial L}{\partial \dot{q}} = \frac{\partial L}{\partial q}

The Attempt at a Solution


Here are my solutions:

(i) one degree of freedom - the distance from the origin to the point mass. call this distance r.

(ii) I won't put the calculations here, I'll just give my results:

Lagrangian L = T - V = \frac{1}{2}m[\dot{r}^{2}+r^{2}ω^{2}sin^{2}α] - mgrcosα


Lagrange equation: \ddot{r}-rω^{2}sin^{2}α + gcosα = 0

(iii)

Okay, so here is the issue. How do you get the effective potential from this? and do I just differentiate that to get the equilibrium positions and then differentiate again to determine stability?
 
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Okay, so here is the issue. How do you get the effective potential from this?
If you had a particle of mass m confined to 1-dimension of space (a straight line) and you let r be the distance from the origin, how would you express the kinetic energy T? How would you construct a potential energy function V(r) for this particle so that it would have the same Lagrangian L as your three-dimensional problem of the particle on the rotating wire?

and do I just differentiate that to get the equilibrium positions and then differentiate again to determine stability?
Sounds good.
 

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