Small oscillations of constrained particle

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Homework Help Overview

The problem involves a particle of mass m constrained to move on the surface of a paraboloid defined by the equation r^2=4az, subjected to gravitational force. The objective is to determine the frequency of small oscillations about a circular orbit with a specified radius.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the relationship between the gravitational force and the motion of the particle, with one participant attempting to derive the frequency from a differential equation. Others emphasize the importance of considering equilibrium in the circular orbit before analyzing oscillations.

Discussion Status

There is ongoing exploration of the problem, with participants sharing their attempts and expressing challenges in arriving at the correct answer. Some guidance has been offered regarding the need to consider equilibrium conditions.

Contextual Notes

Participants are working under the constraints of the problem statement and are questioning their assumptions about the forces acting on the particle and the setup of the motion on the paraboloid surface.

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Homework Statement


Consider a particle of mass m constrained to move on the surface of a paraboloid whose equation (in cylindrical coordinates) is r^2=4az. If the particle is subject to a gravitational force, show that the frequency of small oscillations about a cirrcular orbit with radius \rho=\sqrt{4az_0} is

\omega=\sqrt{\frac{2g}{a+z_0}}


Homework Equations





The Attempt at a Solution



I'm aware that the \omega must come from the equation:

\ddot{x}+\omega x=0

This DiffEq comes from F=m\ddot{x}, so we need F=-\frac{2gm}{a+z_0}.

The only definition of g goes to \frac{MG}{R^2}, so we must be looking for a force F=-\frac{mMG}{R^2}*\frac{2}{a+z_0}

My attempt is based on looking at the radial component of a gravitational force pulling out of the plane along \hat{s}, however, every time, I get:

\vec{F}=-\frac{mMG}{S^2}\hat{s}, where the radial component would be \vec{F}\bullet\hat{r}


In a nutshell...my answer keeps turning up wrong.
 
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The particle is rotating about z axis and in equilibrium at z = z0. First consider equilibrium of particle in the circular orbit and then think of its oscillation on the surface.
 
mukundpa said:
The particle is rotating about z axis and in equilibrium at z = z0. First consider equilibrium of particle in the circular orbit and then think of its oscillation on the surface.

That's exactly what I'm doing, but I can't get the correct answer.
 
I'm going to make a late bump on this thread because I still haven't solved this problem.
 

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