How to Derive the Theta Function for a Free Particle on a Spherical Surface?

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Homework Help Overview

The discussion revolves around deriving the theta function for a free particle constrained to move on a spherical surface, utilizing the Lagrangian and a specific metric. The original poster presents their attempts to derive the equation of motion and solve an integral related to the motion of the particle.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to derive the theta function by integrating a differential equation that arises from the equations of motion. They express uncertainty about solving a specific integral. Other participants suggest variable substitutions to simplify the integral and question the effectiveness of these substitutions.

Discussion Status

Participants are actively engaging with the problem, exploring different substitution methods and discussing the nature of the integral involved. While some guidance has been provided regarding standard integrals, there is no explicit consensus on the best approach to solve the integral at this stage.

Contextual Notes

The original poster mentions the presence of an integration constant and expresses difficulty in solving the integral, indicating potential constraints in their understanding or approach. There is also a reference to a related thread that may provide additional context.

Matt atkinson
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Homework Statement


By finding the Lagrangian and using the metric:
\left(\begin{array}{cc}R^2&0\\0&R^2sin^2(\theta)\end{array}\right)
show that:
\theta (t)=arccos(\sqrt{1-\frac{A^2}{\omega^2}}cos(\omega t +\theta_o))

Homework Equations

The Attempt at a Solution


So I got the lagrangian to be L=R^2 \dot{\theta^2} +R^2sin^2(\theta)\dot{\phi^2} and then used the E-L equation to find the equations of motion and the fact that 2R^2sin^2(\theta) \dot{\phi}=const=p.
Using this and substituting into the equation i get for \theta I get:
\frac{d}{dt}(2R^2\dot{\theta})=\frac{p^2}{2R^2}cot(\theta)csc^2(\theta)
which I then integrate using the substitution dt=d\theta / \dot{\theta} to get:
\dot{\theta}=\frac{p}{2R^2}\sqrt{c-\frac{1}{2}sin^{-2}(\theta)}
Where c is the integration constant. Now if I separate variables to attempt to get a solution for \theta i get:
\int _{\theta_o}^{\theta} \frac{d\theta}{\sqrt{c-\frac{1}{2}sin^{-2}}}=\frac{tp}{2R^2}
But i have absolutely no idea how to solve that integral. Please any pointers would be appreciated.
 
Last edited:
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Ah okay, I did just try u=cos(\theta) but it gives:
\int \frac{du}{\sqrt{c(1-u^2)-1/2}}
It didn't prove to be any easier to solve.
Also tired doing u=cos(\theta) from the beginning just now as you suggested in the other post (although this could be the wrong substitution) and I must be doing something wrong because I get a complex square root on the LHS of the differential equation for \dot{u}.
 
Matt atkinson said:
Ah okay, I did just try u=cos(\theta) but it gives:
\int \frac{du}{\sqrt{c(1-u^2)-1/2}}
It didn't prove to be any easier to solve.
This is a quite standard integral. It is of the form
$$
\int \frac{dx}{\sqrt{1 - x^2}}.
$$
 
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Thankyou so much! I managed to get the answer now, i think it was just the fact i hadn't noticed that it was a standard integral.
 

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