Coupled 2nd-Order Non-linear ODEs

cepheid

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1. The problem statement, all variables and given/known data

I'm trying to solve the equations:

[tex] \ddot{\phi} + 2\left(\frac{\cos \theta}{\sin \theta}\right) \dot{\theta}\dot{\phi} =0 [/tex]​

and

[tex] \ddot{\theta} - \sin \theta \cos \theta \dot{\phi^2} =0 [/tex]​

for [itex] \theta(\lambda), \phi(\lambda) [/itex] where the dots represent differentiation w.r.t the parameter [itex] \lambda [/itex].

2. Relevant equations

Chain rule, other differentiation tricks


3. The attempt at a solution


I've tried to tackle the first equation by writing:

[tex] \frac{\cos \theta}{\sin \theta} \dot{\theta} = \frac{1}{\sin \theta} \frac{d}{d\theta}(\sin \theta) \dot{\theta} = \frac{d}{d\lambda}[\ln (\sin \theta) ] [/tex]​

I'm wondering if it's correct to do that. It seems to follow from the chain rule, but I'm not sure. If so, then the equation becomes:

[tex]\frac{\ddot{\phi}}{\dot{\phi}} = -2\frac{d}{d\lambda}[\ln (\sin \theta) ] [/tex]

[tex]\frac{1}{\dot{\phi}}\frac{d \dot{\phi}}{d\lambda} = -2\frac{d}{d\lambda}[\ln (\sin \theta) ] [/tex]

[tex]\frac{d \ln ( \dot{\phi})}{d\lambda} = -2\frac{d}{d\lambda}[\ln (\sin \theta) ] [/tex]​

Then I integrated both sides w.r.t. lambda:

[tex]\ln ( \dot{\phi}) = - 2\ln (\sin \theta) + \mathrm{~const.} [/tex]

[tex] \dot{\phi} \propto \frac{1}{\sin^2 \theta} [/tex]​

Then I tried substituting this result into the second ODE, but it gave me:

[tex] \ddot{\theta} \propto \frac{\cos \theta}{\sin^3 \theta} [/tex]​

which I don't know what to do with.
 
Last edited:

cepheid

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Science Advisor
Gold Member
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Just bumping the thread. Any insight you might have, esp. regarding the last line, would be most helpful.
 

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