Finding the Polar Equation of a Circular Orbit in a Central Force Field

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A particle in a central force field moving in a circular orbit requires the polar equation of the orbit to be derived. The discussion highlights the confusion around setting up the equation, specifically the second-order differential equation involving the inverse radius and angle. The equation mentioned is related to Goldstein's mechanics text, suggesting a specific form to simplify the problem. A transformation involving the inverse radius is recommended to facilitate finding the solution. The conversation emphasizes the need for clarity in the steps to derive the polar equation accurately.
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A particle moves on a circular orbit in a central force field. The origin of the force lies on the circle.

Find the polar equation of the orbit.


I am confused as to how to set up this question.
 

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Start with the equation for the invers radius of the orbit with respect to angle

{d^2u}\over {d/ \theta^2} + u =
 
Can't work it right now, back later... anyway it is r^-5.
 
I need a few more steps to be explained. I am sure that if you could please explain them to me that I will get it.
 
Also, I ahve never sen that queation before. IS it derived somewhere on the net?

Are you saying that the polar equation is r^(-5)? I need some help here desparately.
 
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My typing is bad, and it was late.

Start with Goldstein 3-34a,

\frac{d^2 u}{d\theta^2} + u = -\frac{m}{l^2u^2}f(1/u)
 
My typing is bad, and it was late.

Start with Goldstein 3-34a,

\frac{d^2 u}{d\theta^2} + u = -\frac{m}{l^2u^2}f(1/u)

set 1/u = 2acos\theta and crank away. The answer should pop out when you eliminate the \theta.

For some reason, the \frac is not working...
 
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