How do I solve for r(theta) in central force motion with r''=(k^2)*r?

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The discussion focuses on solving the central force motion equation r''=(k^2)*r, where k^2>0, and specifically on finding r(theta). The user encounters a second-order differential equation of the form r''=A/r^3+Br and seeks guidance on solving it. They derive relationships by multiplying both sides by r', leading to an expression for r'^2 in terms of a constant and the potential function X. The user expresses confidence in their progress after this derivation. The conversation highlights techniques for tackling differential equations in central force problems.
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I have a central force motion with vector form r''=(k^2)*r, where k^2>0. It's trivial to solve for the vector r(t), but I'm having a little trouble solving for r(theta). I get a second order differential equation of the form r''=A/r^3+Br. Any tips on solving this?
 
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r'' = \frac {A}{r^3} + Br = - \frac {d}{dr}(\frac{A}{2r^2} - \frac{Br^2}{2})

Multiply both sides with r' = dr/dt

LHS = r'r" = \frac{1}{2} \frac {d}{dt} r'^2
RHS = -\frac{dX}{dr}.\frac{dr}{dt} = -\frac{dX}{dt}
This gives :
r'^2 = -2(X) + const.
 
think i got it, thanks gokul
 
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