voko
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Since r is periodic w.r.t. the angle, the orbit has to be closed. But it is not repeated every 120 degrees. It is repeated every 360 degrees.
The discussion focuses on the motion of a particle under a central force defined by $$\underline{F(r)} = -mk\left[\frac{3}{r^2} - 2\frac{a}{r^3}\right] \hat{r}$$. The radial equation of motion is derived as $$\ddot{r} - \frac{9}{4} \frac{ka}{r^3} = -\frac{3k}{r^2}$$, which simplifies to a linear form $$u''(\theta) + 9u(\theta) = 12/a$$ by substituting $$u(\theta) = 1/r(t)$$. The solution yields the orbit equation $$r = \frac{3a}{4 - \cos(3 \theta)}$$, indicating a bounded trajectory with specific minima and maxima at defined angles.
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voko said:Since r is periodic w.r.t. the angle, the orbit has to be closed. But it is not repeated every 120 degrees. It is repeated every 360 degrees.
voko said:Without analyzing it further, there is clearly a sign error in the 1/r term after rearranging.
voko said:Well, I cannot really say what the questions means. But at this stage, you might want to read this:
http://en.wikipedia.org/wiki/Newton's_theorem_of_revolving_orbits
Pay attention to Fig. 10, green orbit.
voko said:Perhaps you could compare that to an elliptical orbit.