Here , so the Binet equation reduces to
The initial conditions become
Multiply the differential equation by and use the chain rule:
The initial conditions give . Since , cannot change sign at a finite value of . Thus on the physical branch. Separation of variables gives
Therefore
The natural logarithm must be positive because . For the forward trajectory, and , so : the particle travels counterclockwise while strictly decreases.
For , it starts at , with tangent vector proportional to . Its successive crossings of the positive coordinate axis have radii
It makes infinitely many inward turns, approaching the origin as . There is no finite-time arrival at the origin: behaves as , whose improper integral diverges. If extended backwards, it comes from infinity as .
Figure 1.
Forward central-force trajectory for a=1, with arrows showing counterclockwise inward motion
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