For first order systems the motion tends to fixed points or infinity, but for second order systems the situation can be more complex. Consider for example a system separable in polar coordinates
such that the motion has a fixed point (in terms of
) other than at the origin:
![]()
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where
are constant.
The circle
is a phase curve and since the motion moves around it indefinitely it is a cycle. Any closed phase curve is a cycle – a motion for which
are periodic with the same period.
For
the motion of the system above is a circle and we may treat
as a fixed point of the system. In the region of
the motion obeys the equations
where![]()
![]()
The solution of this linearisation is
and the phase curves are given by eliminating
from these two equations, obtaining
![]()
If
the system is stable in the sense that motion initially close to the system will be attracted to it, and any perturbed motion initially on the circle will return to it. If
the system is unstable.
A more general form of limit cycle is shown below with various starting points.
