I am having difficulty using Poincare-Bendixson to show that a particular system of differential equations has a periodic orbit. The system is
$$
\left\{\begin{array}{rcl}
\dot{x} & = & -3y+x(1-x^2-y^2+y)
\\
\dot{y} & = & \phantom{-}2x+y(1-x^2-y^2-4x)
\end{array}\right.
$$
Now, the expression $1-x^2-y^2$ made me investigate the unit circle:
- However, I found that some solutions enter through the unit circle while others leave it, so it wasn't a useful "boundary".
- So, more generally, I converted to polar and consider the circle $x^2+y^2=r^2$.
- I was able to verify that for sufficiently large $r$, no solutions leave through the circle of radius $r$ (i.e. $\dot{r}<0$).
- Thus, any solution starting in the circle of radius $r$ remains in it.
- Thus, if I take a solution starting within this circle, I can consider its forward $\omega$-limit set, which will be nonempty, compact, and connected.
- The issue is that there is at least one fixed point within this circle (at the origin) and there could be more. - I am not sure how to find the fixed points and argue that there is a solution not converging to any of them in forward time.
Any ideas $?$.