Poincare-Bendixson in n-dimensions

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The discussion centers on the Poincare-Bendixson theorem and its applicability in n-dimensional systems. It establishes that while a bounded 2D invariant manifold M exists without critical points, this does not guarantee the presence of a periodic orbit in M. A counterexample is provided using the 2-torus S^1 × S^1 with a trajectory defined by (\dot \theta_1, \dot \theta_2) = (1, \alpha) where α is irrational, resulting in dense trajectories without periodic orbits. Furthermore, it is concluded that chaos cannot occur in two dimensions, as three dimensions are necessary for chaotic behavior.

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  • Understanding of dynamical systems and invariant manifolds
  • Familiarity with the Poincare-Bendixson theorem
  • Knowledge of periodic orbits and chaos theory
  • Basic concepts of topology, specifically regarding the 2-torus
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This discussion is beneficial for mathematicians, physicists, and researchers in dynamical systems, particularly those interested in the implications of the Poincare-Bendixson theorem and the behavior of systems in various dimensions.

motherh
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Suppose that [itex]\dot{x}[/itex] = f(x) in [itex]\Re[/itex][itex]^{n}[/itex]. There exists a bounded 2D invariant manifold M for this system. There are no critical points in M. Does it follow that there is a periodic orbit in M?

I've realized that this has it's similarities to Poincare-Bendixon's theorem but I don't believe that it holds for a system in n dimensions. Would I be correct in thinking that even with the strict conditions above we could end up with chaos? If I am correct here, does anybody know of any counterexamples for the above statement? Thanks.
 
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motherh said:
Suppose that [itex]\dot{x}[/itex] = f(x) in [itex]\Re[/itex][itex]^{n}[/itex]. There exists a bounded 2D invariant manifold M for this system. There are no critical points in M. Does it follow that there is a periodic orbit in M?

No, as for example if [itex]M = S^1 \times S^1[/itex] (the 2-torus) and the reduction of the system on [itex]M[/itex] is (after rescaling time)
[tex] (\dot \theta_1, \dot \theta_2) = (1, \alpha)[/tex]
with irrational [itex]\alpha[/itex]. All trajectories are then dense in [itex]M[/itex], and there are no periodic orbits.

I've realized that this has it's similarities to Poincare-Bendixon's theorem but I don't believe that it holds for a system in n dimensions. Would I be correct in thinking that even with the strict conditions above we could end up with chaos?

No: three dimensions are necessary for chaos, so the behaviour of the system on M cannot be chaotic.
 

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