Abstract

This paper reports a new bifurcation pattern observed in a Lorenz-type system. The pattern is composed of a main bifurcation route to chaos (n=1) and a sequence of sub-bifurcation routes with n=3,4,5,…,14 isolated sub-branches to chaos. When n is odd, the n isolated sub-branches are from a period-n limit cycle, followed by twin period-n limit cycles via a pitchfork bifurcation, twin chaotic attractors via period-doubling bifurcations, and a symmetric chaotic attractor via boundary crisis. When n is even, the n isolated sub-branches are from twin period-n/2 limit cycles, which become twin chaotic attractors via period-doubling bifurcations. The paper also shows that the main route and the sub-routes can coexist peacefully by studying basins of attraction.

Highlights

  • Nonlinear phenomena in physics and engineering are o en described by quadratic systems, such as the famous Lorenz system [1], the Nose-Hoover equations [2, 3], the brushless DC motor system [4], the pendulum system [5], etc

  • The isolated sub-branches are from a period- limit cycle, otherwise the sub-branches are from twin period-푛/2 limit cycles

  • E detailed bifurcations are shown in Figure 1(b), which all follows the known pattern: When is odd, like the branch-3 shown in Figure 5, the sub-branches first start with a periodlimit cycle introduced by a fold bifurcation, bifurcate into a pair of twin limit cycles with the same period, a er that the twin cycles become a pair of twin chaotic attractors via period doubling bifurcations, at last the twin chaotic attractors merge into one larger chaotic attractor

Read more

Summary

Introduction

Nonlinear phenomena in physics and engineering are o en described by quadratic systems, such as the famous Lorenz system [1], the Nose-Hoover equations [2, 3], the brushless DC motor system [4], the pendulum system [5], etc. The period of the initial limit cycle increases with step size 1, the pattern is different from the period-adding phenomena reported in [24,25,26] since there is no parameter overlap between these branches and the period-doubling and period-adding happen in different parameter-changing directions For this phenomenon, the maximal found is 7, and the systems are all nonsymmetrical. The isolated sub-branches are from a period- limit cycle, otherwise the sub-branches are from twin period-푛/2 limit cycles All these branches lead to chaos as a parameter increases, this pattern is completely different (see Figure 1) from the existing literature, according to the best of the authors’ knowledge. E rest of paper is organized as follows: Section 2 introduces the Lorenz-type system, studies its symmetry, equilibria and their stability, and briefly explores the nonlinear dynamics; Section 3 carries out detailed numerical research on the sequence of bifurcation branches; Section 4 draws the conclusion

The Lorenz Type System e Lorenz type system is given by following equations:
Sequence of Routes to Chaos
Connections with Periodic Windows of the Main
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call