Abstract
This paper estimates a new ultimate bound set (UBS) for the chaotic system caused by the interaction of the whistler and ion-acoustic waves with the plasma oscillation. The intrinsic Hamilton energy is estimated by using the Helmholtz theorem, and this kind of energy function is the most suitable Lyapunov function to discern its dynamic stability. It is found that the Hamilton energy is relative to the firing states of the dynamical system. In a stable state, the energy is also a constant, while a chaotic state is resulting from an oscillation in the energy. We use the Lagrange coefficient method to solve an optimization problem analytically so that we can find an accurate UBS for the plasma chaotic system. Further, we present the competitive modes (CMs) for the plasma system to investigate its different dynamical behaviors for different parameters. Simulation results for CMs confirm the theories presented about the Hamilton energy function and UBS.
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Acknowledgements
The First author is supported by the National Natural Science Foundation of China (11601525). The second author extends her appreciation to the Al Mustaqbal University college for supporting this work for grant number (MUC-E\(_0\)122).
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He, F., Abdullah, Z.K., Saberi-Nik, H. et al. The bounded sets, Hamilton energy, and competitive modes for the chaotic plasma system. Nonlinear Dyn 111, 4847–4862 (2023). https://doi.org/10.1007/s11071-022-08098-8
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DOI: https://doi.org/10.1007/s11071-022-08098-8