Mathematical Theory and Applications ›› 2024, Vol. 44 ›› Issue (4): 45-69.doi: 10.3969/j.issn.1006-8074.2024.04.004

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Bounded and Unbounded Solutions of the SD Oscillator at Resonance

Bian Jingke, Liu Jie*   

  1. School of Mathematics and Information Science, Henan Polytechnic University, Jiaozuo 454003, China
  • Online:2024-12-28 Published:2025-01-21
  • Contact: Liu Jie
  • Supported by:

    The work is supported by the Key Research Funds for the Universities of Henan Province (No. 19A110018), and the Foundation

    for Key Teachers of Henan Polytechnic University (No. 2022XQG-09)

Abstract:

In this paper we study the boundedness and unboundedness of the solutions of the smooth and discontinuous (SD) oscillator

\begin{equation*}

x''+f(x)x'+x-\frac{x}{\sqrt{x^{2}+\alpha^{2}}}=p(t).

\end{equation*}

Since $f(x)\neq 0$, the system is non-Hamiltonian, so we have to introduce some reversibility assumptions to apply a suitable twist theorem, for reversible maps with small twist. Moreover, when the nonnegative parameter $\alpha$ decreases to 0, the system becomes discontinuous. In this case, we need to introduce some suitable transformations to overcome the lack of regularity. We will prove that for any nonnegative parameter $\alpha$, when $p(t)$ is an odd periodic function satisfying $\left|\int^{2\pi}_{0}p(t)\sin t\,\dif\,t\right|<4$, all the solutions are bounded; when $p(t)$ satisfies $\left|\int^{2\pi}_{0}p(t)\sin t\,\dif\,t\right|>4$, the SD oscillator has unbounded solutions, and when $p(t)$ satisfies $\left|\int^{2\pi}_{0}p(t)\sin t\,\dif\,t\right|\geqslant 4+|F|_{\infty}$, all the solutions are unbounded.

Key words: SD oscillator, Reversible system, Bounded solution, Unbounded solution