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arXiv 2602.22797math.DSnlin.CD
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共振滑动分岔重新审视

Resonant grazing bifurcations revisited

School of Mathematical and Computational Sciences, Massey University(梅西大学数学与计算科学学院);School of Mathematics and Statistics, University College Dublin(都柏林大学学院数学与统计学院)

David J. W. Simpson, Indranil Ghosh

AI总结:

本文研究了共振条件下滑动分岔的二次切点特性,通过修改Poincaré映射消除平方根奇点,推导了鞍点和倍周期分岔曲线的二次系数,并解释了实验中滑动分岔后无混沌现象的原因。

摘要:

在振动冲击力学中,冲击与近似擦碰之间的分界是一个零速度滑动事件。稳定周期运动的滑动分岔通常会在滑动产生Poincaré映射中的平方根项时产生复杂的吸引子。本文关注的是当平方根项在某些迭代中消失的二维情形。对于受迫单自由度振子,当激励频率是阻尼自然频率的某个有理数倍时,即系统处于共振状态。在双参数分岔图中,单冲击周期运动的鞍点分岔和倍周期分岔曲线从二维点出发。本文证明这些曲线与滑动分岔曲线二次相切,并推导出其二次系数的显式公式。这通过修改Poincaré映射以绕过平方根奇点,从而能够使用隐函数定理来证明光滑性,并进行鞍点分岔和倍周期分岔曲线的渐近计算。在此过程中,我们通过补充渐近计算的几何和拓扑论证,解决了长期存在的关于单冲击周期运动可接受性的猜想。我们通过线性冲击振子模型进行说明,将理论展开与数值计算的分岔曲线匹配。结果解释了之前报告的物理实验为何在滑动分岔之后不久没有出现混沌。

英文摘要:

In vibro-impact mechanics, the division between an impact and a near miss is a zero-velocity grazing event. Grazing bifurcations of stable periodic motions often produce complicated attractors when grazing generates a square-root term in the Poincaré map. This paper concerns codimension-two scenarios for which the square-root term vanishes in some iterate of the Poincaré map. For forced one-degree-of-freedom oscillators, this occurs when the forcing frequency is a certain rational multiple of the damped natural frequency, i.e., the system is in resonance. In two-parameter bifurcation diagrams, curves of saddle-node and period-doubling bifurcations of single-impact periodic motions emanate from the codimension-two points. In this paper we prove these curves are quadratically tangent to the curve of grazing bifurcations, and derive explicit formulas for their quadratic coefficients. This is achieved by modifying the Poincaré map in a way that circumvents the square-root singularity, enabling us to use the implicit function theorem to demonstrate smoothness and perform asymptotic calculations of the saddle-node and period-doubling bifurcation curves. In doing so we resolve a long-standing conjecture on the admissibility of single-impact periodic motions by supplementing raw asymptotic computations with geometric and topological arguments. We illustrate the results with a linear impact oscillator model, matching the theoretical unfolding to numerically computed bifurcation curves. The results explain why previously reported physical experiments reveal an absence of chaos shortly past the grazing bifurcation.

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