截断旋转非线性浅水模型中的混沌与共振三元相互作用之路

Francesco Carbone, Denys Dutykh
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引用次数: 0

摘要

我们利用一个具有复杂变量的五模 Galerkin 截断系统,对旋转浅水模型中的混沌和相态动力学路线进行了理论研究。该系统对于研究大尺度/介质尺度如何失稳并演变为混沌非常有价值。随着能级的增加,确定了两种不同的混沌行为过渡。最初的过渡是按照费根鲍姆序列通过分岔发生的。随后的过渡,在更高的能级上,显示了从准周期状态到混沌状态的转变。第一种混沌状态主要是由非线性相互作用的惯性力引起的。第二种混沌状态是由于自由表面升高在动力学中的重要性增加。对每个截断变量使用相位和振幅表示法进行新的重构后发现,相位分量表现出时间上的片断锁定行为,在$\pm\pi$中断转换前的较长时间内保持恒定值,而振幅则保持混沌状态。据观察,相位稳定持续时间随着能量的增加而减少,导致相位分量在高能量水平上出现混沌。这归因于方程中的非线性项,其中相位分量是通过具有不同模式的三元组的线性组合引入的。当锁定持续时间在不同模式间变化时,动力学会导致多个$/pi$相移的随机相互作用,从而在耦合相位三元组内产生随机动力学,即使在注入最小能量时也能观察到。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Route to chaos and resonant triads interaction in a truncated Rotating Nonlinear shallow-water model
The route to chaos and phase dynamics in a rotating shallow-water model were rigorously examined using a five-mode Galerkin truncated system with complex variables. This system is valuable for investigating how large/meso-scales destabilize and evolve into chaos. Two distinct transitions into chaotic behaviour were identified as energy levels increased. The initial transition occurs through bifurcations following the Feigenbaum sequence. The subsequent transition, at higher energy levels, shows a shift from quasi-periodic states to chaotic regimes. The first chaotic state is mainly due to inertial forces governing nonlinear interactions. The second chaotic state arises from the increased significance of free surface elevation in the dynamics. A novel reformulation using phase and amplitude representations for each truncated variable revealed that phase components exhibit a temporal piece-wise locking behaviour, maintaining a constant value for a prolonged interval before an abrupt transition of $\pm\pi$, while amplitudes remain chaotic. It was observed that phase stability duration decreases with increased energy, leading to chaos in phase components at high energy levels. This is attributed to the nonlinear term in the equations, where phase components are introduced through linear combinations of triads with different modes. When locking durations vary across modes, the dynamics result in a stochastic interplay of multiple $\pi$ phase shifts, creating a stochastic dynamic within the coupled phase triads, observable even at minimal energy injections.
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