参数共振频率响应分析与振动稳定

Karthik Chikmagalur, Bassam Bamieh
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引用次数: 2

摘要

从流体动力学、结构和MEMS器件到量子力学和天体物理学,在自然界和工程系统中都发现了周期性时变模型。已知这样的系统表现出参数共振,这是一种由模型参数波动引起的不稳定性。在不稳定的条件下,它们也可以通过适当的力来实现振动稳定。这里感兴趣的问题是在这两种稳定状态下的行为变化,以及从设计的角度来看,某些参数配置是否更可取。这一动机使我们把带调和强迫的马蒂厄方程看作一个典型模型。为了解决这些问题,我们使用基于提升的方法来获得频率响应算子的表示,该表示适用于LTI系统的方法。研究了系统的极点作为系统参数的函数,得到了Mathieu方程的自由响应作为两个简单函数乘积的描述。研究了Mathieu方程的${\mathcal{H}_2}$范数对其参数的依赖性。我们发现了两种模式之间${\mathcal{H}_2}$范数的显著差异,以及每个域内有趣的行为。
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Frequency Response Analysis of Parametric Resonance and Vibrational Stabilization
Periodically time-varying models are found across nature and engineered systems, from fluid dynamics, structures and MEMS devices to quantum mechanics and astrophysics. Such systems are known to exhibit parametric resonance, a kind of instability caused by fluctuating model parameters. Under conditions of instability, they can also be vibrationally stabilized with the right forcing. The question of interest here is variation in behavior within these two stable regimes, and whether certain parameter configurations are preferred from a design perspective. This motivation leads us to consider Mathieu’s equation with harmonic forcing as a canonical model. To address these questions, we use a lifting based approach to obtain a representation of the frequency response operator that is amenable to methods from LTI systems. We study the poles of the system as a function of its parameters, and obtain a description of the free response of Mathieu’s equation as the product of two simple functions. We also investigate the dependence of the ${\mathcal{H}_2}$ norm of Mathieu’s equation on its parameters. A considerable difference in ${\mathcal{H}_2}$ norm between the two regimes is found, as well as interesting behavior within each domain.
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