Sojahrood A J, Wegierak D, Haghi H, Karshfian R, Kolios Michael C
Department of Physics, Ryerson University, Toronto, Canada; Institute for Biomedical Engineering, Science and Technology (IBEST) a partnership between Ryerson University and St. Mike's Hospital, Toronto, Ontario, Canada.
Department of Physics, Ryerson University, Toronto, Canada; Institute for Biomedical Engineering, Science and Technology (IBEST) a partnership between Ryerson University and St. Mike's Hospital, Toronto, Ontario, Canada.
Ultrason Sonochem. 2019 Jun;54:99-109. doi: 10.1016/j.ultsonch.2019.02.010. Epub 2019 Feb 13.
The bubble oscillator is a highly nonlinear system, which makes it difficult to generate a comprehensive understanding of its oscillatory behavior. One method used to investigate such complex dynamical systems is the bifurcation analysis. Numerous investigations have employed the method of bifurcation diagrams to study the effect of different control parameters on the bubble behavior. These studies, however, focused mainly on investigating the subharmonic (SH) and chaotic oscillations of the bubbles. Super-harmonic (SuH) and ultra-harmonic (UH) bubble oscillations remain under-investigated. One reason is that the conventional method used for generating bifurcation diagrams cannot reliably identify features that are responsible for the identification of SuH and UH oscillations. Additionally, the conventional method cannot distinguish between the UHs and SHs. We introduce a simple procedure to address this shortcoming. In this method, the maxima of the bubble oscillatory response were selected and plotted alongside the traditional bifurcation points for the corresponding control parameter. Results show that depending on the control parameters the conventional method or the method of maxima may miss intricate details of the oscillations. In order to have a comprehensive knowledge on the rich dynamics of the system, the two methods should be employed side by side. Through plotting the two bifurcation structures in tandem, the oscillatory behavior of the bubble was analyzed with more detail, and stable SuH and UH bubble oscillations were investigated. Based on this new analysis, the conditions for the generation and amplification of UH and SuH regimes are discussed.
气泡振荡器是一个高度非线性系统,这使得全面理解其振荡行为变得困难。用于研究此类复杂动力系统的一种方法是分岔分析。许多研究采用分岔图方法来研究不同控制参数对气泡行为的影响。然而,这些研究主要集中在研究气泡的亚谐波(SH)和混沌振荡。超谐波(SuH)和超高频(UH)气泡振荡仍未得到充分研究。一个原因是用于生成分岔图的传统方法无法可靠地识别导致SuH和UH振荡识别的特征。此外,传统方法无法区分UH和SH。我们引入了一个简单的程序来解决这一缺点。在该方法中,选择气泡振荡响应的最大值,并与相应控制参数的传统分岔点一起绘制。结果表明,根据控制参数的不同,传统方法或最大值方法可能会遗漏振荡的复杂细节。为了全面了解系统丰富的动力学特性,应同时采用这两种方法。通过串联绘制两种分岔结构,更详细地分析了气泡的振荡行为,并研究了稳定的SuH和UH气泡振荡。基于这一新的分析,讨论了UH和SuH状态产生和放大的条件。