Univ Lyon, INSA Lyon, Ecole Centrale de Lyon, Université Claude Bernard Lyon I, CNRS, LMFA, UMR 5509, F-69621 Villeurbanne, France.
Univ Lyon, Université Lyon 1, Centre Léon Bérard, INSERM, LabTAU, F-69003 Lyon, France.
Phys Rev E. 2019 Sep;100(3-1):033104. doi: 10.1103/PhysRevE.100.033104.
A theory is developed that allows one to model the velocity field of acoustic microstreaming produced by nonspherical oscillations of an acoustically driven gas bubble. It is assumed that some of the bubble oscillation modes are excited parametrically and hence can oscillate at frequencies different from the driving frequency. Analytical solutions are derived in terms of complex amplitudes of oscillation modes, which means that the mode amplitudes are assumed to be known and serve as input data when the velocity field of acoustic microstreaming is calculated. No restrictions are imposed on the ratio of the bubble radius to the viscous penetration depth. The present paper is the first part of our study in which a general theory is developed and then applied to the case that acoustic microstreaming is generated by the interaction of the breathing mode (mode 0) with a mode of arbitrary order m≥1. Examples of numerical simulations and a comparison with experimental results are provided.
本文提出了一种理论,用于对受激气泡非球形振动所产生的声微流速度场进行建模。假设某些气泡振动模式通过参激方式被激发,因此它们可以以不同于激励频率的频率进行振动。通过振荡模式的复振幅导出了解析解,这意味着在计算声微流速度场时,假定模式振幅已知,并且作为输入数据。本文对气泡半径与粘性穿透深度的比值没有限制。本文是我们研究的第一部分,在这部分中,我们发展了一种通用理论,并将其应用于由呼吸模式(模式 0)与任意阶 m≥1 的模式相互作用产生声微流的情况。提供了数值模拟的示例,并与实验结果进行了比较。