Sojahrood A J, Li Q, Haghi H, Karshafian R, Porter T M, Kolios M C
Department of Physics, Toronto Metropolitan 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 Biomedical Engineering, Boston University, Boston, MA, USA.
Ultrason Sonochem. 2023 May;95:106319. doi: 10.1016/j.ultsonch.2023.106319. Epub 2023 Feb 6.
The problem of attenuation and sound speed of bubbly media has remained partially unsolved. Comprehensive data regarding pressure-dependent changes of the attenuation and sound speed of a bubbly medium are not available. Our theoretical understanding of the problem is limited to linear or semi-linear theoretical models, which are not accurate in the regime of large amplitude bubble oscillations. Here, by controlling the size of the lipid coated bubbles (mean diameter of ≈5.4μm), we report the first time observation and characterization of the simultaneous pressure dependence of sound speed and attenuation in bubbly water below, at and above microbubbles resonance (frequency range between 1-3 MHz). With increasing acoustic pressure (between 12.5-100 kPa), the frequency of the peak attenuation and sound speed decreases while maximum and minimum amplitudes of the sound speed increase. We propose a nonlinear model for the estimation of the pressure dependent sound speed and attenuation with good agreement with the experiments. The model calculations are validated by comparing with the linear and semi-linear models predictions. One of the major challenges of the previously developed models is the significant overestimation of the attenuation at the bubble resonance at higher void fractions (e.g. 0.005). We addressed this problem by incorporating bubble-bubble interactions and comparing the results to experiments. Influence of the bubble-bubble interactions increases with increasing pressure. Within the examined exposure parameters, we numerically show that, even for low void fractions (e.g. 5.1×10) with increasing pressure the sound speed may become 4 times higher than the sound speed in the non-bubbly medium.
气泡介质的衰减和声速问题仍有部分未解决。关于气泡介质衰减和声速随压力变化的综合数据尚不完整。我们对该问题的理论理解仅限于线性或半线性理论模型,这些模型在大振幅气泡振荡区域并不准确。在此,通过控制脂质包裹气泡的大小(平均直径约为5.4μm),我们首次观察并表征了在微气泡共振以下、共振时及共振以上的气泡水中声速和衰减随压力的同时变化(频率范围在1 - 3MHz之间)。随着声压增加(在12.5 - 100kPa之间),峰值衰减和声速的频率降低,而声速的最大和最小幅度增加。我们提出了一个非线性模型来估计随压力变化的声速和衰减,该模型与实验结果吻合良好。通过与线性和半线性模型的预测结果进行比较,验证了模型计算的正确性。先前开发的模型的主要挑战之一是在较高空隙率(例如0.005)下,对气泡共振时的衰减有显著高估。我们通过纳入气泡 - 气泡相互作用并将结果与实验进行比较来解决这个问题。气泡 - 气泡相互作用的影响随着压力增加而增大。在研究的暴露参数范围内,我们通过数值计算表明,即使对于低空隙率(例如5.1×10),随着压力增加,声速可能比非气泡介质中的声速高出4倍。