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本文引用的文献

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Dynamics of tandem bubble interaction in a microfluidic channel.微流道中串联气泡相互作用的动力学。
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2
The inertial terms in equations of motion for bubbles in tubular vessels or between plates.管内或板间气泡运动方程中的惯性项。
J Acoust Soc Am. 2011 Nov;130(5):3333-8. doi: 10.1121/1.3638132.
3
Pulsating tandem microbubble for localized and directional single-cell membrane poration.脉动串联微泡用于局部化和定向的单细胞细胞膜穿孔。
Phys Rev Lett. 2010 Aug 13;105(7):078101. doi: 10.1103/PhysRevLett.105.078101. Epub 2010 Aug 9.
4
Cavitation bubble dynamics in microfluidic gaps of variable height.可变高度微流体间隙中的空化泡动力学
Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Oct;80(4 Pt 2):047301. doi: 10.1103/PhysRevE.80.047301. Epub 2009 Oct 6.
5
A millisecond micromixer via single-bubble-based acoustic streaming.一种基于单气泡声流的毫秒级微混合器。
Lab Chip. 2009 Sep 21;9(18):2738-41. doi: 10.1039/b903687c. Epub 2009 Jun 23.
6
Controlled cavitation in microfluidic systems.微流体系统中的可控空化
Phys Rev Lett. 2007 Jun 22;98(25):254501. doi: 10.1103/PhysRevLett.98.254501. Epub 2007 Jun 19.
7
Bubble pulsations between parallel plates.平行板间的气泡脉动
J Acoust Soc Am. 2006 Apr;119(4):2067-72. doi: 10.1121/1.2172545.
8
Impact on soft sand: void collapse and jet formation.对软砂的影响:孔洞坍塌与射流形成。
Phys Rev Lett. 2004 Nov 5;93(19):198003. doi: 10.1103/PhysRevLett.93.198003. Epub 2004 Nov 3.

圆柱形气泡脉动模型。

Models of cylindrical bubble pulsation.

机构信息

Applied Research Laboratories, University of Texas at Austin, Austin, Texas 78713-8029, USA.

出版信息

J Acoust Soc Am. 2012 Sep;132(3):1346-57. doi: 10.1121/1.4730888.

DOI:10.1121/1.4730888
PMID:22978863
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3460979/
Abstract

Three models are considered for describing the dynamics of a pulsating cylindrical bubble. A linear solution is derived for a cylindrical bubble in an infinite compressible liquid. The solution accounts for losses due to viscosity, heat conduction, and acoustic radiation. It reveals that radiation is the dominant loss mechanism, and that it is 22 times greater than for a spherical bubble of the same radius. The predicted resonance frequency provides a basis of comparison for limiting forms of other models. The second model considered is a commonly used equation in Rayleigh-Plesset form that requires an incompressible liquid to be finite in extent in order for bubble pulsation to occur. The radial extent of the liquid becomes a fitting parameter, and it is found that considerably different values of the parameter are required for modeling inertial motion versus acoustical oscillations. The third model was developed by V. K. Kedrinskii [Hydrodynamics of Explosion (Springer, New York, 2005), pp. 23-26] in the form of the Gilmore equation for compressible liquids of infinite extent. While the correct resonance frequency and loss factor are not recovered from this model in the linear approximation, it provides reasonable agreement with observations of inertial motion.

摘要

考虑了三种模型来描述脉动圆柱气泡的动力学。推导了无限可压缩液体中圆柱气泡的线性解。该解考虑了由于粘性、热传导和声波辐射引起的损失。结果表明,辐射是主要的损失机制,比相同半径的球形气泡大 22 倍。预测的共振频率为其他模型的限制形式提供了比较基础。考虑的第二种模型是常用的瑞利-普莱塞特形式的方程,要求不可压缩液体在有限范围内才能发生气泡脉动。液体的径向范围成为一个拟合参数,结果发现,对于模拟惯性运动与声振动,需要使用非常不同的参数值。第三种模型是由 V. K. Kedrinskii 以无限可压缩液体的吉尔莫方程的形式发展起来的[爆炸动力学(Springer,纽约,2005 年),第 23-26 页]。在这个模型中,在线性近似下,无法从该模型中恢复出正确的共振频率和损耗因子,但它与惯性运动的观测结果吻合较好。