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基于气泡群动力学的水和粘弹性介质中空化阈值的数值模拟。

Numerical simulation of cavitation threshold in water and viscoelastic medium based on bubble cluster dynamics.

作者信息

Shen Xiaozhuo, Wu Pengfei, Lin Weijun

机构信息

State Key Laboratory of Acoustics, Institute of Acoustics and Marine Information, Chinese Academy of Sciences, Beijing 100190, China; University of Chinese Academy of Sciences, Beijing 100049, China.

State Key Laboratory of Acoustics, Institute of Acoustics and Marine Information, Chinese Academy of Sciences, Beijing 100190, China; University of Chinese Academy of Sciences, Beijing 100049, China.

出版信息

Ultrason Sonochem. 2025 Aug;119:107414. doi: 10.1016/j.ultsonch.2025.107414. Epub 2025 Jun 2.


DOI:10.1016/j.ultsonch.2025.107414
PMID:40479980
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12171623/
Abstract

The ultrasonic cavitation threshold is a significant area of research in therapeutic ultrasound. This study conducts a numerical simulation of the ultrasound cavitation threshold by solving the dynamic equations of bubble clusters composed of bubbles with varying sizes. The effects of different criteria for cavitation threshold, bubble dynamics models, medium types, viscoelasticity and number of bubbles on the cavitation threshold are analyzed. Moreover, a comparison is made between calculation outcomes and those from previous experimental research. The results show that the relationship between the cavitation threshold P and frequency f can be expressed as P = Af + B, where A, B and α depend on the properties of the medium and different criteria of cavitation threshold. As the number of bubbles increases, the cavitation threshold initially rises and then falls, indicating a non-monotonic trend. Furthermore, the influence of the medium's shear modulus on the cavitation threshold is more intricate, and the cavitation threshold in viscoelastic medium is not consistently higher than that in water. Among all parameters in this study, the cavitation threshold is more sensitive to the change of frequency.

摘要

超声空化阈值是治疗超声研究的一个重要领域。本研究通过求解由不同尺寸气泡组成的气泡簇的动力学方程,对超声空化阈值进行了数值模拟。分析了不同空化阈值判据、气泡动力学模型、介质类型、粘弹性和气泡数量对空化阈值的影响。此外,还将计算结果与以往实验研究结果进行了比较。结果表明,空化阈值P与频率f之间的关系可表示为P = Af + B,其中A、B和α取决于介质的性质和不同的空化阈值判据。随着气泡数量的增加,空化阈值先升高后降低,呈现非单调趋势。此外,介质剪切模量对空化阈值的影响更为复杂,粘弹性介质中的空化阈值并不总是高于水中的空化阈值。在本研究的所有参数中,空化阈值对频率变化更为敏感。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/7f8539b77689/gr14.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/a781d807b8af/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/44b06b197c10/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/41682b7a76ea/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/90b875ca6039/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/bdde24752fd4/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/16102a865831/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/4f2a4f9d4059/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/8f463adec10f/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/98828422db55/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/6f669b80adc3/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/7c6a896ee184/gr11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/a0a4c8be3a95/gr12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/99b30650cbd2/gr13.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/7f8539b77689/gr14.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/a781d807b8af/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/44b06b197c10/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/41682b7a76ea/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/90b875ca6039/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/bdde24752fd4/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/16102a865831/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/4f2a4f9d4059/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/8f463adec10f/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/98828422db55/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/6f669b80adc3/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/7c6a896ee184/gr11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/a0a4c8be3a95/gr12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/99b30650cbd2/gr13.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3dc4/12171623/7f8539b77689/gr14.jpg

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本文引用的文献

[1]
Evolutionary mechanism of Y-branches in acoustic Lichtenberg figures just below the water surface.

J Acoust Soc Am. 2024-11-1

[2]
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Ultrason Sonochem. 2024-11

[3]
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[4]
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Ultrason Sonochem. 2024-10

[5]
A new model for bubble cluster dynamics in a viscoelastic media.

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[6]
Mechanism study of aging oil demulsification and dehydration under ultrasonic irradiation.

Ultrason Sonochem. 2024-5

[7]
Histotripsy: A Method for Mechanical Tissue Ablation with Ultrasound.

Annu Rev Biomed Eng. 2024-7

[8]
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Food Res Int. 2023-12

[9]
Bubble pulsation characteristics in multi-bubble systems affected by bubble size polydispersity and spatial structure.

Ultrasonics. 2023-9

[10]
Study on the real-time variation laws and mechanism of oil sample viscosity during ultrasonic irradiation.

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