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声泡簇的光学产生与持续存在。

Optic generation and perpetuation of acoustic bubble clusters.

作者信息

Mur Jaka, Reuter Fabian, Agrež Vid, Petkovšek Rok, Ohl Claus-Dieter

机构信息

Faculty of Natural Sciences, Institute for Physics, Otto-von-Guericke-University Magdeburg, Universitätsplatz 2, 39106 Magdeburg, Germany; Faculty of Mechanical Engineering, University of Ljubljana, Aškerčeva 6, SI-1000 Ljubljana, Slovenia.

Faculty of Natural Sciences, Institute for Physics, Otto-von-Guericke-University Magdeburg, Universitätsplatz 2, 39106 Magdeburg, Germany.

出版信息

Ultrason Sonochem. 2024 Nov;110:107023. doi: 10.1016/j.ultsonch.2024.107023. Epub 2024 Aug 15.

DOI:10.1016/j.ultsonch.2024.107023
PMID:39153420
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11378257/
Abstract

Laser-induced cavitation bubbles offer precise control of the flow in space and time, but they are rarely used for the mechanical and chemical processing of liquids. Instead, strong acoustic fields are commonly used to nucleate and drive cavitation bubbles for liquid process applications. While acoustic field creates many more cavitation events, the resulting chaotic dynamics offers little control on the fluid mechanics, i.e., where and how bubbles deliver their energy. Here we present a method that utilizes a laser to nucleate a single cavitation bubble, which is then driven into violent oscillations by the ultrasound field, resulting in splitting of the bubble followed by formation of a cluster of cavitation bubbles. This combination offers means for cavitation control not available in conventional acoustic cavitation. Here, the cavitation bubble is generated with a custom build pulsed laser that is focused below a sonotrode driven at 20 kHz. In absence of the acoustic driving the bubble reaches a maximum diameter of 130 µm with a lifetime of approximately 10 µs. In the presence of the acoustic field the first few expansions and bubble collapses are strongly affected by the phase of nucleation. Over successive acoustic cycles a small bubble cluster develops that loses its connection with the phase of generation. We study the dynamics in the free field and constrained by a rigid boundary. For both geometries the cluster over many acoustic cycles dies off, yet through repetitive optical bubble seeding the cluster lifetime and its location can be controlled.

摘要

激光诱导的空化泡能在空间和时间上实现对流体流动的精确控制,但它们很少用于液体的机械和化学处理。相反,强声场通常用于引发和驱动空化泡以用于液体处理应用。虽然声场会产生更多的空化事件,但由此产生的混沌动力学对流体力学几乎没有控制作用,即气泡在何处以及如何传递其能量。在此,我们提出一种方法,该方法利用激光引发单个空化泡,然后该空化泡被超声场驱动至剧烈振荡,导致气泡分裂,随后形成一群空化泡。这种组合提供了传统声空化中所没有的空化控制手段。在此,空化泡由定制的脉冲激光产生,该激光聚焦在以20kHz驱动的超声换能器下方。在没有声驱动的情况下,气泡达到最大直径130μm,寿命约为10μs。在声场存在的情况下,最初的几次膨胀和气泡坍塌受到成核相位的强烈影响。在连续的声循环中,会形成一个小气泡群,该气泡群与产生相位失去联系。我们研究了在自由场以及受刚性边界约束情况下的动力学。对于这两种几何形状,经过许多声循环后气泡群都会消失,但通过重复的光学气泡播种,可以控制气泡群的寿命及其位置。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/dd444ed0f1b6/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/b73892d3337b/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/f41cfc381de8/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/1f2a4adf586a/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/940bb0231f8f/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/8b00747c0468/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/a29ac4bcb14a/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/dd444ed0f1b6/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/b73892d3337b/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/f41cfc381de8/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/1f2a4adf586a/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/940bb0231f8f/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/8b00747c0468/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/a29ac4bcb14a/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5cbc/11378257/dd444ed0f1b6/gr7.jpg

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