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Cavitation bubble structures below a soft boundary in an ultrasonic field

We studied the layer structure of bubbles just below water/air and water/EPE (Expand aple poly ephylene) interfaces using high-speed photography. The layer structure was generated by floating spherical clusters, the source bubbles of which were identified to come from the attachment of bubble nuclei...

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Autores principales: Li, Fan, Huang, Chenyang, Zhang, Xianmei, Wang, Chenghui, Hu, Jing, Chen, Shi, Tian, Hua, Shen, Zhuangzhi, Guo, Jianzhong, Lin, Shuyu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Elsevier 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10345162/
https://www.ncbi.nlm.nih.gov/pubmed/37413916
http://dx.doi.org/10.1016/j.ultsonch.2023.106500
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author Li, Fan
Huang, Chenyang
Zhang, Xianmei
Wang, Chenghui
Hu, Jing
Chen, Shi
Tian, Hua
Shen, Zhuangzhi
Guo, Jianzhong
Lin, Shuyu
author_facet Li, Fan
Huang, Chenyang
Zhang, Xianmei
Wang, Chenghui
Hu, Jing
Chen, Shi
Tian, Hua
Shen, Zhuangzhi
Guo, Jianzhong
Lin, Shuyu
author_sort Li, Fan
collection PubMed
description We studied the layer structure of bubbles just below water/air and water/EPE (Expand aple poly ephylene) interfaces using high-speed photography. The layer structure was generated by floating spherical clusters, the source bubbles of which were identified to come from the attachment of bubble nuclei at the interface, the floating of bubbles in the bulk liquid, or bubbles generated on the surface of the ultrasonic transducer. The boundary shape affected the layer structure, which assumed a similar profile below the water/EPE interface. We developed a simplified model composed of a bubble column and bubble chain to describe interface impacts and the interaction of bubbles in a typical branching structure. We found that the resonant frequency of the bubbles is smaller than that of an isolated single bubble. Moreover, the primary acoustic field plays an important role in the generation of the structure. A higher acoustic frequency and pressure were found to shorten the distance between the structure and the interface. A hat-like layer structure of bubbles was more likely to exist in the low-frequency (28 and 40 kHz) intense inertial cavitation field, in which bubbles oscillate violently. By contrast, structures composed of discrete spherical clusters were more likely to form in the relatively weak cavitation field at 80 kHz, in which stable and inertial cavitation coexisted. The theoretical predictions were in good agreement with the experimental observations.
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spelling pubmed-103451622023-07-15 Cavitation bubble structures below a soft boundary in an ultrasonic field Li, Fan Huang, Chenyang Zhang, Xianmei Wang, Chenghui Hu, Jing Chen, Shi Tian, Hua Shen, Zhuangzhi Guo, Jianzhong Lin, Shuyu Ultrason Sonochem UC and HC intensification We studied the layer structure of bubbles just below water/air and water/EPE (Expand aple poly ephylene) interfaces using high-speed photography. The layer structure was generated by floating spherical clusters, the source bubbles of which were identified to come from the attachment of bubble nuclei at the interface, the floating of bubbles in the bulk liquid, or bubbles generated on the surface of the ultrasonic transducer. The boundary shape affected the layer structure, which assumed a similar profile below the water/EPE interface. We developed a simplified model composed of a bubble column and bubble chain to describe interface impacts and the interaction of bubbles in a typical branching structure. We found that the resonant frequency of the bubbles is smaller than that of an isolated single bubble. Moreover, the primary acoustic field plays an important role in the generation of the structure. A higher acoustic frequency and pressure were found to shorten the distance between the structure and the interface. A hat-like layer structure of bubbles was more likely to exist in the low-frequency (28 and 40 kHz) intense inertial cavitation field, in which bubbles oscillate violently. By contrast, structures composed of discrete spherical clusters were more likely to form in the relatively weak cavitation field at 80 kHz, in which stable and inertial cavitation coexisted. The theoretical predictions were in good agreement with the experimental observations. Elsevier 2023-06-23 /pmc/articles/PMC10345162/ /pubmed/37413916 http://dx.doi.org/10.1016/j.ultsonch.2023.106500 Text en © 2023 The Author(s) https://creativecommons.org/licenses/by-nc-nd/4.0/This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle UC and HC intensification
Li, Fan
Huang, Chenyang
Zhang, Xianmei
Wang, Chenghui
Hu, Jing
Chen, Shi
Tian, Hua
Shen, Zhuangzhi
Guo, Jianzhong
Lin, Shuyu
Cavitation bubble structures below a soft boundary in an ultrasonic field
title Cavitation bubble structures below a soft boundary in an ultrasonic field
title_full Cavitation bubble structures below a soft boundary in an ultrasonic field
title_fullStr Cavitation bubble structures below a soft boundary in an ultrasonic field
title_full_unstemmed Cavitation bubble structures below a soft boundary in an ultrasonic field
title_short Cavitation bubble structures below a soft boundary in an ultrasonic field
title_sort cavitation bubble structures below a soft boundary in an ultrasonic field
topic UC and HC intensification
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10345162/
https://www.ncbi.nlm.nih.gov/pubmed/37413916
http://dx.doi.org/10.1016/j.ultsonch.2023.106500
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