Acoustic cavitation: the fluid dynamics of non–spherical bubbles

In acoustic cavitation the spatial variation and time-dependent nature of the acoustic pressure field, whether it is a standing or propagating wave, together with the presence of other bubbles, particles and boundaries produces gradients and asymmetries in the flow field. This will inevitably lead t...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences physical, and engineering sciences, 1999-02, Vol.357 (1751), p.251-267
Hauptverfasser: Blake, J. R., Blake, John R., Keen, Giles S., Tong, Robert P., Wilson, Miles
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 267
container_issue 1751
container_start_page 251
container_title Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences
container_volume 357
creator Blake, J. R.
Blake, John R.
Keen, Giles S.
Tong, Robert P.
Wilson, Miles
description In acoustic cavitation the spatial variation and time-dependent nature of the acoustic pressure field, whether it is a standing or propagating wave, together with the presence of other bubbles, particles and boundaries produces gradients and asymmetries in the flow field. This will inevitably lead to non-spherical bubble behaviour, often of short duration, before break-up into smaller bubbles which may act as nuclei for the generation of further bubbles. During the collapse phase, high temperatures and pressures will occur in the gaseous interior of the bubble. This paper concentrates on the non-spherical bubble extension to the earlier spherical-bubble studies for acoustic cavitation by exploiting the techniques that had previously been used to model incompressible hydraulic cavitation phenomena. Bubble behaviour near an oscillating boundary, jet impact and damage to boundaries, bubble interactions, bubble clouds and bubble behaviour near rough surfaces are considered. In many cases the key manifestation of the asymmetry is the development of a high-speed liquid jet that penetrates the interior of the bubble. Jetting behaviour can lead to high pressures, high strain rates (of importance to break-up of macromolecules) and toroidal bubbles, all of which can enhance mixing. In addition it may provide a mechanism for injecting the liquid into the hot bubble interior. Many practical applications such as cleaning, enhanced rates of chemical reactions, luminescence and novel metallurgical processes may be associated with this phenomenon.
doi_str_mv 10.1098/rsta.1999.0326
format Article
fullrecord <record><control><sourceid>jstor_istex</sourceid><recordid>TN_cdi_istex_primary_ark_67375_V84_261GXCJZ_5</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><jstor_id>54999</jstor_id><sourcerecordid>54999</sourcerecordid><originalsourceid>FETCH-LOGICAL-c609t-46b3bb502b8b4bac8e9a3b0928948961f9c1b507fe0c9b155f9c6424404ee7e73</originalsourceid><addsrcrecordid>eNp9UMtu1DAUjRBIlMKWBav8QAY7fiRmg4ZRKaBKSLSgis2V7XEYD2kc2U4hrPiH_mG_BCdBVStEF1bsnNe9J8ueY7TCSNQvfYhyhYUQK0RK_iA7wLTCRSl4-TDdCacFQ-T8cfYkhD1CGHNWHmRv1toNIVqda3lpo4zWda_yuDN50w52m2_HTl5YHXLX5J3rrn9fhX5nvNWyzdWgVGvC0-xRI9tgnv39Hmaf3x6dbd4VJx-P32_WJ4XmSMSCckWUYqhUtaJK6toISRQSZS1oLThuhMYJrhqDtFCYsfSD05JSRI2pTEUOs9Xiq70LwZsGem8vpB8BI5gagKkBmBqAqYEkCIvAuzEN5rQ1cYS9G3yXnvDp9GydyPySsMriimFANcGoIjUW8Mv2s91EgEQAG8JgYKbdjfk3ldyX-t9ZXyyqfYjO32zGaGIksFhAG6L5eQNK_x14RSoGX2oKJcfH55sPX4El_uuFv7Pfdj-sN3Bnljlauy6aLs67zVuV6TRD20K_bZIDutfBjX3yuK0lfwBOM8cD</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Acoustic cavitation: the fluid dynamics of non–spherical bubbles</title><source>JSTOR Mathematics and Statistics</source><creator>Blake, J. R. ; Blake, John R. ; Keen, Giles S. ; Tong, Robert P. ; Wilson, Miles</creator><contributor>Blake, J. R. ; Blake, J. R.</contributor><creatorcontrib>Blake, J. R. ; Blake, John R. ; Keen, Giles S. ; Tong, Robert P. ; Wilson, Miles ; Blake, J. R. ; Blake, J. R.</creatorcontrib><description>In acoustic cavitation the spatial variation and time-dependent nature of the acoustic pressure field, whether it is a standing or propagating wave, together with the presence of other bubbles, particles and boundaries produces gradients and asymmetries in the flow field. This will inevitably lead to non-spherical bubble behaviour, often of short duration, before break-up into smaller bubbles which may act as nuclei for the generation of further bubbles. During the collapse phase, high temperatures and pressures will occur in the gaseous interior of the bubble. This paper concentrates on the non-spherical bubble extension to the earlier spherical-bubble studies for acoustic cavitation by exploiting the techniques that had previously been used to model incompressible hydraulic cavitation phenomena. Bubble behaviour near an oscillating boundary, jet impact and damage to boundaries, bubble interactions, bubble clouds and bubble behaviour near rough surfaces are considered. In many cases the key manifestation of the asymmetry is the development of a high-speed liquid jet that penetrates the interior of the bubble. Jetting behaviour can lead to high pressures, high strain rates (of importance to break-up of macromolecules) and toroidal bubbles, all of which can enhance mixing. In addition it may provide a mechanism for injecting the liquid into the hot bubble interior. Many practical applications such as cleaning, enhanced rates of chemical reactions, luminescence and novel metallurgical processes may be associated with this phenomenon.</description><identifier>ISSN: 1364-503X</identifier><identifier>EISSN: 1471-2962</identifier><identifier>DOI: 10.1098/rsta.1999.0326</identifier><language>eng</language><publisher>The Royal Society</publisher><subject>Acoustic Cavitation ; Bubbles ; Cavitation flow ; Flow distribution ; Fluid jets ; Fluid mechanics ; Fluids ; Lead ; Liquid Jet ; Liquids ; Non-Spherical Bubbles ; Pressure distribution ; Shock waves ; Sonoluminescence ; Toroidal Bubble</subject><ispartof>Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences, 1999-02, Vol.357 (1751), p.251-267</ispartof><rights>Copyright 1999 The Royal Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c609t-46b3bb502b8b4bac8e9a3b0928948961f9c1b507fe0c9b155f9c6424404ee7e73</citedby><cites>FETCH-LOGICAL-c609t-46b3bb502b8b4bac8e9a3b0928948961f9c1b507fe0c9b155f9c6424404ee7e73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/54999$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/54999$$EHTML$$P50$$Gjstor$$H</linktohtml><link.rule.ids>314,780,784,832,27924,27925,58021,58254</link.rule.ids></links><search><contributor>Blake, J. R.</contributor><contributor>Blake, J. R.</contributor><creatorcontrib>Blake, J. R.</creatorcontrib><creatorcontrib>Blake, John R.</creatorcontrib><creatorcontrib>Keen, Giles S.</creatorcontrib><creatorcontrib>Tong, Robert P.</creatorcontrib><creatorcontrib>Wilson, Miles</creatorcontrib><title>Acoustic cavitation: the fluid dynamics of non–spherical bubbles</title><title>Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences</title><description>In acoustic cavitation the spatial variation and time-dependent nature of the acoustic pressure field, whether it is a standing or propagating wave, together with the presence of other bubbles, particles and boundaries produces gradients and asymmetries in the flow field. This will inevitably lead to non-spherical bubble behaviour, often of short duration, before break-up into smaller bubbles which may act as nuclei for the generation of further bubbles. During the collapse phase, high temperatures and pressures will occur in the gaseous interior of the bubble. This paper concentrates on the non-spherical bubble extension to the earlier spherical-bubble studies for acoustic cavitation by exploiting the techniques that had previously been used to model incompressible hydraulic cavitation phenomena. Bubble behaviour near an oscillating boundary, jet impact and damage to boundaries, bubble interactions, bubble clouds and bubble behaviour near rough surfaces are considered. In many cases the key manifestation of the asymmetry is the development of a high-speed liquid jet that penetrates the interior of the bubble. Jetting behaviour can lead to high pressures, high strain rates (of importance to break-up of macromolecules) and toroidal bubbles, all of which can enhance mixing. In addition it may provide a mechanism for injecting the liquid into the hot bubble interior. Many practical applications such as cleaning, enhanced rates of chemical reactions, luminescence and novel metallurgical processes may be associated with this phenomenon.</description><subject>Acoustic Cavitation</subject><subject>Bubbles</subject><subject>Cavitation flow</subject><subject>Flow distribution</subject><subject>Fluid jets</subject><subject>Fluid mechanics</subject><subject>Fluids</subject><subject>Lead</subject><subject>Liquid Jet</subject><subject>Liquids</subject><subject>Non-Spherical Bubbles</subject><subject>Pressure distribution</subject><subject>Shock waves</subject><subject>Sonoluminescence</subject><subject>Toroidal Bubble</subject><issn>1364-503X</issn><issn>1471-2962</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1999</creationdate><recordtype>article</recordtype><recordid>eNp9UMtu1DAUjRBIlMKWBav8QAY7fiRmg4ZRKaBKSLSgis2V7XEYD2kc2U4hrPiH_mG_BCdBVStEF1bsnNe9J8ueY7TCSNQvfYhyhYUQK0RK_iA7wLTCRSl4-TDdCacFQ-T8cfYkhD1CGHNWHmRv1toNIVqda3lpo4zWda_yuDN50w52m2_HTl5YHXLX5J3rrn9fhX5nvNWyzdWgVGvC0-xRI9tgnv39Hmaf3x6dbd4VJx-P32_WJ4XmSMSCckWUYqhUtaJK6toISRQSZS1oLThuhMYJrhqDtFCYsfSD05JSRI2pTEUOs9Xiq70LwZsGem8vpB8BI5gagKkBmBqAqYEkCIvAuzEN5rQ1cYS9G3yXnvDp9GydyPySsMriimFANcGoIjUW8Mv2s91EgEQAG8JgYKbdjfk3ldyX-t9ZXyyqfYjO32zGaGIksFhAG6L5eQNK_x14RSoGX2oKJcfH55sPX4El_uuFv7Pfdj-sN3Bnljlauy6aLs67zVuV6TRD20K_bZIDutfBjX3yuK0lfwBOM8cD</recordid><startdate>19990215</startdate><enddate>19990215</enddate><creator>Blake, J. R.</creator><creator>Blake, John R.</creator><creator>Keen, Giles S.</creator><creator>Tong, Robert P.</creator><creator>Wilson, Miles</creator><general>The Royal Society</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19990215</creationdate><title>Acoustic cavitation: the fluid dynamics of non–spherical bubbles</title><author>Blake, J. R. ; Blake, John R. ; Keen, Giles S. ; Tong, Robert P. ; Wilson, Miles</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c609t-46b3bb502b8b4bac8e9a3b0928948961f9c1b507fe0c9b155f9c6424404ee7e73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1999</creationdate><topic>Acoustic Cavitation</topic><topic>Bubbles</topic><topic>Cavitation flow</topic><topic>Flow distribution</topic><topic>Fluid jets</topic><topic>Fluid mechanics</topic><topic>Fluids</topic><topic>Lead</topic><topic>Liquid Jet</topic><topic>Liquids</topic><topic>Non-Spherical Bubbles</topic><topic>Pressure distribution</topic><topic>Shock waves</topic><topic>Sonoluminescence</topic><topic>Toroidal Bubble</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Blake, J. R.</creatorcontrib><creatorcontrib>Blake, John R.</creatorcontrib><creatorcontrib>Keen, Giles S.</creatorcontrib><creatorcontrib>Tong, Robert P.</creatorcontrib><creatorcontrib>Wilson, Miles</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><jtitle>Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Blake, J. R.</au><au>Blake, John R.</au><au>Keen, Giles S.</au><au>Tong, Robert P.</au><au>Wilson, Miles</au><au>Blake, J. R.</au><au>Blake, J. R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Acoustic cavitation: the fluid dynamics of non–spherical bubbles</atitle><jtitle>Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences</jtitle><date>1999-02-15</date><risdate>1999</risdate><volume>357</volume><issue>1751</issue><spage>251</spage><epage>267</epage><pages>251-267</pages><issn>1364-503X</issn><eissn>1471-2962</eissn><abstract>In acoustic cavitation the spatial variation and time-dependent nature of the acoustic pressure field, whether it is a standing or propagating wave, together with the presence of other bubbles, particles and boundaries produces gradients and asymmetries in the flow field. This will inevitably lead to non-spherical bubble behaviour, often of short duration, before break-up into smaller bubbles which may act as nuclei for the generation of further bubbles. During the collapse phase, high temperatures and pressures will occur in the gaseous interior of the bubble. This paper concentrates on the non-spherical bubble extension to the earlier spherical-bubble studies for acoustic cavitation by exploiting the techniques that had previously been used to model incompressible hydraulic cavitation phenomena. Bubble behaviour near an oscillating boundary, jet impact and damage to boundaries, bubble interactions, bubble clouds and bubble behaviour near rough surfaces are considered. In many cases the key manifestation of the asymmetry is the development of a high-speed liquid jet that penetrates the interior of the bubble. Jetting behaviour can lead to high pressures, high strain rates (of importance to break-up of macromolecules) and toroidal bubbles, all of which can enhance mixing. In addition it may provide a mechanism for injecting the liquid into the hot bubble interior. Many practical applications such as cleaning, enhanced rates of chemical reactions, luminescence and novel metallurgical processes may be associated with this phenomenon.</abstract><pub>The Royal Society</pub><doi>10.1098/rsta.1999.0326</doi><tpages>17</tpages></addata></record>
fulltext fulltext
identifier ISSN: 1364-503X
ispartof Philosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences, 1999-02, Vol.357 (1751), p.251-267
issn 1364-503X
1471-2962
language eng
recordid cdi_istex_primary_ark_67375_V84_261GXCJZ_5
source JSTOR Mathematics and Statistics
subjects Acoustic Cavitation
Bubbles
Cavitation flow
Flow distribution
Fluid jets
Fluid mechanics
Fluids
Lead
Liquid Jet
Liquids
Non-Spherical Bubbles
Pressure distribution
Shock waves
Sonoluminescence
Toroidal Bubble
title Acoustic cavitation: the fluid dynamics of non–spherical bubbles
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-25T06%3A44%3A49IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-jstor_istex&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Acoustic%20cavitation:%20the%20fluid%20dynamics%20of%20non%E2%80%93spherical%20bubbles&rft.jtitle=Philosophical%20transactions%20of%20the%20Royal%20Society%20of%20London.%20Series%20A:%20Mathematical,%20physical,%20and%20engineering%20sciences&rft.au=Blake,%20J.%20R.&rft.date=1999-02-15&rft.volume=357&rft.issue=1751&rft.spage=251&rft.epage=267&rft.pages=251-267&rft.issn=1364-503X&rft.eissn=1471-2962&rft_id=info:doi/10.1098/rsta.1999.0326&rft_dat=%3Cjstor_istex%3E54999%3C/jstor_istex%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rft_jstor_id=54999&rfr_iscdi=true