Please use this identifier to cite or link to this item: https://hdl.handle.net/20.500.14279/31010
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dc.contributor.authorBidi, Saeed-
dc.contributor.authorShams, Armand-
dc.contributor.authorKoukouvinis, Foivos (Phoevos)-
dc.contributor.authorGavaises, Manolis-
dc.date.accessioned2024-01-24T08:52:51Z-
dc.date.available2024-01-24T08:52:51Z-
dc.date.issued2023-12-
dc.identifier.citationUltrasonics Sonochemistry, 2023, vol. 101en_US
dc.identifier.issn13504177-
dc.identifier.urihttps://hdl.handle.net/20.500.14279/31010-
dc.description.abstractNumerical simulations of collapsing air bubbles considering complex and more accurate equations of state (EoS) for estimating the properties of both the liquid and gas are presented. The necessity for utilising such EoSs in bubble collapse simulations is illustrated by the unphysical (spurious) liquid temperature jump formed in the vicinity of the bubble-air interface when simplified EoSs are used. The solved fluid flow equations follow the mechanical equilibrium multiphase method of Kapila. The solver is coded in the AMReX platform, enabling high-performance computation with parallel processing and Adaptive Mesh Refinement for speeding up simulations. It is initially demonstrated that the frequently used Stiffened Gas (SG) EoS overpredicts the liquid temperature at high compression. More sophisticated EoS models, such as the International Association for the Properties of Water and Steam (IAPWS), the Modified Noble Abel Stiffened Gas (MNASG) and a modified Tait EoS introduced here, are also implemented into the flow solver and their differences are highlighted for bubble collapse cases for the first time. Subsequently, application of the developed model to cases of practical interest is showcased. More specifically, simulations of bubble collapse near a solid wall are presented for conditions simulating shock wave lithotripsy (SWL). It is concluded that for such cases, a maximum increase of 25 K of the liquid temperature in contact along the solid wall is caused during the collapse of the air bubble due to shock wave focusing effects. It is also highlighted that the maximum liquid heating varies depending on the initial bubble-wall stand-off distance.en_US
dc.formatpdfen_US
dc.language.isoenen_US
dc.relation.ispartofUltrasonics sonochemistryen_US
dc.rights© The Author(s)en_US
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 International*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.subjectBubble collapse dynamicsen_US
dc.subjectIAPWS dataen_US
dc.subjectMNASGen_US
dc.subjectReal-liquid EoSen_US
dc.subjectShock wave lithotripsy (SWL)en_US
dc.subjectTait EoSen_US
dc.titlePrediction of shock heating during ultrasound-induced bubble collapse using real-fluid equations of stateen_US
dc.typeArticleen_US
dc.collaborationUniversity of Londonen_US
dc.collaborationSorbonne Universitésen_US
dc.subject.categoryComputer and Information Sciencesen_US
dc.journalsOpen Accessen_US
dc.countryUnited Kingdomen_US
dc.countryFranceen_US
dc.subject.fieldNatural Sciencesen_US
dc.publicationPeer Revieweden_US
dc.identifier.doi10.1016/j.ultsonch.2023.106663en_US
dc.identifier.pmid38039592-
dc.identifier.scopus2-s2.0-85180411214-
dc.identifier.urlhttps://api.elsevier.com/content/abstract/scopus_id/85180411214-
dc.relation.volume101en_US
cut.common.academicyear2023-2024en_US
item.grantfulltextopen-
item.openairecristypehttp://purl.org/coar/resource_type/c_6501-
item.fulltextWith Fulltext-
item.languageiso639-1en-
item.cerifentitytypePublications-
item.openairetypearticle-
crisitem.author.deptDepartment of Mechanical Engineering and Materials Science and Engineering-
crisitem.author.facultyFaculty of Engineering and Technology-
crisitem.author.orcid0000-0002-3945-3707-
crisitem.author.parentorgFaculty of Engineering and Technology-
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