{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1363388843962063872.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1017/jfm.2013.525"}},{"identifier":{"@type":"URI","@value":"https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112013005259"}}],"dc:title":[{"@value":"Thermodynamic effects during growth and collapse of a single cavitation bubble"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:title>Abstract</jats:title><jats:p>The thermodynamic effects associated with the growth and collapse of a single cavitation bubble are investigated in the present paper by an experimental approach. The study focuses on the temperature variations in the liquid surrounding the bubble. Experiments are conducted in a cylinder partially filled with water at an ambient temperature and atmospheric pressure. The bubble growth results from the expansion of an initial air bubble, due to the pressure wave generated by a so-called ‘tube-arrest’ method. Several locations of the bubble, at different distances from the bottom wall of the cylinder, are considered. The bottom wall is made of sapphire, which is transparent to both the visible and infrared light spectra which enables temperature measurements by a high-speed thermovision camera at a wavelength of 3–<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"gif\" xlink:type=\"simple\" xlink:href=\"S0022112013005259_inline1\"/><jats:tex-math>$5~\\unicode[.5,0][STIXGeneral,Times]{x03BC} \\mathrm{m} $</jats:tex-math></jats:alternatives></jats:inline-formula>. Water is opaque to the infrared light spectrum, hence only temperatures in the boundary layer and on the liquid vapour interface could be determined. A temperature decrease of<jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"gif\" xlink:type=\"simple\" xlink:href=\"S0022112013005259_inline2\"/><jats:tex-math>${\\sim }3$</jats:tex-math></jats:alternatives></jats:inline-formula> K was recorded during the bubble growth while an increase up to 4 K was detected during the collapse. Experimental results are compared to the predictions of the ‘thermal delay’ model based on the assumption that the bubble growth and collapse are due to phase changes only. In this approach, the temperature variations are related to the latent heat exchanges during the vapourization and condensation processes. On the basis of these results, the respective effects of phase change and air dilatation/compression in the bubble dynamics are discussed.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1383388843962063872","@type":"Researcher","foaf:name":[{"@value":"Matevž Dular"}]},{"@id":"https://cir.nii.ac.jp/crid/1383388843962063873","@type":"Researcher","foaf:name":[{"@value":"Olivier Coutier-Delgosha"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00221120"},{"@type":"EISSN","@value":"14697645"}],"prism:publicationName":[{"@value":"Journal of Fluid Mechanics"}],"dc:publisher":[{"@value":"Cambridge University Press (CUP)"}],"prism:publicationDate":"2013-11-01","prism:volume":"736","prism:startingPage":"44","prism:endingPage":"66"},"reviewed":"false","dc:rights":["https://www.cambridge.org/core/terms"],"url":[{"@id":"https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112013005259"}],"createdAt":"2013-11-01","modifiedAt":"2024-05-19","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360004232544228608","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Fundamental study of sterilization effects on marine Vibrio sp. in a cylindrical water chamber with supply of only underwater shock waves"}]},{"@id":"https://cir.nii.ac.jp/crid/1360022307168992768","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Study of Sterilization Effects on Marine\n                  <i>Vibrio</i>\n                  sp. using Interaction of Cavitation with Shock Wave in a Narrow Water Chamber"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567182497676928","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A theoretical model to estimate inactivation effects of OH radicals on marine Vibrio sp. in bubble-shock interaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1390861150942708096","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Hard water can be softened by atomization"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1017/jfm.2013.525"},{"@type":"CROSSREF","@value":"10.1016/j.ultsonch.2017.11.047_references_DOI_5yPLUP2aWz1ve34XdAU2xghRGGM"},{"@type":"CROSSREF","@value":"10.1016/j.ultsonch.2018.10.001_references_DOI_5yPLUP2aWz1ve34XdAU2xghRGGM"},{"@type":"CROSSREF","@value":"10.3136/fstr.fstr-d-23-00059_references_DOI_5yPLUP2aWz1ve34XdAU2xghRGGM"},{"@type":"CROSSREF","@value":"10.1101/370445_references_DOI_5yPLUP2aWz1ve34XdAU2xghRGGM"},{"@type":"CROSSREF","@value":"10.1063/1.5052521_references_DOI_5yPLUP2aWz1ve34XdAU2xghRGGM"}]}