{"@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/1362262944654670848.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1017/s0022112074001121"}},{"identifier":{"@type":"URI","@value":"https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112074001121"}}],"dc:title":[{"@value":"Vortex pairing : the mechanism of turbulent mixing-layer growth at moderate Reynolds number"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>A mixing layer is formed by bringing two streams of water, moving at different velocities, together in a lucite-walled channel. The Reynolds number, based on the velocity difference and the thickness of the shear layer, varies from about 45, where the shear layer originates, to about 850 at a distance of 50 cm. Dye is injected between the two streams just before they are brought together, marking the vorticity-carrying fluid. Unstable waves grow, and fluid is observed to roll up into discrete two-dimensional vortical structures. These turbulent vortices interact by rolling around each other, and a single vortical structure, with approximately twice the spacing of the former vortices, is formed. This pairing process is observed to occur repeatedly, controlling the growth of the mixing layer. A simple model of the mixing layer contains, as the important elements controlling growth, the degree of non-uniformity in the vortex train and the ‘lumpiness’ of the vorticity field.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382262944654670849","@type":"Researcher","foaf:name":[{"@value":"C. D. Winant"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262944654670848","@type":"Researcher","foaf:name":[{"@value":"F. K. Browand"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00221120"},{"@type":"EISSN","@value":"14697645"},{"@type":"PISSN","@value":"http://id.crossref.org/issn/00221120"}],"prism:publicationName":[{"@value":"Journal of Fluid Mechanics"}],"dc:publisher":[{"@value":"Cambridge University Press (CUP)"}],"prism:publicationDate":"1974-04-03","prism:volume":"63","prism:number":"2","prism:startingPage":"237","prism:endingPage":"255"},"reviewed":"false","dc:rights":["https://www.cambridge.org/core/terms"],"url":[{"@id":"https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022112074001121"}],"createdAt":"2006-03-29","modifiedAt":"2025-06-21","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360286993800833536","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Unified mechanisms for separation control around airfoil using plasma actuator with burst actuation over Reynolds number range of 103–106"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588380593859968","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Nonlinear Wave Damping by Kelvin–Helmholtz Instability-induced Turbulence"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204079294848","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"On Evolution of Flow Structure and Vortex Dynamics for Right-Angle and Sharp-Edged Orifice Plane Jet"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204183328256","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Large-Eddy Structures in a Turbulent Mixing Layer"},{"@value":"Large-Eddy Structures in a Turbulent Mixing Layar"},{"@language":"ja-Kana","@value":"Large Eddy Structures in a Turbulent Mi"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204183331456","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Formation of Vortices around a Sinkhole"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001205309036672","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"BUOYANCY EFFECTS IN TURBULENT JETS AND PLUMES"},{"@language":"ja","@value":"ジェットとプルーム"},{"@language":"ja-Kana","@value":"ジェット ト プルーム"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001205601175168","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"TURBULENT STRUCTURE AND CONTROL OF COHERENT VORTEX IN MIXING LAYER OF OPEN-CHANNEL PARALLEL COFLOWS"},{"@language":"ja","@value":"開水路合流部の混合層における乱流構造と組織渦の制御に関する研究"}]},{"@id":"https://cir.nii.ac.jp/crid/1390282679546092416","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Investigation of Turbulent-Mixing-Layer Flow with Polymer Additives and Bubble Injection by Particle Image Velocimetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1390282679653071232","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Toward Smart Control of Turbulent Jet Mixing and Combustion"}]},{"@id":"https://cir.nii.ac.jp/crid/1390282680577354496","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"SPATIAL-TEMPORAL STRUCTURE OF LARGE VORTEX IN A MIXING SHEAR FLOW AND ITS HYDRAULIC ROLES"},{"@language":"ja","@value":"混合せん断流における大規模渦の時空間構造とその水理学的役割"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1017/s0022112074001121"},{"@type":"CROSSREF","@value":"10.1143/jpsj.53.1026_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.1063/1.5136072_references_DOI_66h8HOPqSaqwOo7frAiDsgA6fZW"},{"@type":"CROSSREF","@value":"10.1252/jcej.09we232_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.1299/jsmeb.49.941_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.2322/tjsass.53.296_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.3847/1538-4357/ad306f_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.1143/jpsj.53.3378_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.2208/jscej.1987.387_153_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.2208/jscej.1991.429_1_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"},{"@type":"CROSSREF","@value":"10.2208/jscej.1989.405_89_references_DOI_PyLGslwk06xAeQwqZooJgXJwLKI"}]}