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dc.creatorGordillo Arias de Saavedra, José Manueles
dc.creatorSevilla, A.es
dc.creatorMartínez Bazán, C.es
dc.date.accessioned2017-04-07T13:56:44Z
dc.date.available2017-04-07T13:56:44Z
dc.date.issued2007
dc.identifier.citationGordillo Arias de Saavedra, J.M., Sevilla, A. y Martínez Bazán, C. (2007). Bubbling in a co-flow at high Reynolds numbers. Physics of fluids, 19 (7), 077102-1-077102-18.
dc.identifier.issn1070-6631es
dc.identifier.urihttp://hdl.handle.net/11441/57370
dc.description.abstractThe physical mechanisms underlying bubble formation from a needle in a co-flowing liquid environment at high Reynolds numbers are studied in detail with the aid of experiments and boundary-integral numerical simulations. To determine the effect of gas inertia the experiments were carried out with air and helium. The influence of the injection system is elucidated by performing experiments using two different facilities, one where the constancy of the gas flow-rate entering the bubble is ensured, and another one where the gas is injected through a needle directly connected to a pressurized chamber. In the case of constant flow-rate injection conditions, the bubbling frequency has been shown to hardly depend on the gas density, with a bubble size given by db / ro  ? 6U? K * U + k2 /? U- 1? 1/3 for U? 2, where U is the gas-to-liquid ratio of the mean velocities, ro is the radius of the gas injection needle, and k * = 5,84 and k2 = 4,29, whit db / ro3,3U1 / 3 for U1.. Nevertheless, in this case the effect of gas density is relevant to describe the final instants of bubble breakup, which take place at a time scale much smaller than the bubbling time, tb. This effect is evidenced by the liquid jets penetrating the gas bubbles upon their pinch-off. Our measurements indicate that the velocity of the penetrating jets is considerably larger in air bubbles than in helium bubbles due to the distinct gas inertia of both situations. However, in the case of constant pressure supply conditions, the bubble size strongly depends on the density of the gas through the pressure loss along the gas injection needle. Furthermore, under the operating conditions reported here, the equivalent diameters of the bubbles are between 10% and 20% larger than their constant flow-rate counterparts. In addition, the experiments and the numerical results show that, under constant pressure supply, helium bubbles are approximately 10% larger than air bubbles due to the gas density effect on the bubbling process.es
dc.formatapplication/pdfes
dc.language.isoenges
dc.publisherAIP Publishinges
dc.relation.ispartofPhysics of fluids, 19 (7), 077102-1-077102-18.
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.subjectBubblinges
dc.subjectReynolds numberses
dc.subjectCo-flowes
dc.titleBubbling in a co-flow at high Reynolds numberses
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Ingeniería Aeroespacial y Mecánica de Fluidoses
dc.relation.publisherversionhttp://aip.scitation.org/doi/abs/10.1063/1.2747996es
dc.identifier.doi10.1063/1.2747996es
dc.contributor.groupUniversidad de Sevilla. TEP103: Mecánica de Fluidoses
idus.format.extent18 p.es
dc.journaltitlePhysics of fluidses
dc.publication.volumen19es
dc.publication.issue7es
dc.publication.initialPage077102-1es
dc.publication.endPage077102-18es

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