Mostrar el registro sencillo del ítem

dc.contributor.authorRuiz Rus, J.
dc.contributor.authorErn, P.
dc.contributor.authorRoig, V.
dc.contributor.authorMartínez Bazán, Jesús Carlos 
dc.date.accessioned2024-12-12T09:18:39Z
dc.date.available2024-12-12T09:18:39Z
dc.date.issued2022-06-23
dc.identifier.citationRuiz Rus, J. et. al. J. Fluid Mech. (2022), vol. 944, A13. [https://doi.org/10.1017/jfm.2022.492]es_ES
dc.identifier.urihttps://hdl.handle.net/10481/97934
dc.description.abstractWe investigate experimentally the coalescence cascade process for a confined swarm of deformable bubbles immersed in a bidimensional vertical cell filled with water. For different gas volume fractions, air bubbles of size D0 larger than the cell thickness are injected at the bottom of the cell. The bubbles swarms transformation is explored using high-speed visualizations. The time evolution of each bubble in the swarm is determined using a specifically developed algorithm, enabling bubble tracking and coalescence detection. We determine the evolution of the bubble size distribution downstream from the injection point, and show that the stages of the coalescence cascade are characterized by the diameter, DV90, representative of the largest bubbles. The collision frequency of pairs of bubbles of sizes Dk and Dk , h(Dk,Dk ), and their coalescence efficiency, λ, are obtained from the experiments. The efficiency is nearly constant, independently of the bubble sizes and of the gas volume fraction. Concerning collision frequency, our results reveal the existence of two different coalescence regimes depending on the capability of the bubbles to deform. Models describing h(Dk,Dk ) for both regimes are provided. They take into account the specific response of the bubble pair, which depends on the reduced diameter Dp = 2DkDk /(Dk + Dk ), to the global swarm-induced agitation governed by DV90 and the gas volume fraction. In the first regime, occurring for smaller Dp, bubbles are brought together by agitation and rapidly coalesce, while for sufficiently large Dp, both bubbles are able to deform and spend more time adapting mutually their shapes before coalescing.es_ES
dc.description.sponsorshipSpanishMINECO and European Funds under projects DPI2017-88201-C3-2-Res_ES
dc.description.sponsorshipPrograma Operativo FEDER Andalucía 2014–2020es_ES
dc.description.sponsorshipConsejería de Economía y Conocimiento de la Junta de Andalucía under project 1263528es_ES
dc.description.sponsorshipFrench Agence Nationale de la Recherche (ANR) under reference ANR-19-CE43-0002-02 (ALLIGATOR project)es_ES
dc.description.sponsorshipSpanish MINECO for the financial support provided by the fellowship BES-2015-071329es_ES
dc.description.sponsorshipRed Nacional para el Desarrollo de la Microfluídica, RED2018-102829-Tes_ES
dc.language.isoenges_ES
dc.publisherCambridge University Presses_ES
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectbreakup/coalescencees_ES
dc.subjectgas/liquid flowes_ES
dc.subjectbubble dynamicses_ES
dc.titleCoalescence of bubbles in a high Reynolds number confined swarmes_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1017/jfm.2022.492
dc.type.hasVersionVoRes_ES


Ficheros en el ítem

[PDF]

Este ítem aparece en la(s) siguiente(s) colección(ones)

Mostrar el registro sencillo del ítem

Atribución 4.0 Internacional
Excepto si se señala otra cosa, la licencia del ítem se describe como Atribución 4.0 Internacional