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dc.contributor.authorArias Calderón, Santiago
dc.contributor.otherUniversitat Politècnica de Catalunya. Departament de Física
dc.date.accessioned2020-07-04T06:52:49Z
dc.date.available2021-05-25T00:32:54Z
dc.date.issued2020-05-28
dc.identifier.citationArias, S. Comparison of Two Gas Injection Methods for Generating Bubbles in a T-Junction. "Microgravity science and technology", 28 Maig 2020, p. 1-11.
dc.identifier.issn0938-0108
dc.identifier.otherhttps://rdcu.be/b4tWW
dc.identifier.urihttp://hdl.handle.net/2117/192420
dc.description.abstractIn this work, we compare the performance of two different methods for generating bubbles in conditions relevant to microgravity. A T-junction formed by two cylindrical (1 mm of internal diameter) and perpendicular channels is used to generate trains of non-wetting bubbles. Air and distilled water are used as dispersed and continuous phases, respectively. The difference between both methods lies in the strategy used to inject the fluids. In one case (here referred to as TJ-A configuration), the gas is injected into the side channel. In the other case (referred to as TJ-B), the gas is injected into the main channel. Bubble size dispersion is analyzed and quantified with the polydispersity index. The increase of the capillary number (based on the continuous phase) has shown a strong influence on the regularity of the bubble generation process. The TJ-A method can produce monodisperse bubbles at higher capillary numbers than configuration TJ-B. The limits of monodispersity, as far as the capillary number is concerned, are studied. These limits determine the optimal operating range of the T-junction for generating highly monodisperse bubbles. Beyond these limits, polydispersity increases, although much more abruptly in TJ-B than in TJ-A. The bubble generation frequency is also studied, with special attention to the two main regimes that characterize the frequency, i.e. the linear regime (at very low gas flow rate) and the saturation regime (at high gas flow rates). A new dimensionless expression of the bubble generation frequency is proposed in this work.
dc.format.extent11 p.
dc.language.isoeng
dc.rightsAttribution-NonCommercial-NoDerivs 3.0 Spain
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es/
dc.subjectÀrees temàtiques de la UPC::Física
dc.subject.lcshReduced gravity environments
dc.subject.lcshMicrobubbles
dc.subject.otherMicrogravity
dc.subject.otherTwo-phase flow
dc.subject.otherBubble formation
dc.subject.otherMicrochannel
dc.subject.otherT-junction
dc.subject.otherMonodisperse bubbles
dc.titleComparison of Two Gas Injection Methods for Generating Bubbles in a T-Junction
dc.typeArticle
dc.subject.lemacAmbients de microgravetat
dc.subject.lemacBombolles
dc.contributor.groupUniversitat Politècnica de Catalunya. BIOCOM-SC - Grup de Biologia Computacional i Sistemes Complexos
dc.identifier.doi10.1007/s12217-020-09790-3
dc.description.peerreviewedPeer Reviewed
dc.relation.publisherversionhttp://link.springer.com/article/10.1007/s12217-020-09790-3
dc.rights.accessOpen Access
local.identifier.drac28622623
dc.description.versionPostprint (author's final draft)
local.citation.authorArias, S.
local.citation.publicationNameMicrogravity science and technology
local.citation.startingPage1
local.citation.endingPage11


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