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dc.contributor.authorProkopev, Sergei
dc.contributor.authorLyubimova, Tatyana
dc.contributor.authorMialdun, Aliaksandr
dc.contributor.authorShevtsova, Valentina
dc.date.accessioned2025-04-30T10:28:03Z
dc.date.available2025-04-30T10:28:03Z
dc.date.issued2021
dc.identifier.issn1463-9084en
dc.identifier.otherhttps://katalogoa.mondragon.edu/janium-bin/janium_login_opac.pl?find&ficha_no=163295en
dc.identifier.urihttps://hdl.handle.net/20.500.11984/6985
dc.description.abstractTernary mixtures with the Soret effect are prone to triple-diffusive convection in a thermal field. The Soret coefficients of the toluene–methanol–cyclohexane mixture, measured in microgravity at a given composition [0.62–0.31–0.07] in mass fractions, showed that the net separation ratio, Ψ, the parameter responsible for the hydrodynamic stability in a gravity field is close to zero. Furthermore, the large cross-diffusion of toluene leads to a curious situation: the Soret coefficient ST1 is positive while the thermodiffusion coefficient DT1 is negative. The behavior of this ternary mixture on the border of stability, when Ψ is slightly negative or positive, is examined experimentally and numerically. The mixture is placed in an elongated cell between the differently heated walls. Depending on Ψ and the initial temperature of the liquid (mean temperature, linear profile or cold one), the evolution of concentration patterns are classified by four regimes. We observe the emergence of motionless, metastable, and convective patterns. In the case of Ψ > 0, it was found that cross-diffusion fluxes cause a temporarily unstable density pattern. The initially cold mixture at either Ψ sign shows dissimilar Soret separation in the upper and lower parts of the cell. It leads to the formation of a long-lived inverse density gradient at the upper part of the cell, which finally results in a motionless (Ψ > 0) or convective (Ψ < 0) pattern.es
dc.language.isoengen
dc.publisherRoyal Society of Chemistryen
dc.rights© 2021 Royal Society of Chemistryen
dc.titleA ternary mixture at the border of Soret separation stabilityen
dcterms.accessRightshttp://purl.org/coar/access_right/c_abf2en
dcterms.sourcePhysical Chemistry Chemical Physicsen
local.contributor.groupMecánica de fluidoses
local.description.peerreviewedtrueen
local.description.publicationfirstpage8466en
local.description.publicationlastpage8477en
local.identifier.doihttps://doi.org/10.1039/D0CP06471Hen
local.contributor.otherinstitutionhttps://ror.org/01cc3fy72es
local.contributor.otherinstitutionhttps://ror.org/03ymmms77es
local.contributor.otherinstitutionhttps://ror.org/029njb796es
local.contributor.otherinstitutionhttps://ror.org/01r9htc13es
local.source.detailsVol. 23. N. 14.en
oaire.format.mimetypeapplication/pdfen
oaire.file$DSPACE\assetstoreen
oaire.resourceTypehttp://purl.org/coar/resource_type/c_6501en
oaire.versionhttp://purl.org/coar/version/c_ab4af688f83e57aaen
dc.unesco.tesaurohttp://vocabularies.unesco.org/thesaurus/concept134en
oaire.funderNameGobierno Vascoen
oaire.funderIdentifierhttps://ror.org/00pz2fp31 / http://data.crossref.org/fundingdata/funder/10.13039/501100003086en
oaire.fundingStreamPrograma Elkartek 2019en
oaire.awardNumberKK-2019-00101en
oaire.awardTitleMicrosistemas inteligentes avanzados e integrados en la industria. Monitorización, digitalización e inspección preventiva en entornos de producción (µ4INDUST)en
oaire.awardURISin informaciónen
dc.unesco.clasificacionhttp://skos.um.es/unesco6/2213en


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