dc.creatorLonginotti, María Paula
dc.creatorFuentes Landete, Violeta
dc.creatorLoerting, Thomas
dc.creatorCorti, Horacio Roberto
dc.date.accessioned2021-01-04T19:07:19Z
dc.date.accessioned2022-10-15T03:44:48Z
dc.date.available2021-01-04T19:07:19Z
dc.date.available2022-10-15T03:44:48Z
dc.date.created2021-01-04T19:07:19Z
dc.date.issued2019-08
dc.identifierLonginotti, María Paula; Fuentes Landete, Violeta; Loerting, Thomas; Corti, Horacio Roberto; Glass transition of LiCl aqueous solutions confined in mesoporous silica; American Institute of Physics; Journal of Chemical Physics; 151; 6; 8-2019; 1-12
dc.identifier0021-9606
dc.identifierhttp://hdl.handle.net/11336/121411
dc.identifierCONICET Digital
dc.identifierCONICET
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4341515
dc.description.abstractThe thermal transitions of confined LiCl aqueous solutions were studied by differential scanning calorimetry for solutions with salt concentrations with eutectic (R = 7) and subeutectic (R > 7) compositions (R = moles of water/moles of LiCl). The confinement media consist of mesoporous silica with pore diameters between 2 nm and 58 nm, with a small negative surface charge density. The vitrification of confined LiCl aqueous solutions was observed in all samples, expanding the vitrification region up to R = 15, and probably beyond for cooling rates of ≈1000 K/min. Ice crystallization was observed in some samples, except for those confined in the narrower pores. The onset and endpoint glass transition temperatures for the confined eutectic samples increase by 2 K and 5 K, respectively, for the smallest pore diameters (2 nm), which is equivalent to the effect of applying a pressure of up to 100 MPa to the bulk sample. This behavior is opposite of that reported for aqueous subeutectic NaCl solutions confined in silica glasses of similar sizes. We speculate that this is due to the fact that the mechanism of double confinement of the NaCl solution, between the pore wall and the precipitated ice, is not operative for LiCl solutions. Instead, the Li+ ions might force the hydration water in to a high-density state.
dc.languageeng
dc.publisherAmerican Institute of Physics
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1063/1.5102142
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://aip.scitation.org/doi/10.1063/1.5102142
dc.rightshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectglass transition
dc.subjectLiCl
dc.subjectconfinement
dc.subjectaqueous solutions
dc.titleGlass transition of LiCl aqueous solutions confined in mesoporous silica
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:ar-repo/semantics/artículo
dc.typeinfo:eu-repo/semantics/publishedVersion


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