Ice-Crystal Nucleation in Water: Thermodynamic Driving Force and Surface Tension. Part I: Theoretical Foundation

dc.bibliographicCitation.firstPage50eng
dc.bibliographicCitation.issue1eng
dc.bibliographicCitation.journalTitleEntropy : an international and interdisciplinary journal of entropy and informationeng
dc.bibliographicCitation.volume22eng
dc.contributor.authorHellmuth, Olaf
dc.contributor.authorSchmelzer, Jürn W.P.
dc.contributor.authorFeistel, Rainer
dc.date.accessioned2021-07-12T09:37:26Z
dc.date.available2021-07-12T09:37:26Z
dc.date.issued2020
dc.description.abstractA recently developed thermodynamic theory for the determination of the driving force of crystallization and the crystal–melt surface tension is applied to the ice-water system employing the new Thermodynamic Equation of Seawater TEOS-10. The deviations of approximative formulations of the driving force and the surface tension from the exact reference properties are quantified, showing that the proposed simplifications are applicable for low to moderate undercooling and pressure differences to the respective equilibrium state of water. The TEOS-10-based predictions of the ice crystallization rate revealed pressure-induced deceleration of ice nucleation with an increasing pressure, and acceleration of ice nucleation by pressure decrease. This result is in, at least, qualitative agreement with laboratory experiments and computer simulations. Both the temperature and pressure dependencies of the ice-water surface tension were found to be in line with the le Chatelier–Braun principle, in that the surface tension decreases upon increasing degree of metastability of water (by decreasing temperature and pressure), which favors nucleation to move the system back to a stable state. The reason for this behavior is discussed. Finally, the Kauzmann temperature of the ice-water system was found to amount TK=116K , which is far below the temperature of homogeneous freezing. The Kauzmann pressure was found to amount to pK=−212MPa , suggesting favor of homogeneous freezing on exerting a negative pressure on the liquid. In terms of thermodynamic properties entering the theory, the reason for the negative Kauzmann pressure is the higher mass density of water in comparison to ice at the melting point.eng
dc.description.fondsLeibniz_Fonds
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/6256
dc.identifier.urihttps://doi.org/10.34657/5303
dc.language.isoengeng
dc.publisherBasel : MDPIeng
dc.relation.doihttps://doi.org/10.3390/e22010050
dc.relation.essn1099-4300
dc.rights.licenseCC BY 4.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/eng
dc.subject.ddc530eng
dc.subject.ddc510eng
dc.subject.otherclassical nucleation theoryeng
dc.subject.othercrystallization thermodynamicseng
dc.subject.otherhomogeneous freezingeng
dc.subject.otherthermodynamic driving force of nucleationeng
dc.subject.otherice–water surface tensioneng
dc.subject.otherKauzmann temperature and pressureeng
dc.subject.otherTEOS-10eng
dc.titleIce-Crystal Nucleation in Water: Thermodynamic Driving Force and Surface Tension. Part I: Theoretical Foundationeng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorTROPOSeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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