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Some Considerations on Confined Water: The Thermal Behavior of Transport Properties in Water-Glycerol and Water-Methanol Mixtures

Published online by Cambridge University Press:  26 January 2016

Francesco Mallamace ,
Carmelo Corsaro ,
Domenico Mallamace ,
Cirino Vasi ,
Sebastiano Vasi  and
H. Eugene Stanley
Francesco Mallamace*
Affiliation:
Dipartimento MIFT, Sezione di Fisica,Università di Messina I-98166, Messina, Italy Consiglio Nazionale delle Ricerche-IPCF Messina, I-98166, Messina, Italy Center for Polymer Studies and Department of Physics, Boston University Boston, MA 02215USA.
Carmelo Corsaro
Affiliation:
Dipartimento MIFT, Sezione di Fisica,Università di Messina I-98166, Messina, Italy Consiglio Nazionale delle Ricerche-IPCF Messina, I-98166, Messina, Italy
Domenico Mallamace
Affiliation:
Dipartimento SASTAS, Università di Messina Viale F. Stagno d'Alcontres 31, 98166 Messina, Italy
Cirino Vasi
Affiliation:
Consiglio Nazionale delle Ricerche-IPCF Messina, I-98166, Messina, Italy
Sebastiano Vasi
Affiliation:
Dipartimento MIFT, Sezione di Fisica,Università di Messina I-98166, Messina, Italy
H. Eugene Stanley
Affiliation:
Center for Polymer Studies and Department of Physics, Boston University Boston, MA 02215USA.
*
*(Email: [email protected])
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Abstract

We discuss recent literature data on the relaxation times (the primary tα), viscosity, and self-diffusion in water-glycerol and water-methanol mixtures across a wide temperature range from the stable water phase to the deep supercooled regime (373–147K). In particular, to clarify the role of hydrophilicity interactions (the hydrogen bonds) and hydrophobic interactions we study the mixture in terms of the water molar fraction (XW) with fixed temperatures at 5K steps across the entire composition range, and we find a marked deviation from the ideal thermodynamic behavior of the transport functions. This deviation is strongly T and XW dependent and spans values that range from two orders of magnitude at the highest temperature to more than five in the deeply supercooled regime (more precisely, at ≃200K). We analyze these deviations in terms of how the measured values differ from ideal values and find that the hydrogen-bonding water network dominates system properties up to XW = 0.3. We also examine an Arrhenius plot of the maximum excess value (Δtα(T) vs. 1/T) and find two significant changes due to water: one at the dynamical crossover temperature (TL ≃ 225K, i.e., the locus of the Widom line), and one at T ≃ 315K (the water isothermal compressibility χT minimum).

Keywords

liquidmixturewater
Type
Articles
Information
MRS Advances , Volume 1 , Issue 26: Theory, Characterization, and Modeling , 2016 , pp. 1891 - 1902
Copyright
Copyright © Materials Research Society 2016 

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