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Abstract
In this article, we present three mesoscopic models for water. All three models
make use of local density-dependent interaction potentials, as employed within the Pagonabarraga-Frenkel framework [I. Pagonabarraga and D. Frenkel, J. Chem. Phys., 2001, 115, 5015–5026]. The forms of these three interaction potentials are based on the free energy function of the SAFT-VR Mie equation of state (EoS) [T. Lafitte et al., J. Chem. Phys., 2013, 139, 154504]. Two of these models represent the water-water interaction as a spherically symmetric Mie interaction with temperature-dependent parameters, whilst the third model works with a temperature-independent Mie potential, but then explicitly models the effect of hydrogen bonding. All three models provide good predictions of the vapor-liquid equilibrium of water over a wide temperature range. They also give accurate predictions of the isothermal compressibility for both sub- and supercritical conditions. To model the interfacial tension of the vapor-liquid interface with our mesoscale simulations, we added a square-gradient term to our potential
energy function. We show that the addition of this term has a minimal effect on
the bulk properties of water. However, by parameterising the coefficient of this term as a function of temperature, all three models again provide excellent predictions of water’s interfacial tension over a wide temperature range. Of the three models, our preference is for the model that includes an association term, as this model can operate successfully over a wider range of conditions.
make use of local density-dependent interaction potentials, as employed within the Pagonabarraga-Frenkel framework [I. Pagonabarraga and D. Frenkel, J. Chem. Phys., 2001, 115, 5015–5026]. The forms of these three interaction potentials are based on the free energy function of the SAFT-VR Mie equation of state (EoS) [T. Lafitte et al., J. Chem. Phys., 2013, 139, 154504]. Two of these models represent the water-water interaction as a spherically symmetric Mie interaction with temperature-dependent parameters, whilst the third model works with a temperature-independent Mie potential, but then explicitly models the effect of hydrogen bonding. All three models provide good predictions of the vapor-liquid equilibrium of water over a wide temperature range. They also give accurate predictions of the isothermal compressibility for both sub- and supercritical conditions. To model the interfacial tension of the vapor-liquid interface with our mesoscale simulations, we added a square-gradient term to our potential
energy function. We show that the addition of this term has a minimal effect on
the bulk properties of water. However, by parameterising the coefficient of this term as a function of temperature, all three models again provide excellent predictions of water’s interfacial tension over a wide temperature range. Of the three models, our preference is for the model that includes an association term, as this model can operate successfully over a wider range of conditions.
Original language | English |
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Pages (from-to) | 1836–1845 |
Journal | The Journal of Physical Chemistry Part B |
Volume | 129 |
Issue number | 6 |
Early online date | 30 Jan 2025 |
DOIs | |
Publication status | Published - 13 Feb 2025 |
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