(256e) Polarizable Contributions to the Surface Tension of Liquid Water | AIChE

(256e) Polarizable Contributions to the Surface Tension of Liquid Water

Authors 

Rivera, J. L. - Presenter, Universidad Michoacana de San Nicolas de Hidalgo
Starr, F. W. - Presenter, Wesleyan University
Cummings, P. T. - Presenter, Vanderbilt University
Paricaud, P. L. - Presenter, Ecole Nationale Supérieure des Techniques Avancées


Surface tension, γ, strongly affects interfacial properties in fluids. The degree to which polarizability affects in water is thus far not well established. To address this situation, we carry out molecular dynamics (MD) simulations to study the interfacial forces acting on a slab of liquid water surrounded by vacuum using the Gaussian Charge Polarizable (GCP) model [1] at 298.15 K. The GCP model incorporates both a fixed dipole due to Gaussian distributed charges and a polarizable dipole. We find a well-defined bulk-like region forms with a width of ≈ 31 Å. The average density of the bulk-like region agrees with the experimental value of 0.997 g/cm3. However, we find that the orientation of the molecules in the bulk-like region is strongly influenced by the interfaces, even at a distance 5 molecular diameters from the interface. Specifically, the orientation of both the permanent and induced dipoles show a preferred orientation parallel to the interface. Near the interface, the preferred orientation of the dipoles becomes more pronounced and the average magnitude of the induced dipoles decreases monotonically. To quantify the degree to which molecular orientation affects γ, we calculate the contributions to γ from permanent dipolar interactions, induced dipolar interactions, and dispersion forces. We find that the induced dipole interactions and the permanent dipole interactions, as well as the cross interactions, have positive contributions to γ, and therefore contribute stability to the interface. The repulsive core interactions result in a negative contribution to γ, which nearly cancels the positive contributions from the dipoles. The large negative core contributions to γ are the result of small oxygen?oxygen separation between molecules. These small separations occur due to the strong attractions between hydrogen and oxygen atoms. The final predicted value for γ (68.65 mN/m) shows a deviation of ≈ 4 % of the experimental value of 71.972 mN/m [2]. The inclusion of polarization is critical for this model to produce an accurate value.

[1] P. Paricaud, M. Predota, A. A. Chiavo, and P. T. Cummings, J. Chem. Phys. 122, 244511 (2005). [2] N. B. Vargaftik, V. N. Volkov, and L. D. Voljak, J. Phys. Chem. Ref. Data 12, 817 (1983).