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Eighth Condensed Phase and Interfacial Molecular Science (CPIMS)

Eighth Condensed Phase and Interfacial Molecular Science (CPIMS)

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Figure 2: Schematic on the effects of two<br />

different solvents on the surface adsorption<br />

of hard-sphere ions. Our results indicate<br />

that the driving force of ions to interfaces<br />

is model dependent [2].<br />

continuum theory to explain the surface tension of the<br />

halide salts. Levin <strong>and</strong> co-workers [Physical Review<br />

Letters 103, 257802 (2009)] have used a polarizable<br />

ion dielectric continuum theory to also explain the<br />

surface tension data of halide salts. Interestingly, the<br />

single ion potential of mean force (PMF) for iodide<br />

agrees quite well (regarding the depth of the shallow<br />

local minimum at the interface) with these two very<br />

different approaches. Our Recent DFT calculations<br />

that intrinsically include polarization also show good<br />

agreement with the aforementioned PMFs for iodide<br />

[10]. The question regarding the role of polarization<br />

<strong>and</strong> the connection of molecular simulation to<br />

dielectric continuum theory still remains. To this end,<br />

we constructed molecular simulations of charged hardspheres<br />

(HS) in model solvents (SPC/E <strong>and</strong><br />

Stockmayer fluid) where the separation of cavitation<br />

<strong>and</strong> dielectric response is clear (see Figure 2). We<br />

proposed a dielectric theory that contains the free<br />

energy of cavitation (proportional to volume of HS), <strong>and</strong> charging (proportional to square of the<br />

charge) where the dielectric constants <strong>and</strong> volume scaling was determined by molecular<br />

simulation [2]. Our results indicate that the underlying physics of anion adsorption is dependent<br />

on the nature of the solvent (e.g. SPC/E or Stockmayer). The symmetric nature of the<br />

Stockmayer fluid precludes the existence of a surface potential <strong>and</strong> it is only cavitation that<br />

determines surface activity. SPC/E water has a surface potential due to the broken symmetry of<br />

both the cavity <strong>and</strong> interface. It was shown in our study [2] <strong>and</strong> a recent independent study<br />

[Arslagarin <strong>and</strong> Beck, Journal of Chemical Physics 136, 104503 (2012)] that this notional<br />

“surface potential” provides an additional crucial driving force that allows point-charge models<br />

in SPC/E to give rise to surface adsorption.<br />

Future directions<br />

The role of this notional “surface potential” is currently being explored in the context of DFT<br />

<strong>and</strong> the use of inherently polarizable models for the solute <strong>and</strong> solvent (with G.K. Schenter).<br />

Future research will be extended to elucidation of the solvation <strong>and</strong> surface properties of more<br />

complex anions such as the oxyanions (with G.K. Schenter <strong>and</strong> J. Fulton) such as ClO3 - <strong>and</strong><br />

BrO3 - where both exhibit very interesting behavior in the context of the Hofmeister series. We<br />

are currently investigating the role of hydrophobic solvation with John D. Weeks. We are using<br />

multiple representations of the molecular interaction for water (e.g. TIP5P, SPC/E, flavors of<br />

DFT) to underst<strong>and</strong> the structural response to a model hydrophobe <strong>and</strong> the signatures of volume<br />

to area scaling.<br />

Acknowledgements. This work was performed with Yan Levin (Brazil) John D. Weeks (U.<br />

Maryl<strong>and</strong>), D.J. Tobias (UC-I), Ilja Siepmann (U. Minn.), <strong>and</strong> I.-F.W. Kuo (LLNL), Greg<br />

Schenter (PNNL), Liem Dang (PNNL), Marcel D. Baer (PNNL), Abe Stern (UC-I), Joost<br />

V<strong>and</strong>eVondele (U. Zurich), Greg Kimmel (PNNL), John Fulton (PNNL), Roger Rousseau<br />

(PNNL) <strong>and</strong> Shawn M. Kathmann ( PNNL).<br />

137

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