Abstract

The interface between water and folded proteins is very complex. Proteins have "patchy" solvent-accessible areas composed of domains of varying hydrophobicity. The textbook understanding is that these domains contribute additively to interfacial properties (Cassie's equation, CE). An ever-growing number of modeling papers question the validity of CE at molecular length scales, but there is no conclusive experiment to support this and no proposed new theoretical framework. Here, we study the wetting of model compounds with patchy surfaces differing solely in patchiness but not in composition. Were CE to be correct, these materials would have had the same solid-liquid work of adhesion (WSL ) and time-averaged structure of interfacial water. We find considerable differences in WSL , and sum-frequency generation measurements of the interfacial water structure show distinctively different spectral features. Molecular-dynamics simulations of water on patchy surfaces capture the observed behaviors and point toward significant nonadditivity in water density and average orientation. They show that a description of the molecular arrangement on the surface is needed to predict its wetting properties. We propose a predictive model that considers, for every molecule, the contributions of its first-nearest neighbors as a descriptor to determine the wetting properties of the surface. The model is validated by measurements of WSL in multiple solvents, where large differences are observed for solvents whose effective diameter is smaller than ∼6 Å. The experiments and theoretical model proposed here provide a starting point to develop a comprehensive understanding of complex biological interfaces as well as for the engineering of synthetic ones.

Highlights

  • The interface between water and folded proteins is very complex

  • Such complexity affects a number of interfacial properties ranging from the work of adhesion [WSL, the main component in the interfacial energy [2]] to the very complex time-averaged structure of interfacial water (TASIW) [3]

  • To tackle this question, we have developed model compounds, i.e., gold nanoparticles coated with SAMs composed of a binary mixture of hydrophobic and hydrophilic ligands that separate into patches [15, 16]

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Summary

Contact angle AFM

These simulations demonstrate that the nonadditivity in the systems containing trenches is due to the water structure at the boundary between 2 types of ligand These systems contain only straight boundaries between ligands of different types, and do not provide an exhaustive list of possible nearestneighbor configurations, limiting the power of a model based on trench systems to predict the results of a general surface. For this reason, we generated a set of simulation boxes in which the ligands in each site on both the top and the bottom surfaces were chosen randomly. Reevaluating those data, we find that the subset of solvent that showed a nonmonotonic dependence on ligand-shell composition is x10-3 40

DMSO GLY IPA
Findings
Materials and Methods
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