Abstract

BackgroundMany important geochemical and biogeochemical reactions occur in the mineral/formation water interface of the highly abundant mineral, goethite [α-Fe(OOH)]. Ab initio molecular dynamics (AIMD) simulations of the goethite α-FeOOH (100) surface and the structure, water bond formation and dynamics of water molecules in the mineral/aqueous interface are presented. Several exchange correlation functionals were employed (PBE96, PBE96 + Grimme, and PBE0) in the simulations of a (3 × 2) goethite surface with 65 absorbed water molecules in a 3D-periodic supercell (a = 30 Å, FeOOH slab ~12 Å thick, solvation layer ~18 Å thick).ResultsThe lowest energy goethite (100) surface termination model was determined to have an exposed surface Fe3+ that was loosely capped by a water molecule and a shared hydroxide with a neighboring surface Fe3+. The water molecules capping surface Fe3+ ions were found to be loosely bound at all DFT levels with and without Grimme corrections, indicative that each surface Fe3+ was coordinated with only five neighbors. These long bonds were supported by bond valence theory calculations, which showed that the bond valence of the surface Fe3+ was saturated and surface has a neutral charge. The polarization of the water layer adjacent to the surface was found to be small and affected only the nearest water. Analysis by density difference plots and localized Boys orbitals identified three types of water molecules: those loosely bound to the surface Fe3+, those hydrogen bonded to the surface hydroxyl, and bulk water with tetrahedral coordination. Boys orbital analysis showed that the spin down lone pair orbital of the weakly absorbed water interact more strongly with the spin up Fe3+ ion. These weakly bound surface water molecules were found to rapidly exchange with the second water layer (~0.025 exchanges/ps) using a dissociative mechanism.ConclusionsWater molecules adjacent to the surface were found to only weakly interact with the surface and as a result were readily able to exchange with the bulk water. To account for the large surface Fe–OH2 distances in the DFT calculations it was proposed that the surface Fe3+ atoms, which already have their bond valence fully satisfied with only five neighbors, are under-coordinated with respect to the bulk coordination.Graphical abstractAll first principle calculations, at all practically achievable levels, for the goethite 100 aqueous interface support a long bond and weak interaction between the exposed surface Fe3+ and water molecules capping the surface. This result is supported by bond valence theory calculations and is indicative that each surface Fe3+ is coordinated with only 5 neighbors.

Highlights

  • Many important geochemical and biogeochemical reactions occur in the mineral/formation water interface of the highly abundant mineral, goethite [α-Fe(OOH)]

  • In this article we report results using Ab initio molecular dynamics (AIMD) simulations to predict the structural, bonding and dynamical properties of the solvated (~6 water layers) goethite (100) surface

  • To establish the accuracy of the density functional theory (DFT) PBE96 approach used in this manuscript, we evaluated its accuracy by calculating the bulk structural properties of the perfect goethite crystal

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Summary

Introduction

Many important geochemical and biogeochemical reactions occur in the mineral/formation water interface of the highly abundant mineral, goethite [α-Fe(OOH)]. As the thermodynamically most stable Fe-oxyhydroxide, goethite(α-FeOOH) occurs widely in natural environments [1,2,3] and is the dominant reactive mineral in lake and marine sediments [4]. It is found in weathering products, primary hydrothermal minerals, acid mine drainage precipitates, bog and marine environments [3,4,5] and has been observed in abundance on Mars [6]. The crystal structure has a perfect cleavage on the (100) ((010) Pbnm) plane This plane (more clearly illustrated below) is not the main crystal growth surface of this mineral. It is a common surface and is cleaved to provide a well-structured surface for spectroscopic studies [22, 23]

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