Abstract

Classical molecular dynamics (MD) simulations have been performed to investigate the effects of substitutions in the octahedral sheet (Mg for Al) and layer charge on an atomistic model of the montmorillonite edge. The edge models considered substitutions in both the solvent accessible and inaccessible octahedral positions of the edge bond chain for a representative edge surface. The MD simulations based on CLAYFF, a fully-flexible forcefield widely used in the MD simulations of bulk clay minerals, predicted Mg–O bond distances at the edge and in bulk that agreed with those of the density functional theory (DFT) geometry optimizations and available experimental data. The DFT results for the edge surfaces indicated that substitutions in the solvent inaccessible positions of the edge bond chain are energetically favorable and an increase in layer charge and local substitution density coincided with the occurrence of five-coordinate, square pyramidal Mg and Al edge structures. Both computational methods predicted these square pyramidal structures, which are stabilized by water bridging H-bonds between the unsaturated bridging oxygen [(Al or Mg)–O–Si] and other surface O atoms. The MD simulations predict that the presence of Mg substitutions in the edge bond chain results in increased disorder of the edge Al polyhedra relative to the unsubstituted edge. In addition to the square pyramidal Al, these disordered structures include trigonal bipyramidal and tetrahedral Al at the edge and inverted Si tetrahedra. These simulation results represent the first test of the fully-flexible CLAYFF forcefield for classical MD simulations of the Na-monmorillonite edge and demonstrate the potential of combined classical MD simulations and DFT geometry-optimizations to elucidate the edge structure of 2:1 phyllosilicate minerals.

Highlights

  • Smectites are 2:1 dioctahedral phyllosilicates abundant in soils and sediments [1]

  • We report the results of molecular dynamics (MD) simulations of a MMT edge with substitutions of Mg for Al in the octahedral sheet using the CLAYFF forcefield

  • We provide a quantitative description of the octahedral sheet edge structures and infer a relationship between layer charge and disordered edge structures

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Summary

Introduction

Smectites are 2:1 dioctahedral phyllosilicates abundant in soils and sediments [1]. Smectites are natural nanominerals with layers ~1.0 nm thick composed of an octahedral sheet between two tetrahedral sheets. The hydration of interlayer cations that balance this permanent charge results in interlayer swelling and the creation of nanopores This physical structure is responsible for the unique physicochemical properties of smectites that include high surface area, high cation exchange capacity, and low permeability. These microscopic properties affect a range of macroscopic geological and geochemical processes and have been exploited in engineered geologic barriers [2,3] and nanocomposite materials [4,5,6]. These applications have been developed based on the comprehensive experimental and theoretical investigations of the smectite

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