2009
DOI: 10.1016/j.jcis.2009.06.051
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Comparison of molecular dynamics simulations with triple layer and modified Gouy–Chapman models in a 0.1 M NaCl–montmorillonite system

Abstract: Molecular dynamics (MD) simulations of a montmorillonite/water interface at the pore scale were carried out at 0.1molL(-1) NaCl concentration in order to constrain cation, anion, and water distribution and mobility influenced by the mineral surface. MD results enabled anion exclusion and cation condensation at the surface to be quantified. MD-derived values could then be compared with macroscopic model results obtained from the Modified Gouy-Chapman (MGC) theory. While the Na concentration profile is well repr… Show more

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Cited by 125 publications
(136 citation statements)
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“…The simplifying assumption to consider a volumetric mass of water of 1000 kg/m 3 is therefore confirmed in the limit of the measurement precision. It may be noted that adsorbed water locally has a density above one (see for example molecular dynamics results from Wang et al 2006or Tournassat et al, 2009b) but this density must be similar to 1000 kg/dm 3 when normalized to three layers of external water, taking into account the density oscillations with domains also at density below 1000 kg/m 3 .…”
Section: Comparison Of Hto Accessible Porosity and Nmr Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The simplifying assumption to consider a volumetric mass of water of 1000 kg/m 3 is therefore confirmed in the limit of the measurement precision. It may be noted that adsorbed water locally has a density above one (see for example molecular dynamics results from Wang et al 2006or Tournassat et al, 2009b) but this density must be similar to 1000 kg/dm 3 when normalized to three layers of external water, taking into account the density oscillations with domains also at density below 1000 kg/m 3 .…”
Section: Comparison Of Hto Accessible Porosity and Nmr Resultsmentioning
confidence: 99%
“…The number of water layers in the interlayer depends on the nature of the interlayer cations and on the compaction degree (Kozaki et al, 1998;Ferrage et al, 2005). The external surface water structure and properties can be probed by a molecular dynamics study showing significant density oscillations up to three water layers at phyllosilicate mineral surfaces (Greathouse and Cygan, 2006;Wang et al, 2006;Marry et al, 2008;Tournassat et al, 2009b).…”
Section: Introductionmentioning
confidence: 99%
“…In various studies it has been found that the ionic mobility of the counterion species in the Stern and diffuse layers is close to the mobility of this species in the bulk pore electrolytic solution b + f [e.g., Tarasov and Titov, 2007;Leroy et al, 2008]. This can be explained by the location of the counterion on the outer Helmholtz plane of the Stern layer, where it keeps its hydration shell [Tournassat et al, 2009;Jougnot et al, 2010;Revil and Florsch, 2010]. This might be different for counterion species with a higher affinity to the mineral surface and for minerals with permanent structural charges on their basal surface (e.g., illite and smectite) [Leroy and Revil, 2009].…”
Section: Ec Polarizationmentioning
confidence: 93%
“…The results agree with several recent findings, whereby a Stern layer of fixed cations charge balance the clay, and the simulations refute the double layer expansion hypothesis of lowsalinity EOR in this instance. 35,36 DLVO theory states that for a sufficiently highly charged clay-like surface, a Stern layer of immobile cations will be adsorbed to the clay, and act as a buffer to cancel the charge of the clay. The oscillatory nature of the electric field presented in Figure 5 can be described in this manner, whereby an immobile layer of cations charge balanced the clay, followed sequentially by a mobile layer of anions and cations.…”
Section: Double Layer Effectsmentioning
confidence: 99%