Abstract
The proton-induced surface charge of magnetite was investigated in 0.03 and 0.30 molal sodium trifluoromethanesulfonate solutions from 25°C to 290°C by potentiometric titrations using a stirred hydrogen electrode concentration cell. Pure magnetite with excellent crystallinity was produced by reaction with the Ni/NiO/H2O hydrogen fugacity buffer at 500°C. Inflection points in the 0.03 molal proton sorption isotherms (pH(infl)) at 6.50, 6.24, 5.65, 5.47, 5.31 and 5.55 at temperatures of 50°C, 100°C, 150°C, 200°C, 250°C and 290°C, respectively, were used as estimates of the pristine point of zero charge (pH(ppzc)) for modeling purposes. These pH(infl) values parallel 1/2 pK(w) and agree within the assigned uncertainty (±0.3 pH units) at all temperatures with independent estimates of the pH(ppzc) calculated from an extension of 88the revised MUSIC model. The surface charging can be adequately described by a one-p K model with a surface protonation constant fitted to the pH(infl) values, and giving the standard state thermodynamic properties log K(H,298) = 7.00, Δ H298° = -32.4 ± 0.8 kJ/mol and constant Δ C(p) = 128 ± 16 J K-1 mol-1, with Δ S298°assumed to be equal to that of rutile protonation (25.5 ± 3.4 J K-1 mol-1. The 0.03 and 0.30 molal proton sorption isotherms also exhibit pHs of common intersection (pH(cip)) at 6.33, 5.78, 5.37, 4.82, 4.62 and 4.90 at 50°C, 100°C, 150°C, 200°C, 250°c and 290°C, respectively. The difference between the pH(cip) and pH(ppzc) κ pH(infl) values can be related to specific binding of Na+ on the negatively charged surface, which increases with increasing temperature, although the pH(cip) values may also be affected by dissolution of the solid. The electrical double layer model includes a basic Stern layer capacitance, with specific cation and anion binding at the Stern layer, and a fixed diffuse layer capacitance computed from Guoy-Chapman theory. To fit the steepness and asymmetry of the charging curves above the pH(ppzc), an additional cation binding constant was invoked, which allows the cation to experience the surface potential. Significant kinetically controlled dissolution of magnetite was observed below the pH(ppzc), which may be a result of leaching of Fe2+ from the surface, to produce a magnetite + hematite assemblage, despite the high hydrogen partial pressures (ca. 10 bars) used in these experiments. (C) 2000 Elsevier Science B.V. All rights reserved.
Original language | English |
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Pages (from-to) | 193-229 |
Number of pages | 37 |
Journal | Chemical Geology |
Volume | 167 |
Issue number | 1-2 |
DOIs | |
State | Published - Jun 5 2000 |
Funding
This study was funded in part by the Office of Basic Energy Sciences, US Department of Energy, under contract DE-AC05-96OR22464 with Oak Ridge National Laboratory, managed by Lockheed Martin Energy Research. MLM also received support from the Illinois State Water Survey and the Illinois Department of Natural Resources, as well as the National Science Foundation (EAR-9627784). The authors wish to thank Dr. J. Stucki of the University of Illinois and B. Moskowitz of the University of Minnesota for their help in characterizing the solid phases used in this study, and also Dr. J.P. Jolivet of the Université Pierre and Marie Curie for providing an unpublished manuscript on the magnetite structure and surface protonation constants. We also thank Dr. T. Hiemstra and W.H. Van Riemsdijk of Wageningen Agricultural University for many helpful discussions. This manuscript was greatly improved by thorough reviews by Jean Pierre Jolivet and Dimitri Sverjensky.
Keywords
- Magnetite
- Point of zero charge
- Potentiometric titration
- Surface protonation