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Title: Experimental Determination of Dawsonite Stability and Reactivity: Implications for Geological CO2 Sequestration

Journal Article · · Geochimica et Cosmochimica Acta
 [1];  [2];  [2]
  1. Laboratoire des Mecanismes et Transferts en Geologie, Toulouse, France
  2. ORNL

Over the last decade, a significant research effort has focused on determining the feasibility of sequestering large amounts of CO{sub 2} in deep, permeable geologic formations to reduce carbon dioxide emissions to the atmosphere. Most models indicate that injection of CO{sub 2} into deep sedimentary formations will lead to the formation of various carbonate minerals, including the common phases calcite (CaCO{sub 3}), dolomite (CaMg(CO{sub 3}){sub 2}), magnesite (MgCO{sub 3}), siderite (FeCO{sub 3}), as well as the far less common mineral, dawsonite (NaAlCO{sub 3}(OH){sub 2}). Nevertheless, the equilibrium and kinetics that control the precipitation of stable carbonate minerals are poorly understood and few experiments have been performed to validate computer codes that model CO{sub 2} sequestration. In order to reduce this uncertainty we measured the solubility of synthetic dawsonite according to the equilibrium: NaAlCO{sub 3}(OH){sub 2(cr)} + 2H{sub 2}O{sub 1} {r_equilibrium}Al(OH){sub 4}{sup -} + HCO{sub 3}{sup -} + Na{sup +} + H{sup +}, from under- and oversaturated solutions at 50-200 C in basic media at 1.0 mol {center_dot} kg{sup -1} NaCl. The solubility products (Q{sub s}) obtained were extrapolated to infinite dilution to obtain the solubility constants (K{sub s}{sup o}). Combining the fit of these logK{sub s}{sup o} values and fixing {Delta}C{sub pJ}{sup o} at -185.5J {center_dot} mol{sup -1} {center_dot} K{sup -1} at 25 C, which was derived from the calorimetric data of Ferrante et al. [Ferrante, M.J., Stuve, J.M., and Richardson, D.W., 1976. Thermodynamic data for synthetic dawsonite. U.S. Bureau of Mines Report Investigation, 8129, Washington, D.C., 13p.], the following thermodynamic parameters for the dissolution of dawsonite were calculated at 25 C: {Delta}G{sub r}{sup o} = 102.1 kJ {center_dot} mol{sup -1}, {Delta}H{sub r}{sup o} = 97.0 kJ {center_dot} mol{sup -1} and {Delta}s{sub r}{sup o} = -17.1 J {center_dot} mol{sup -1} {center_dot} K{sup -1}. Subsequently, we were able to derive values for the Gibbs energy of formation {Delta}{sub {line_integral}}G{sup 0}{sub 298.15} = -1782 {+-} 2 kJ {center_dot} mol{sup -1}), enthalpy of formation ({Delta}{sub {line_integral}}H{sup o}{sub 298.15} = -1960 {+-} 7 kJ {center_dot} mol{sup -1}) and entropy (S{sup o}{sub 298.15} = 121 {+-} 2 J {center_dot} mol{sup -1} {center_dot} K{sup -1}) of dawsonite. These results are within the combined experimental uncertainties of the values reported by Ferrante et al. (1976). Predominance diagrams are presented for the dawsonite/boehmite and dawsonite/bayerite equilibria at 100 C in the presence of a saline solution with and without silica-containing minerals.

Research Organization:
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
Sponsoring Organization:
USDOE Office of Science (SC)
DOE Contract Number:
DE-AC05-00OR22725
OSTI ID:
1021929
Journal Information:
Geochimica et Cosmochimica Acta, Vol. 71, Issue 18; ISSN 0016-7037
Country of Publication:
United States
Language:
English