Abstract

The solubility of rutile was measured in H 2O, H 2O–SiO 2 and H 2O–NaAlSi 3O 8 fluids at 700–1000 °C, 0.7–2.0 GPa, in a piston-cylinder apparatus. Solubility was determined by weight loss using a double-capsule method. Rutile solubility in pure H 2O shows isothermal increase with pressure ( P), isobaric increase with temperature ( T), and is low at all conditions investigated (6–118 ppm Ti). Rutile solubility in H 2O is given by log c Ti ° = 6.173 − 5425/ T + 178.4 P/ T, where c Ti ° is Ti concentration in ppm, T is in K, and P in GPa. This leads to thermodynamic properties of the reaction rutile = TiO 2,aq of Δ S r ° = 28.6 J/mol K, Δ H r ° = 104 kJ/mol, and Δ V r ° = − 3.4 cm 3/mol. At 800 °C and 1 GPa, addition of SiO 2 (up to quartz saturation) did not change rutile solubility relative to that in pure H 2O. Determination of rutile solubility in H 2O–NaAlSi 3O 8 fluids was complicated by incongruent dissolution of albite to paragonite or corundum + fluid; however, fluid compositions could be estimated within narrow limits using a mass-balance scheme. The solubility of rutile increases linearly with dissolved Na–Al silicate at fixed P and T, as described by c Ti = c Ti ° + Bw s where c Ti is ppm Ti, w s is wt.% dissolved silicate and B is given by log B 6.512 − 1.665 P − 6224/ T + 2215 P/ T, with T and P again in K and GPa. The results help explain discrepancies among previous studies of rutile solubility in H 2O at similar P and T. The new data agree within error with those of Tropper and Manning [Tropper, P., Manning, C.E., 2005. Very low solubility of rutile in H 2O at high pressure and temperature, and its implications for Ti mobility in subduction zones. American Mineralogist 90, 502–505.], but give lower solubility than earlier piston-cylinder-based determinations due to suppression of new crystal growth in the present experiments. However, the new data yield higher solubilities than are predicted from a hydrothermal diamond-anvil study, probably because of our longer run times and more complete equilibration. Combination of predicted Ti concentrations in melt-saturated H 2O with H 2O-saturated albite melts suggests that the melt–vapor partition coefficient for Ti is constant at 9.5 ± 1.5 from 700 to 900 °C at 1 GPa and rutile saturation, implying that an H 2O-rich magmatic vapor phase can transport significant Ti in mid- to deep-crustal settings. Because crustal and mantle fluids will contain alkalis, Al and Si, the results in H 2O–NaAlSi 3O 8 fluids provide a better foundation for modeling high- P metasomatic processes than pure H 2O values. The strong increase in rutile solubility with dissolved Na–Al silicate suggests that complexing with these constituents promotes Ti mobility and transport during fluid–rock interaction in the lower crust and upper mantle.

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