Abstract

To more completely assess the primary magmatic origin of Ru–Os–Ir (IPGE) alloys, we conducted experiments to evaluate the effects of T, fO 2, fS 2 and melt composition on the solubility of Ru in molten Fe–Ni–sulfide. Fe–Ni–S melt+Ru were held in olivine crucibles, and experiments were done in a vertical-tube gas-mixing furnace at 1200–1400 °C for 1–5 days. At constant fO 2 and fS 2, Ru solubility increases with T, and a similar result is obtained if fO 2 is varied parallel to the fayalite–magnetite–quartz buffer (FMQ), with fS 2 levels to maintain sulfide liquid saturation. At log fS 2 of −1.7, Ru solubility decreases from ∼11 wt.% at log fO 2 of −10.8, to ∼0.3 wt.% at log fO 2 of −8.1. At a log fO 2 of −8.6, a similar reduction in Ru solubility occurred as log fS 2 decreased from −0.9 to −3.0. Substitution of Ni for Fe in the sulfide results in an increase in Ru solubility, with values ranging from ∼3 wt.% at Fe/Ni of 36 to ∼10 wt.% at Fe/Ni of 6 (log fO 2, fS 2 of −9.1, −1.7, respectively). Dilution of Ru with a 1:1 mix of Os+Ir results in a 4- and 10-fold decrease in melt Ru content for alloys with ∼60 and 35 mol% Ru, respectively. For the fO 2– fS 2 conditions required for sulfide liquid saturation in natural basaltic magmas, pure Ru solubility in molten sulfide is expected to exceed 10 wt.%, and dilution by Os+Ir is still likely to require wt.% levels of Ru for IPGE alloy saturation. Since Ru abundances of ore-grade massive sulfide is <50 ppm, our results would preclude IPGE alloy saturation in the presence of immiscible sulfide liquid. Activity–composition relations determined for Ru in ternary Ru–Os–Ir alloy suggest, however, that the concentration of Ru in molten silicate required for alloy saturation is at or below levels in natural, high Mg igneous rocks, implying such alloys could form in sulfide-undersaturated systems. The negative fO 2 dependence of Ru solubility in sulfide liquid is opposite that for Ru (and other PGEs) in silicate melt, suggesting that a decrease in fO 2 will favor the partitioning of Ru into the sulfide liquid. However, it is not clear how much this effect will be offset by the concomitant reduction in fS 2 required to maintain saturation in immiscible sulfide liquid. Comparison of our Ru solubility data with values determined in silicate melt yields apparent sulfide–silicate melt partition coefficients that exceed 10 7, which is more than 1000× larger than direct measurements on coexisting sulfide–silicate compositions. Possible reasons for this discrepancy are that (1) measured sulfide–silicate partition coefficients are inaccurate due to incomplete phase separation, (2) non-Henryian activity–composition relations at high Ru concentrations, (3) Ru solubilities in silicate melt measured at both high fO 2 and in the absence of sulfur cannot be accurately extrapolated to the low fO 2 and sulfur-bearing conditions of previous two-liquid partitioning experiments.

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