5:15 PM - 6:45 PM
[SGC33-P04] Hf and W partitioning between liquid metal and silicate melt calculated by using ab initio free energy calculations: implications for the evolution of 182W isotope of the earth.
Keywords:W isotope, first-principle calculation, core-mantle interaction, partitioning of W and Hf
To understand the 182W variations in the mantle and their evolution, it is necessary to focus on the behavior of Hf and W under high pressure and the influence of extraterrestrial materials such as meteorite impacts. μ182W variations can be attributed to three possible processes. (1) Hf-W fractionation in the mantle. First-principles calculations (Deng and Stixrude, 2021) report that Hf is enriched in bridgmanite; however, the isotopic results are not consistent with the Hf enrichment of bridgmanite subducted into the lower mantle. (2) Hf-W fractionation occurred during core formation. (Mundl et al., 2017; Rizo et al., 2017) (3) Extraterrestrial material with low μ182W fell to the surface by intermittent impact.
It is, thus, important to constrain the partition behavior of Hf and W between silicate and metal for better understanding of the evolution of 182W isotopes. However, it has been difficult to determine the partition coefficients of Hf and W in laboratory experiments because of their low concentration and also the nugget effects of the highly siderophile elements such as W. In this study, we investigated the Hf-W partitioning as HfO2, HfO3 and WO2 between silicate melts and molten iron under high temperature and pressure conditions using ab initio free energy calculations. We also calculated whether the distribution coefficient changes when iron is mixed with silicate and vice versa. The distribution coefficients of W and Hf were not significantly affected by the addition of Fe to the silicate melt, while the mixing of Fe with O decreased and increased the distribution coefficients of W and Hf, respectively. Importantly, however, in both cases, W and Hf remained siderophile and lithophile, respectively, under the calculated conditions, which is consistent with the model in (2). In the future, it is necessary to clarify the evolution of the μ182W while taking into account the models in (2) and (3).