Density-Pressure Profiles of Fe-Bearing MgSiO3 Liquid: Effects of Valence and Spin States, and Implications for the Chemical Evolution of the Lower Mantle

被引:27
|
作者
Karki, Bijaya B. [1 ]
Ghosh, Dipta B. [2 ]
Maharjan, Charitra [2 ]
Karato, Shun-ichiro [1 ]
Park, Jeffrey [1 ]
机构
[1] Yale Univ, Dept Geol & Geophys, New Haven, CT 06520 USA
[2] Louisiana State Univ, Sch Elect Engn & Comp Sci, Baton Rouge, LA 70803 USA
基金
美国国家科学基金会;
关键词
silicate melts; density; spin transition; first-principles simulation; high pressure; EQUATION-OF-STATE; SEISMIC EVIDENCE; SILICATE PEROVSKITE; MELTING EXPERIMENTS; TRANSITION ZONE; WATER TRANSPORT; DEEP MANTLE; MAGMA OCEAN; AB-INITIO; IRON;
D O I
10.1029/2018GL077149
中图分类号
P [天文学、地球科学];
学科分类号
07 ;
摘要
Density is a key property controlling the chemical state of Earth's interior. Our knowledge about the density of relevant melt compositions is currently poor at deep-mantle conditions. Here we report results from first-principles molecular-dynamics simulations of Fe-bearing MgSiO3 liquids considering different valence and spin states of iron over the whole mantle pressure conditions. Our simulations predict the high-spin to low-spin transition in both ferrous and ferric iron in the silicate liquid to occur gradually at pressures around 100GPa. The calculated iron-induced changes in the melt density (about 8% increase for 25% iron content) are primarily due to the difference in atomic mass between Mg and Fe, with smaller contributions (<2%) from the valence and spin states. A comparison of the predicted density of mixtures of (Mg,Fe)(Si,Fe)O-3 and (Mg,Fe)O liquids with the mantle density indicates that the density contrast between the melt and residual-solid depends strongly on pressure (depth): in the shallow lower mantle (depths<1,000km), the melt is lighter than the solids, whereas in the deep lower mantle (e.g., the D-n layer), the melt density exceeds the mantle density when iron content is relatively high and/or melt is enriched with Fe-rich ferropericlase.
引用
收藏
页码:3959 / 3966
页数:8
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