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First‐principles study of density, viscosity, and diffusion coefficients of liquid MgSiO3 at conditions of the Earth's deep mantle

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TLDR
In this paper, the diffusion coefficients and shear viscosities of MgSiO3 at conditions near the Earth's core-mantle boundary were determined for different thermodynamic conditions.
Abstract
[1] Constant-pressure constant-temperature ab initio molecular dynamics simulations at high temperatures have been used to study MgSiO3, the major constituent of the Earth's lower mantle to conditions of the Earth's core-mantle boundary. The calculated equilibrium volumes and densities are compared with simulations using an orthorhombic perovskite configuration under the same conditions. For molten MgSiO3, we have determined the diffusion coefficients and shear viscosities at different thermodynamic conditions. Our results provide new constraints on the properties of molten MgSiO3 at conditions near the core-mantle boundary. The volume of the liquid is greater than that of the solid throughout the pressure-temperature conditions examined, and the volume change on fusion ranges from 5% at 88 GPa and 3500 K to 2.9% at 120 GPa and 5000 K. Existing experimental constraints on solid-liquid partition coefficients for Fe suggest that Fe is preferentially partitioned into the liquid. Such enrichment of Fe increases the density of the liquid, thus allowing the possibility of negatively buoyant melts from (Mg,Fe)SiO3 perovskite compositions at deep lower mantle conditions for plausible values of solid-liquid partition coefficients for Fe. At 120 GPa and 4500–5000 K, the diffusion coefficient of liquid MgSiO3 is 2–3 × 10−5 cm 2/s and the diffusion rates of the different chemical species are similar. The shear viscosity is estimated using Zwanzig's formula to be 19–31 cP under these conditions. On the basis of our calculated diffusivities, MgSiO3 is above the glass transition temperature at 120 GPa and 4500 K.

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Journal ArticleDOI

Thermodynamics of silicate liquids in the deep Earth

TL;DR: In this paper, the authors discuss the geophysical implications of recent first principles molecular dynamics simulations of MgSiO3 liquid, in particular the findings that the Gruneisen parameter increases by a factor of three on two-fold compression, and the predicted melting curve.
Journal ArticleDOI

The MgSiO3 system at high pressure: Thermodynamic properties of perovskite, postperovskite, and melt from global inversion of shock and static compression data

TL;DR: In this paper, the authors presented new equation-of-state (EoS) data acquired by shock loading to pressures up to 245 GPa on both low-density samples (MgSiO_3 glass) and high-density, polycrystalline aggregates (mgSi O_3 perovskite + majorite).
Journal ArticleDOI

Self-consistent thermodynamic description of silicate liquids, with application to shock melting of MgO periclase and MgSiO3 perovskite

TL;DR: In this article, a self-consistent thermodynamic description of silicate liquids applicable across the entire mantle pressure and temperature regime was developed, which combines the finite strain free energy expansion with an account of the temperature dependence of liquid properties into a single fundamental relation.
Journal ArticleDOI

Origin of HIMU and EM-1 domains sampled by ocean island basalts, kimberlites and carbonatites: The role of CO2-fluxed lower mantle melting in thermochemical upwellings

TL;DR: In this article, the authors show that the parent/daughter isotope ratios of the enriched mantle (EM) and high-μ (HIMU) mantle reservoirs sampled by ocean island basalt (OIB), kimberlite and carbonatite magmas are produced entirely by CO2-fluxed melting in the lower mantle.
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Computer modeling of natural silicate melts: What can we learn from ab initio simulations

TL;DR: In this paper, the structural and dynamical properties of four silicate liquids (silica, rhyolite, a model basalt and enstatite) are evaluated by ab initio molecular dynamics simulation using the density functional theory and are compared with classical simulations using a simple empirical force field.
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