Melt-crystal density crossover in a deep magma ocean

被引:76
作者
Caracas, Razvan [1 ,2 ]
Hirose, Kei [3 ,4 ]
Nomura, Ryuichi [3 ,5 ]
Ballmer, Maxim D. [3 ,6 ,7 ]
机构
[1] Ecole Normale Super Lyon, CNRS, Lab Geol Lyon, UMR 5276, F-69364 Lyon, France
[2] Univ Oslo, CEED, Oslo, Norway
[3] Tokyo Inst Technol, Earth Life Sci Inst, Meguro Ku, Tokyo 1528550, Japan
[4] Univ Tokyo, Grad Sch Sci, Dept Earth & Planetary Sci, Bunkyo Ku, Tokyo 1130033, Japan
[5] Ehime Univ, Geodynam Res Ctr, Matsuyama, Ehime 7908577, Japan
[6] Swiss Fed Inst Technol, Inst Geophys, CH-8092 Zurich, Switzerland
[7] UCL, Dept Earth Sci, London WC1E 6BT, England
基金
欧洲研究理事会;
关键词
magma ocean; density crossover; pyrolite; bridgmanite; molecular dynamics; early Earth; MOLECULAR-DYNAMICS; MANTLE CONDITIONS; HIGH-PRESSURE; GIANT IMPACT; PERIDOTITE; LIQUID; EARTH; MOON; DIFFUSION; SOLIDUS;
D O I
10.1016/j.epsl.2019.03.031
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
The crystallization of a magma ocean (MO) early in Earth's history shaped the entire evolution of our planet. The buoyancy relations between the forming crystals and the residual melt is the most important but also the most unknown parameter affecting the large-scale structure and evolution of the MO. The accumulation of crystals, near the depth of neutral buoyancy between crystals and the coexisting melt, if happening at mid-depths, can separate convecting regions within the MO. Here we use jointly first-principles molecular-dynamics calculations and diamond-anvil cell experiments to obtain the density relations between the molten bulk silicate Earth and the bridgmanite crystals during the crystallization of the MO. The chemical evolutions of the liquid and the coexisting solid during progressive crystallization were constrained by experiments, and the relevant densities were calculated by molecular dynamics. We find that the first crystal of bridgmanite that is formed in a fully molten mantle is Fe-poor, and becomes neutrally buoyant at 110-120 GPa. Since the cooling of the deep MO is fast, and related convection is vigorous, however, first crystals remain entrained. As crystallization advances, the relative Fe content increases in the melt, and the pressure of neutral buoyancy decreases. At 50% solidification, close to the rheological transition, the pressure of the density crossover moves to similar to 50 GPa. At this pressure, crystals form an interconnected network and block global convection currents, which in turn leads to the separation of the partly crystallized MO into a surficial MO and a basal MO through melt-solid segregation. Such a shallow segregation of a crystal mush at mid-mantle depth has important implications for the dynamics and timescales of early mantle differentiation. Moreover, the shallow segregation should have promoted the formation of a voluminous basal MO that evolves into a large geochemically enriched reservoir. Accordingly, the seismically observed residues of basal MO crystallization in the present-day mantle may host an unmixed reservoir for the missing budget of highly incompatible elements. (C) 2019 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
引用
收藏
页码:202 / 211
页数:10
相关论文
共 50 条
[1]  
Abe Y., 1995, The Earth's Central Part: Its Structure and Dynamics, P215
[2]   The Argon constraints on mantle structure. [J].
Allegre, CJ ;
Hofmann, A ;
ONions, K .
GEOPHYSICAL RESEARCH LETTERS, 1996, 23 (24) :3555-3557
[3]   Solid-liquid iron partitioning in Earth's deep mantle [J].
Andrault, Denis ;
Petitgirard, Sylvain ;
Lo Nigro, Giacomo ;
Devidal, Jean-Luc ;
Veronesi, Giulia ;
Garbarino, Gaston ;
Mezouar, Mohamed .
NATURE, 2012, 487 (7407) :354-+
[4]   Solidus and liquidus profiles of chondritic mantle: Implication for melting of the Earth across its history [J].
Andrault, Denis ;
Bolfan-Casanova, Nathalie ;
Lo Nigro, Giacomo ;
Bouhifd, Mohamed A. ;
Garbarino, Gaston ;
Mezouar, Mohamed .
EARTH AND PLANETARY SCIENCE LETTERS, 2011, 304 (1-2) :251-259
[5]   BAND THEORY AND MOTT INSULATORS - HUBBARD-U INSTEAD OF STONER-I [J].
ANISIMOV, VI ;
ZAANEN, J ;
ANDERSEN, OK .
PHYSICAL REVIEW B, 1991, 44 (03) :943-954
[6]   Structure and density of basaltic melts at mantle conditions from first-principles simulations [J].
Bajgain, Suraj ;
Ghosh, Dipta B. ;
Karki, Bijaya B. .
NATURE COMMUNICATIONS, 2015, 6
[7]   Reconciling magma-ocean crystallization models with the present-day structure of the Earth's mantle [J].
Ballmer, Maxim D. ;
Lourenco, Diogo L. ;
Hirose, Kei ;
Caracas, Razvan ;
Nomura, Ryuichi .
GEOCHEMISTRY GEOPHYSICS GEOSYSTEMS, 2017, 18 (07) :2785-2806
[8]   Compositional layering within the large low shear-wave velocity provinces in the lower mantle [J].
Ballmer, Maxim D. ;
Schumacher, Lina ;
Lekic, Vedran ;
Thomas, Christine ;
Ito, Garrett .
GEOCHEMISTRY GEOPHYSICS GEOSYSTEMS, 2016, 17 (12) :5056-5077
[9]   Numerical solution of a non-linear conservation law applicable to the interior dynamics of partially molten planets [J].
Bower, Dan J. ;
Sanan, Patrick ;
Wolf, Aaron S. .
PHYSICS OF THE EARTH AND PLANETARY INTERIORS, 2018, 274 :49-62
[10]   142Nd evidence for early (>4.53 Ga) global differentiation of the silicate Earth [J].
Boyet, M ;
Carlson, RW .
SCIENCE, 2005, 309 (5734) :576-581