TY - JOUR
T1 - Liquidus and solidus temperatures of a Fe-O-S alloy up to the pressures of the outer core
T2 - Implication for the thermal structure of the Earth's core
AU - Terasaki, H.
AU - Kamada, S.
AU - Sakai, T.
AU - Ohtani, E.
AU - Hirao, N.
AU - Ohishi, Y.
N1 - Funding Information:
The authors acknowledge N. Sata, N. Nishitani, M. Murakami, and K. Kobayashi for their technical assistance. This work was partly supported by the Grants-in-Aid for Scientific Research from the Ministry of Education, Culture, Science, and Sport and Technology of the Japanese Government to E. O. (no. 18104009 ) and by the “ Global Education and Research Center for the Earth and Planetary Dynamics ”. The experiments were performed under contract at SPring-8 (proposal numbers: 2008B1582, 2009A1570 and 2009B0028).
PY - 2011/4/15
Y1 - 2011/4/15
N2 - The solidus and liquidus temperatures of the Fe75O5S20 alloy are determined up to 157GPa using a laser-heated diamond anvil cell combined with in situ X-ray diffraction technique. Fe (fcc/hcp), Fe3S2/Fe3S, and FeO B1/B8/rhombohedral phases are stable under subsolidus conditions. First, Fe3S2 or Fe3S phase melts at a temperature close to the eutectic point of the Fe-Fe3S system, suggesting that the alloying effect of 5at.% oxygen on the eutectic temperature in the Fe-Fe3S system is minor. Then FeO melts at several hundreds of degrees Kelvin higher than the solidus, and Fe is a liquidus phase in this system. The liquidus temperature is 260-670K lower than the melting temperature of pure Fe because of the alloying effect of S and O on the melting temperature of Fe. Based on our results, the temperatures at the core/mantle boundary (TCMB) and at the boundary of the inner/outer core (TICB) are estimated to be 3600±200<TCMB<4310±350K and TICB~5630±350K, respectively. These results provide important constraints on the thermal structure of the Earth's core.
AB - The solidus and liquidus temperatures of the Fe75O5S20 alloy are determined up to 157GPa using a laser-heated diamond anvil cell combined with in situ X-ray diffraction technique. Fe (fcc/hcp), Fe3S2/Fe3S, and FeO B1/B8/rhombohedral phases are stable under subsolidus conditions. First, Fe3S2 or Fe3S phase melts at a temperature close to the eutectic point of the Fe-Fe3S system, suggesting that the alloying effect of 5at.% oxygen on the eutectic temperature in the Fe-Fe3S system is minor. Then FeO melts at several hundreds of degrees Kelvin higher than the solidus, and Fe is a liquidus phase in this system. The liquidus temperature is 260-670K lower than the melting temperature of pure Fe because of the alloying effect of S and O on the melting temperature of Fe. Based on our results, the temperatures at the core/mantle boundary (TCMB) and at the boundary of the inner/outer core (TICB) are estimated to be 3600±200<TCMB<4310±350K and TICB~5630±350K, respectively. These results provide important constraints on the thermal structure of the Earth's core.
KW - Core
KW - Fe-alloy
KW - High pressure
KW - Melting temperature
KW - Thermal structure
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U2 - 10.1016/j.epsl.2011.02.041
DO - 10.1016/j.epsl.2011.02.041
M3 - Article
AN - SCOPUS:79953035856
VL - 304
SP - 559
EP - 564
JO - Earth and Planetary Sciences Letters
JF - Earth and Planetary Sciences Letters
SN - 0012-821X
IS - 3-4
ER -