Abstract

The pressures existing in the outer liquid core of the earth are 130 to 328 GPa. Seismic data demonstrate that the density of the liquid core is some 8 to 10% less than pure iron. Equations of state of Fe-Si, Fe3C, C, FeS2, FeS, KFeS2 and FeO, over the appropriate pressure interval, and a range of possible core temperatures (3500 to 5000 K), can be used to place constraints on the cosmochemically plausible light element constituents of the core (Si, C, S, K and O). The seismically derived density profile allows from 14 to 20 wt. % Si in the outer core. The inclusion of Si or, possibly C (up to 11 wt. %), in the core is possible if, the earth accreted inhomogeneously within a region of the solar nebulae in which a C/0 (atomic) ratio of ≃ 1 existed, as compared to C/0 ∼ 0.6 for the present solar photosphere. In contrast, homogeneous accretion permits Si but not C, to enter the core via reduction of silicates to metallic Fe-Si core material during the late stages of the accumulation of the earth. The equation of state data for the iron sulfides allow up to 8 to 12% S in the core. This composition would provide the entire earth, with a S/Si ratio in the range 0.14 to 0.3 comparable to meteoritic and cosmic abundances. Shock-wave data for KFeS2 give little evidence for an electronic phase change from 4-s to 3-d orbitals which has been suggested to occur in K and allow the earth to store a cosmic abundance of K in the metallic core.

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