Melting curve of (Mg,Fe)SiO3 perovskite to 96 GPa: Evidence for a structural transition in lower mantle melts

E Knittle, R Jeanloz - Geophysical Research Letters, 1989 - Wiley Online Library
Geophysical Research Letters, 1989Wiley Online Library
The melting temperature of (Mg, Fe) SiO3 perovskite, the dominant mineral phase of the
Earth's lower mantle, has been measured to a pressure of 96 (±10) GPa. Below 60 GPa we
find good agreement with the previous measurement of Heinz and Jeanloz [1987a], and
above 60 GPa the melting curve of silicate perovskite has a small positive slope of 19.5
(±5.5) K/GPa. The melting point of (Mg0. 9Fe0. 1) SiO3 perovskite is 3800 (±300) K at 96
GPa; by extrapolation to 136 GPa, it is 4500 (±500) K at the core‐mantle boundary. These …
The melting temperature of (Mg,Fe)SiO3 perovskite, the dominant mineral phase of the Earth's lower mantle, has been measured to a pressure of 96 (±10) GPa. Below 60 GPa we find good agreement with the previous measurement of Heinz and Jeanloz [1987a], and above 60 GPa the melting curve of silicate perovskite has a small positive slope of 19.5 (±5.5) K/GPa. The melting point of (Mg0.9Fe0.1)SiO3 perovskite is 3800 (±300) K at 96 GPa; by extrapolation to 136 GPa, it is 4500 (±500) K at the core‐mantle boundary. These values provide an upper limit to the geotherm through the solid mantle, and they are compatible with recent estimates of the temperature in the core being high (∼4500 K at the core‐mantle boundary). Our melting curve implies that the volume change on melting increases at 60 GPa from ΔVm = 0.0 (±0.2) cm³/mole to ΔVm ≅ 0.16 (±0.03) cm³/mole. We derive an equation of state for the melt from our data, and find that a highly coordinated structure is required to explain the molar volume of liquid (Mg,Fe)SiO3 at pressures above ∼ 20 GPa.
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