TY - JOUR
T1 - Is the inner core of the Earth pure iron?
AU - Jephcoat, Andrew
AU - Olson, Peter
PY - 1987
Y1 - 1987
N2 - The properties of the inner core (1C) of the Earth are widely assumed to be consistent with those of pure, solid iron in the hexagonal close-packed (ε) phase. This hypothesis is re-examined here using a density model of the Earth's core generated from extrapolated, static high-pressure data for ε iron and pyrite. Densities of constant-composition mixtures at room temperature and core pressures are compared with corresponding Earth-model densities. An effective volume thermal expansivity, αeff, is calculated for a range of expected core temperatures that brings the room-temperature density into agreement with the Earth-model density at the pressure of the inner-core boundary (ICB). It seems that αeff would have to be significantly larger than previous estimates of the thermal expansion at core conditions. A qualitatively similar conclusion is obtained if an isotherm reduced from shock-wave data is used for ε iron instead of the static data. We argue that, o several explanations for this difference (errors in Earth-model densities, a high-volume thermal expansivity at megabar pressures, a high-temperature core (>7,000 K), and the presence of a light component), the last alternative is the most probable and that the IC is not, therefore, pure iron.
AB - The properties of the inner core (1C) of the Earth are widely assumed to be consistent with those of pure, solid iron in the hexagonal close-packed (ε) phase. This hypothesis is re-examined here using a density model of the Earth's core generated from extrapolated, static high-pressure data for ε iron and pyrite. Densities of constant-composition mixtures at room temperature and core pressures are compared with corresponding Earth-model densities. An effective volume thermal expansivity, αeff, is calculated for a range of expected core temperatures that brings the room-temperature density into agreement with the Earth-model density at the pressure of the inner-core boundary (ICB). It seems that αeff would have to be significantly larger than previous estimates of the thermal expansion at core conditions. A qualitatively similar conclusion is obtained if an isotherm reduced from shock-wave data is used for ε iron instead of the static data. We argue that, o several explanations for this difference (errors in Earth-model densities, a high-volume thermal expansivity at megabar pressures, a high-temperature core (>7,000 K), and the presence of a light component), the last alternative is the most probable and that the IC is not, therefore, pure iron.
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U2 - 10.1038/325332a0
DO - 10.1038/325332a0
M3 - Article
AN - SCOPUS:0023163836
SN - 0028-0836
VL - 325
SP - 332
EP - 335
JO - Nature
JF - Nature
IS - 6102
ER -