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Carbon in the Earth’s core Yingwei Fei Geophysical Laboratory Carnegie Institution of Washington
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Carbon Budget Carbon in the solar system Relatively abundant (e.g., 12xSi) Carbon in the meteorites Iron meteorites (0.01-0.6 wt%) Carbonaceous chondrites (~3.2 wt%) Carbon in the Earth Range from 0.07 to 1.5(?) wt% Carbon in the core Uncertain octahedrite cohenite
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Key factors affecting carbon budget in the Earth and core Earth formation models Element volatility trend Core formation models Mantle/core carbon partitioning
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The relative abundances of elements in the Earth and various carbonaceous chondrites vs. the log of the 50% condensation temperature at 10 -4 atm pressure McDonough [2003] => 0.07 wt% C in the Earth
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Other considerations Pressure effect Planetary accretion and differentiation Carbon added during and after accretion => Higher C in the Earth (>1.5 wt%) Wood [1993]
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Carbon in the core Carbon in the mantle? Carbon partitioning between mantle and core? Carbon partitioning between inner and outer cores?
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Geophysical constraints 6-10% density deficit (outer core) ~2% density deficit (inner core) FeNi alloy + 8-12 wt% light elements S, C, O, Si, H… Earth core Li and Fei [2007]
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Criteria for light elements Density consideration - PVT data Density-velocity relationship - velocity measurements Inner-outer core density difference - element partitioning btw solid and liquid Temperature - melting relations
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Birch’s law - velocity vs. density FeS 2 FeSi FeO FeS Pure Fe PREM Fiquet et al. [2008]
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Melting relations in the Fe-C System at High Pressure Shterenberg et al. [1975] Tsuzuki et al. [1984] Wood [1993] Fei et al. [2007] 1 bar
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Melting relations in the Fe-C system at 20 GPa Fe Liquid Fe+Fe 3 C Fe 3 CFe Fe-C Melt Fe Fe+liq
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Melting relations in the Fe-C system at 20 GPa Fe Liquid Fe+Fe 3 C Fe 3 CFe Fe 3 C
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Melting relations in the Fe-C system at 20 GPa Fe Liquid Fe+Fe 3 C Fe 3 CFe Fe-C Melt Fe 3 C Fe 3 C+L
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Melting relations in the Fe-C system at 20 GPa Fe Liquid Fe+Fe 3 C Fe 3 CFe Fe-C Melt 10µm
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Fe-C System at High Pressure Fei et al. [2007] 1 bar Core temperature Inner core mineralogy Weight% Carbon 5 GPa 10 GPa FeFe 7 C 3 Fe 3 C Temperature, K
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Effect of pressure on eutectic temperature Fe melting Fe-C eutectic melting Fe-S eutectic melting
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Challenges Effect of carbon on liquid and solid iron densities at outer and inner core conditions, respectively. Melting relations at IOC boundary (329 GPa) Partitioning of C between silicate and metallic iron up to CMB conditions Multi-component systems including other light elements such as S, O, and Si
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Solutions TEM NanoSIMS Laser-heating DAC 5µm FIB Synchrotron X-ray Field emission microprobe
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Multi-anvil lab
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Melting in the Fe-C-S system 1.0 GPa 3.6 GPa 4.8 GPa6.2 GPa 25µm
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Melting in the Fe-C-S system C O S
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P = 20 GPa,T = 1375 ˚C Fe-C-S melt C-bearing Fe
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Core stratification may occur in small planetary bodies. Implications: The solid inner core is nearly S-free, but it could contain significant amount of carbon, whereas the liquid outer core would be S-rich and C-poor. Fe-C-S melt C-bearing Fe
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>Melting over a wide pressure range Differentiation of planetary bodies (large or small) occurs through extensive melting
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Melting composition change as a function of pressure Eutectic C C solubility in metallic Fe Wood, EPSL, 1993
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Conclusions The eutectic temperature of Fe-C system increases with increasing pressure Carbon solubility in metallic iron increases with increasing pressure whereas eutectic composition remains constant If carbon is an important component of the Earth’s core, the inner core would crystallize as C-bearing Fe, rather than iron carbide such as Fe 3 C In the Fe-C-S system, we found liquid miscibility gap closure at high pressure. Metallic Fe crystallizes with significant amount of C and negligible S, implying that C is more likely in the solid inner core than S
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Solutions Extend pressure range Use of laser-heating diamond anvil cell Nano analysis
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Multi-Anvil Apparatus Capable of generating pressures up to 27 GPa and reaching temperatures above 2500 K Fe Fe-C Melt
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