Progress in Earth and Planetary Science· 2026Q1
Carbon solubility and liquid–liquid immiscibility in Fe–C–S ternary system up to 6 GPa: implications for the core of small planetary bodies
- 1citations
- Q1SCImago
- 2026year
Short summary
Fe-C-S liquids show immiscibility at 2-4 GPa but not at 5-6 GPa, as increased sulfur limits carbon solubility at higher pressures.
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Key points
- Fe-C-S liquids separate into C-rich and S-rich phases at 2 and 4 GPa.
- Immiscibility is suppressed at 5-6 GPa due to sulfur limiting carbon solubility.
- Carbon solubility decreases with increasing sulfur content at higher pressures.
- Planetary bodies with cores >5 GPa are unlikely to exhibit liquid-liquid immiscibility.
AI-generated from the title and abstract; the full text is not read.
Abstract
Abstract High-pressure, high-temperature experiments were conducted in a multi-anvil press using seven different starting compositions to investigate the phase relations of Fe–C–S liquids at pressures up to 6 GPa and temperatures up to 2000 K. Quenched samples revealed immiscible C-rich and S-rich metallic liquids at 2 and 4 GPa, manifesting as either large immiscible zones or emulsified smaller droplets. On the contrary, no immiscibility was observed at 5 or 6 GPa. At these higher pressures, the carbon solubility limit, significantly reduced by increasing sulfur content in the ternary liquid, prevents the formation of a liquid phase rich in both C and S. Our findings thus indicate that super-liquidus immiscibility in Fe-rich compositions does not occur at pressures above 5 GPa, due to the differential pressure dependence of C solubility and miscibility. The limited C solubility in S-rich liquids at higher pressures effectively suppresses immiscibility. Based on these results, terrestrial planetary bodies with fluid cores at pressures exceeding 5 GPa are unlikely to experience liquid–liquid immiscibility, even when both carbon and sulfur are abundant, as sulfur limits carbon solubility and promotes its exsolution. For the Moon, immiscibility-induced core stratification is not expected, though local emulsification could occur near the core–mantle boundary (CMB). In smaller bodies, a two-liquid Fe–C–S core may form at high temperatures, but progressive cooling may lead to graphite crystallization and the potential development of a graphitic crust.
The authors' abstract, as published at the source. Progress in Earth and Planetary Science, 2026 · DOI ↗
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