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Abstract <p>Subsolidus phase relations in the Fe–Ni–S system were studied in a multianvil press at 6 GPa, 450°C, and a duration of 17 h using ceramic capsules. The nine intermediate compounds were established: FeS<sub>2</sub> pyrite (Ni# ≤ 7), NiS<sub>2</sub> vaesite (Ni# ≥ 96), (Fe, Ni)<sub>1 –</sub> <sub><i>x</i></sub>S (Ni# 0–100), (Ni, Fe)<sub>4</sub>S<sub>3</sub> (S# 42–44, Ni# ≥ 60), Ni<sub>3</sub>S<sub>2</sub> heazlewoodite (S# 40, Ni# ≥ 97), Ni<sub>3 –</sub> <sub><i>x</i></sub>S (S# 26, Ni# 100), Ni<sub>3.5</sub>Fe<sub>0.5</sub>S (S# 21, Ni# 87), and metal phase (Ni# 64–68), where Ni# = Ni/(Ni + Fe) × 100 mol % and S# = S/(S + Ni + Fe) × 100 mol %. A wide solubility gap between disulfides results in two large three-phase fields: (Fe<sub>0.93</sub>Ni<sub>0.07</sub>)S<sub>2</sub> + S + (Ni<sub>0.96</sub>Fe<sub>0.04</sub>)S<sub>2</sub> and (Fe<sub>0.93</sub>Ni<sub>0.07</sub>)S<sub>2</sub> + (Ni<sub>0.96</sub>Fe<sub>0.04</sub>)<sub>1 –</sub> <sub><i>x</i></sub>S + (Ni<sub>0.96</sub>Fe<sub>0.04</sub>)S<sub>2</sub>. A narrow field of monosulfide solid-solution is sandwiched between FeS<sub>2</sub> + (Fe, Ni)<sub>1 –</sub> <sub><i>x</i></sub>S and (Fe, Ni)S + (Ni, Fe)<sub>4</sub>S<sub>3</sub> two-phase fields. Large three-phase fields: Fe<sub>0.88</sub>Ni<sub>0.12</sub> Fe<sub>0.78</sub>Ni<sub>0.22</sub>S + Fe<sub>0.65</sub>Ni<sub>0.35</sub>, Ni<sub>063</sub>Fe<sub>0.37</sub> + Fe<sub>0.78</sub>Ni<sub>0.22</sub>S + (Ni<sub>0.6</sub>Fe<sub>0.4</sub>)<sub>4</sub>S<sub>3</sub>, and Fe<sub>0.32</sub>Ni<sub>068</sub> + (Fe<sub>0.3</sub>Ni<sub>0.7</sub>)<sub>4</sub>S<sub>3</sub> + Fe<sub>0.05</sub>Ni<sub>0.95</sub> appear at bulk S# &lt; 50. Stabilization of a new phase, Ni<sub>3.5</sub>Fe<sub>0.5</sub>S, yields two large three-phase fields: Ni<sub>3.5</sub>Fe<sub>0.5</sub>S + (Fe<sub>0.3</sub>Ni<sub>0.7</sub>)<sub>4</sub>S<sub>3</sub> + Ni<sub>3</sub>S<sub>2</sub> and Ni<sub>3.5</sub>Fe<sub>0.5</sub>S + Ni<sub>3</sub>S<sub>2</sub> + Ni.</p>

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Subsolidus Phase Relations in the System Fe–Ni–S at 450°C and 6 GPa

  • 期刊论文

  • 发表日期：

    2025年12月1日

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  • A. Shatskiy,
  • D. E. Sidko

摘要

Abstract

Subsolidus phase relations in the Fe–Ni–S system were studied in a multianvil press at 6 GPa, 450°C, and a duration of 17 h using ceramic capsules. The nine intermediate compounds were established: FeS2 pyrite (Ni# ≤ 7), NiS2 vaesite (Ni# ≥ 96), (Fe, Ni)1 – xS (Ni# 0–100), (Ni, Fe)4S3 (S# 42–44, Ni# ≥ 60), Ni3S2 heazlewoodite (S# 40, Ni# ≥ 97), Ni3 – xS (S# 26, Ni# 100), Ni3.5Fe0.5S (S# 21, Ni# 87), and metal phase (Ni# 64–68), where Ni# = Ni/(Ni + Fe) × 100 mol % and S# = S/(S + Ni + Fe) × 100 mol %. A wide solubility gap between disulfides results in two large three-phase fields: (Fe0.93Ni0.07)S2 + S + (Ni0.96Fe0.04)S2 and (Fe0.93Ni0.07)S2 + (Ni0.96Fe0.04)1 – xS + (Ni0.96Fe0.04)S2. A narrow field of monosulfide solid-solution is sandwiched between FeS2 + (Fe, Ni)1 – xS and (Fe, Ni)S + (Ni, Fe)4S3 two-phase fields. Large three-phase fields: Fe0.88Ni0.12 Fe0.78Ni0.22S + Fe0.65Ni0.35, Ni063Fe0.37 + Fe0.78Ni0.22S + (Ni0.6Fe0.4)4S3, and Fe0.32Ni068 + (Fe0.3Ni0.7)4S3 + Fe0.05Ni0.95 appear at bulk S# < 50. Stabilization of a new phase, Ni3.5Fe0.5S, yields two large three-phase fields: Ni3.5Fe0.5S + (Fe0.3Ni0.7)4S3 + Ni3S2 and Ni3.5Fe0.5S + Ni3S2 + Ni.