C–Fe system
12 accepted literature values from 2 paper(s) (experimental 3, model 3, unspecified 6); 0 calculated phase diagram(s). 17 further extracted value(s) not accepted by the reader-agreement checks are only in the JSON/CSV.
Data: JSON · CSV · interactive explorer · phases (12) · papers (bibliography) · Markdown
| Evidence class | Values |
|---|---|
| experimental | 3 |
| model | 3 |
| unspecified | 6 |
| Property group | Values |
|---|---|
| invariant reaction | 6 |
| phase transition | 6 |
Convex hulls: Materials Project DFT hull · OQMD DFT hull · CALPHAD hull FeC-10Hal · CALPHAD hull FeC-14Nar-3g · CALPHAD hull FeC-16Goh · CALPHAD hull FeC-19Che · CALPHAD hull FeC-19Mie · CALPHAD hull FeC-20Sae · CALPHAD hull FeC-23Jac · CALPHAD hull FeC-85Gus-LB
Invariant reactions (literature)
| T (K) | Reaction / phases | Compositions (mole fraction) | Class | Source | Location | Quote |
|---|---|---|---|---|---|---|
| 1768.15 | peritectic: L + α -> γ | unspecified | [1] Kumar 1991 | Table 7, p. 6, row 2 report | ||
| 1630.15 | peritectic: L + gr -> κ | unspecified | [1] Kumar 1991 | Table 7, p. 6, row 3 report | ||
| 1601.15 | eutectic: L -> α + κ | unspecified | [1] Kumar 1991 | Table 7, p. 6, row 4 report | ||
| 1488.15 | peritectic: L + α -> ε | unspecified | [1] Kumar 1991 | Table 7, p. 6, row 10 report | ||
| 1427.15 | eutectic: L -> γ + gr | unspecified | [1] Kumar 1991 | Table 7, p. 6, row 17 report | ||
| 1011.15 | other: γ -> α + gr | unspecified | [1] Kumar 1991 | Table 7, p. 6, row 23 report |
Other properties
Phase transition (6)
| Property | Value | T (K) | Phases / composition | Class | Source | Location | Quote |
|---|---|---|---|---|---|---|---|
| Phase transition | 470 K | 470 | other | model | [2] Naraghi 2014 | p. 9 report | The intersection of the lines for cementite and Hägg carbide defines the triple point between α/χ/θ below which Hägg carbide is more stable than cementite. Similarly the intersection of the Hägg and eta carbides gives the α/η/χ triple point below which eta carbide is more stable than Hägg carbide. In the present evaluation these points are located at 720 K and 470 K respectively according to the… |
| Phase transition | 483 K | 483 | magnetic | experimental | [2] Naraghi 2014 cites Umemoto 2001 doi | p. 3 report | Cementite has an orthorhombic crystal structure with a ferromagnetic transition around 483 K [29]. |
| Phase transition | 485 K | 485 | magnetic | model | [2] Naraghi 2014 | p. 3 report | Due to the similarities of orthorhombic and fcc structures, p is selected as 0.25 for cementite as well, TC is set to 485 K and 〈β 〉θ is fitted to the experimental heat capacity data. |
| Phase transition | 520 K | 520 | magnetic | experimental | [2] Naraghi 2014 cites Cohn 1953 doi | p. 3 report | Hägg carbide also appears to be ferromagnetic with a Curie temperature around 520 K [36]. |
| Phase transition | 653 K | 653 | magnetic | experimental | [2] Naraghi 2014 cites Cohn 1953 doi | p. 3 report | ε=η-Fe2 C carbide also appears to have ferromagnetic properties for which Cohn and Hofer [36] gave a Curie temperature around 653 K. |
| Phase transition | 720 K | 720 | other | model | [2] Naraghi 2014 | p. 9 report | The intersection of the lines for cementite and Hägg carbide defines the triple point between α/χ/θ below which Hägg carbide is more stable than cementite. Similarly the intersection of the Hägg and eta carbides gives the α/η/χ triple point below which eta carbide is more stable than Hägg carbide. In the present evaluation these points are located at 720 K and 470 K respectively according to the… |
Sources
Reporting papers the values were read from (a value cited from another work names that work in its row).
- K. C. Hari Kumar, V. Raghavan, A Thermodynamic Analysis of the Al-C-Fe System, JPE 12, 275-286 (1991). doi:10.1007/bf02649916
- Reza Naraghi, Malin Selleby, John Ågren, Thermodynamics of stable and metastable structures in Fe–C system, Calphad 46, 148-158 (2014). doi:10.1016/j.calphad.2014.03.004