Fe2Y: enthalpy of formation
27 accepted literature formation-enthalpy value(s) (experimental 3, model 19, DFT 5); experimental median -7.09 kJ/mol-atom (n = 2); Materials Project -6.024 kJ/mol-atom (mp-aaaaacik); OQMD -6.077 kJ/mol-atom (oqmd-18348).
Systems: Fe–Y
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -7.09 per mol-atom ± 0.61 | Fe2Y | 973 | experimental | EMF | Fe–Y | [1] Kardellass 2014 cites Subramanian 1984 doi | Table 4, p. 4, row 17 report | |
| -7.09 kJ/mol-atom ± 0.61 | Fe2Y | 973 | experimental | EMF | Fe–Y | [2] Saenko 2017 cites Subramanian 1984 doi | Table 5, p. 12, row 36 report | |
| -7.09 kJ/mol-atom ± 0.61 | Fe2Y | 973 | experimental | Exp | Fe–Y | [3] Fan 2021 cites Subramanian 1984 doi | Table 3, p. 5, row 31 report | |
| -12.55 kJ/mol-atom | Fe2Y | 973 | model | Optimization | Fe–Y | [2] Saenko 2017 cites Kardellass 2014 doi | Table 5, p. 12, row 38 report | |
| -12.55 per mol-atom | Fe2Y | 973 | model | Optimization | Fe–Y | [1] Kardellass 2014 | Table 4, p. 4, row 18 report | |
| -12.47 kJ/mol-atom | Fe2Y | 298.15 | model | Opt | Fe–Y | [3] Fan 2021 cites Conclusions | Table 3, p. 5, row 36 report | |
| -12.47 kJ/mol-atom | Fe2Y | 298.15 | model | Optimization | Fe–Y | [2] Saenko 2017 cites Kardellass 2014 doi | Table 5, p. 12, row 35 report | |
| -12.47 per mol-atom | Fe2Y | 298.15 | model | Optimization | Fe–Y | [1] Kardellass 2014 | Table 4, p. 4, row 22 report | |
| -11.8 kJ/mol-atom | Fe2Y | 973 | model | Opt | Fe–Y | [3] Fan 2021 cites Conclusions | Table 3, p. 5, row 36 report | |
| -11.8 per mol-atom | Fe2Y | 973 | model | Optimization | Fe–Y | [1] Kardellass 2014 | Table 4, p. 4, row 19 report | |
| -11.8 kJ/mol-atom | Fe2Y | 973 | model | Optimization | Fe–Y | [2] Saenko 2017 cites Kardellass 2014 doi | Table 5, p. 12, row 39 report | |
| -9.99 per mol-atom | Fe2Y | 298.15 | model | Optimization | Fe–Y | [1] Kardellass 2014 | Table 4, p. 4, row 21 report | |
| -9.99 kJ/mol-atom | Fe2Y | 298.15 | model | Optimization | Fe–Y | [2] Saenko 2017 cites Kardellass 2014 doi | Table 5, p. 12, row 34 report | |
| -9.99 kJ/mol-atom | Fe2Y | 298.15 | model | Opt | Fe–Y | [3] Fan 2021 cites Conclusions | Table 3, p. 5, row 35 report | |
| -7.77 kJ/mol-atom | Fe2Y | 973 | model | Optimization | Fe–Y | [2] Saenko 2017 | Table 5, p. 12, row 37 report | |
| -7.77 kJ/mol-atom | Fe2Y | 973 | model | Opt | Fe–Y | [3] Fan 2021 cites Saenko 2017 doi | Table 3, p. 5, row 33 report | |
| -6.825 kJ/mol-atom | Fe2Y | 973 | model | Opt | Fe–Y | [3] Fan 2021 | Table 3, p. 5, row 29 report | |
| -6.412 kJ/mol-atom | Fe2Y | 298.15 | model | Opt | Fe–Y | [3] Fan 2021 | Table 3, p. 5, row 29 report | |
| -6.3 kJ/mol-atom | Fe2Y | 298.15 | model | Optimization | Fe–Y | [2] Saenko 2017 | Table 5, p. 12, row 33 report | |
| -6.3 kJ/mol-atom | Fe2Y | 298.15 | model | Opt | Fe–Y | [3] Fan 2021 cites Saenko 2017 doi | Table 3, p. 5, row 33 report | |
| -2 per mol-atom | Fe2Y | 298.15 | model | Prediction | Fe–Y | [1] Kardellass 2014 cites Miedema 1976 doi | Table 4, p. 4, row 20 report | |
| -1 kJ/mol-atom | Fe2Y | 298.15 | model | Prediction (a) | Fe–Y | [2] Saenko 2017 cites Niessen 1983 doi | Table 5, p. 12, row 32 report | |
| -7.87 kJ/mol-atom | Fe2Y | 0 | DFT | Ab initio | Fe–Y | [2] Saenko 2017 cites Mihalkovic 2004 doi | Table 5, p. 12, row 31 report | |
| -7.646 kJ/mol-atom | Fe2Y | 0 | DFT | DFT | Fe–Y | [3] Fan 2021 cites Mihalkovic 2004 doi | Table 3, p. 5, row 34 report | |
| -6.24 kJ/mol-atom | Fe2Y | 0 | DFT | DFT | Fe–Y | [3] Fan 2021 cites Jain 2013 doi | Table 3, p. 5, row 32 report | |
| -6.048 kJ/mol-atom | Fe2Y | 0 | DFT | DFT | Fe–Y | [3] Fan 2021 cites Kirklin 2015 doi | Table 3, p. 5, row 30 report | |
| -5.92 kJ/mol-atom | Fe2Y | 0 | DFT | DFT | Fe–Y | [3] Fan 2021 | Table 3, p. 5, row 28 report |
Uncertainty budget
Components kept separate, in the value's unit (literature SCHEMA.md, UNCERTAINTY_CALIBRATION.md): effective = max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter). The method floor is the robust between-study scatter of the method class in ORCHID (calibrated) or a documented prior; printed values and printed uncertainties are unchanged.
| Value | Unit | Printed | Reading | Method (class, basis) | Composition | Scatter | Conversion | Effective |
|---|---|---|---|---|---|---|---|---|
| -7.09 | per mol-atom | 0.61 | 0.005 | unit 'per mol-atom' not convertible to kJ/mol-atom | 0.61 | |||
| -7.09 | kJ/mol-atom | 0.61 | 0.005 | 4.6 (emf, cleaned_below_threshold) | 4.6 | |||
| -7.09 | kJ/mol-atom | 0.61 | 0.005 | 4.1 (experimental_unspecified, cleaned_below_threshold) | 4.1 | |||
| -12.55 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -12.55 | per mol-atom | 0.005 | unit 'per mol-atom' not convertible to kJ/mol-atom | unit 'per mol-atom' not convertible to kJ/mol-atom | ||||
| -12.47 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -12.47 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -12.47 | per mol-atom | 0.005 | unit 'per mol-atom' not convertible to kJ/mol-atom | unit 'per mol-atom' not convertible to kJ/mol-atom | ||||
| -11.8 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -11.8 | per mol-atom | 0.05 | unit 'per mol-atom' not convertible to kJ/mol-atom | unit 'per mol-atom' not convertible to kJ/mol-atom | ||||
| -11.8 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -9.99 | per mol-atom | 0.005 | unit 'per mol-atom' not convertible to kJ/mol-atom | unit 'per mol-atom' not convertible to kJ/mol-atom | ||||
| -9.99 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -9.99 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -7.77 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -7.77 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -6.825 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -6.412 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -6.3 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -6.3 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -2 | per mol-atom | 0.5 | unit 'per mol-atom' not convertible to kJ/mol-atom | unit 'per mol-atom' not convertible to kJ/mol-atom | ||||
| -1 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -7.87 | kJ/mol-atom | 0.005 | 3.929 (dft, calibrated) | 3.929 | ||||
| -7.646 | kJ/mol-atom | 5.000e-4 | 3.929 (dft, calibrated) | 3.929 | ||||
| -6.24 | kJ/mol-atom | 0.005 | 3.929 (dft, calibrated) | 3.929 | ||||
| -6.048 | kJ/mol-atom | 5.000e-4 | 3.929 (dft, calibrated) | 3.929 | ||||
| -5.92 | kJ/mol-atom | 0.005 | 3.929 (dft, calibrated) | 3.929 |
DFT formation energies
Lowest-energy entries at this composition. Materials Project and OQMD use different energy references and are never averaged. 1 eV/atom = 96.485 kJ/mol-atom.
| Source | Entry | kJ/mol-atom | eV/atom | Space group | E above hull (kJ/mol-atom) | E above hull (eV/atom) | Theoretical |
|---|---|---|---|---|---|---|---|
| Materials Project | mp-aaaaacik | -6.024 | -0.062438 | Fd-3m | 0 | 0 | no |
| OQMD | oqmd-18348 | -6.077 | -0.06298 | Fd-3m | 0 | 0 | no |
DFT sources: A. Jain et al., Commentary: The Materials Project: A materials genome approach to accelerating materials innovation, APL Materials 1 (2013) 011002. doi:10.1063/1.4812323 (CC BY 4.0); J. E. Saal et al., JOM 65 (2013) 1501-1509; S. Kirklin et al., npj Comput. Mater. 1 (2015) 15010. doi:10.1007/s11837-013-0755-4 (CC BY 4.0);
Sources
- S. Kardellass, C. Servant, N. Selhaoui, A. Iddaoudi, M. Ait Amar, L. Bouirden, A thermodynamic assessment of the iron–yttrium system, Journal of Alloys and Compounds 583, 598-606 (2014). doi:10.1016/j.jallcom.2013.07.010
- I. Saenko, O. Fabrichnaya, A. Udovsky, New Thermodynamic Assessment of the Fe-Y System, J. Phase Equilib. Diffus. 38, 684-699 (2017). doi:10.1007/s11669-017-0574-3
- Ling Fan, Chen Shen, Kun Hu, Huashan Liu, Hongbin Zhang, DFT Calculations and Thermodynamic Re-Assessment of the Fe-Y Binary System, J. Phase Equilib. Diffus. 42, 348-362 (2021). doi:10.1007/s11669-021-00887-9