Al3Ni: enthalpy of formation
13 accepted literature formation-enthalpy value(s) (experimental 4, model 8, DFT 1); experimental median -38.5 kJ/mol-atom (n = 3); Materials Project -39.068 kJ/mol-atom (mp-aaabjkld); OQMD -39.608 kJ/mol-atom (oqmd-10517).
Systems: Al–Co–Cr–Ni · Al–Ni
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -43.2 unspecified ± 1.1 | Al3Ni | 1073 | experimental | direct reaction calorimetry | Al–Ni | [1] Chen 2011 cites Chrifi-Alaoui 2004 doi | p. 4 report | The enthalpy of formation of the Al3 Ni phase has recently been determined by Chrifi-Alaoui et al. using direct reaction calorimetry [16]. It was reported to be -43.2 ± 1.1 kJ/mol-atoms relative to fcc Al and fcc Ni at 1073 K, by adopting the heat content of pure elements from Barin and Platzki [17]. |
| -41 kJ/mol-atom | Al3Ni | 298.15 | experimental | Al–Ni | [1] Chen 2011 cites Chrifi-Alaoui 2004 doi | Table 1, p. 4, row 1 report | ||
| -38.5 kJ/mol-atom | Al3Ni | 298.15 | experimental | Al–Ni | [1] Chen 2011 cites Oelsen 1937 | Table 1, p. 4, row 2 report | ||
| -37.7 kJ/mol-atom | Al3Ni | 298.15 | experimental | Al–Ni | [1] Chen 2011 cites Kubaschewski 1958 doi | Table 1, p. 4, row 3 report | ||
| -69.8016 kJ/mol (basis unstated) | Al0.75Ni0.25 | 298.15 | model | Al–Ni | [2] Ansara 1988 | Table 1, p. 5, row 9 report | ||
| -48 kJ/mol-atom | Al3Ni | 298.15 | model | Al–Ni | [1] Chen 2011 cites Dupin 2001 doi | Table 1, p. 4, row 6 report | ||
| -42.1 kJ/mol-atom | Al3Ni | 298.15 | model | Al–Ni | [1] Chen 2011 cites Shi 2009 doi | Table 1, p. 4, row 5 report | ||
| -40.7 kJ/mol-atom | Al3Ni | 298.15 | model | Al–Ni | [1] Chen 2011 | Table 1, p. 4, row 7 report | ||
| -39.6 kJ/mol-atom | Al3Ni | 298.15 | model | Al–Ni | [1] Chen 2011 cites Wang 2009 | Table 1, p. 4, row 4 report | ||
| -37.656 kJ/mol (basis unstated) | Al0.75Ni0.25 | 298.15 | model | Al–Ni | [2] Ansara 1988 cites Hultgren 1973 | Table 1, p. 5, row 10 report | ||
| -22.9 kJ/mol-atom | γ'-L12 | 298.15 | model | Al–Co–Cr–Ni | [3] Liu 2016 cites ref. 86 | Table 4, p. 38, row 19 report | ||
| -21.6 kJ/mol (basis unstated) | L12-Al3Ni | model | CALPHAD | Al–Ni | [4] Yang 2022 | Table 3, p. 5, row 1 report | ||
| -21.919 kJ/mol (basis unstated) | L12-Al3Ni | DFT | DFT (OQMD) | Al–Ni | [4] Yang 2022 | Table 3, p. 5, row 2 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 |
|---|---|---|---|---|---|---|---|---|
| -43.2 | unspecified | 1.1 | 0.05 | unit 'unspecified' not convertible to kJ/mol-atom | 1.1 | |||
| -41 | kJ/mol-atom | 0.05 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -38.5 | kJ/mol-atom | 0.05 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -37.7 | kJ/mol-atom | 0.05 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -69.8016 | kJ/mol (basis unstated) | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -48 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -42.1 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -40.7 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -39.6 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -37.656 | kJ/mol (basis unstated) | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -22.9 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -21.6 | kJ/mol (basis unstated) | 0.05 | 15.6 (model_calculated, calibrated) | 15.6 | ||||
| -21.919 | kJ/mol (basis unstated) | 5.000e-4 | 15.72 (dft, calibrated) | 15.72 |
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-aaabjkld | -39.068 | -0.404916 | Pnma | 0 | 0 | no |
| OQMD | oqmd-10517 | -39.608 | -0.410514 | Pnma | 0 | 0 | no |
| OQMD | oqmd-344444 | -21.441 | -0.222218 | Pm-3m | 18.1678 | 0.1883 | yes |
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
- H.-L. Chen, E. Doernberg, P. Svoboda, R. Schmid-Fetzer, Thermodynamics of the Al3Ni phase and revision of the Al–Ni system, Thermochimica Acta 512, 189-195 (2011). doi:10.1016/j.tca.2010.10.005
- I. Ansara, B. Sundman, P. Willemin, Thermodynamic modeling of ordered phases in the NiAl system, Acta Metallurgica 36, 977-982 (1988). doi:10.1016/0001-6160(88)90152-6
- Xuan L. Liu, Greta Lindwall, Thomas Gheno, Zi-Kui Liu, Thermodynamic modeling of Al–Co–Cr, Al–Co–Ni, Co–Cr–Ni ternary systems towards a description for Al–Co–Cr–Ni, Calphad 52, 125-142 (2016). doi:10.1016/j.calphad.2015.12.007
- Wei Yang, Peisheng Wang, Xiaozhong Huang, Shuyan Zhang, Thermodynamic analysis of the Al–Ni system, Intermetallics 149, 107647 (2022). doi:10.1016/j.intermet.2022.107647