Nb7Ni6: enthalpy of formation
10 accepted literature formation-enthalpy value(s) (experimental 4, model 1, DFT 5); experimental median -22.735 kJ/mol-atom (n = 4); Materials Project -19.894 kJ/mol-atom (mp-aaackvmr); OQMD -19.955 kJ/mol-atom (oqmd-30782).
Systems: Nb–Ni
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -23 kJ/mol-atom | Nb7Ni6 | 298.15 | experimental | Experimental | Nb–Ni | [1] Santhy 2015 cites Hultgren 1973 | Table 6, p. 4, row 3 report | |
| -23 kJ/mol-atom ± 3 | Nb7Ni6 | 600.15 | experimental | Experimental | Nb–Ni | [1] Santhy 2015 cites Kubaschewski 2015 | Table 6, p. 4, row 2 report | |
| -22.47 kJ/mol-atom ± 2.2 | Nb7Ni6 | 298.15 | experimental | Experimental | Nb–Ni | [1] Santhy 2015 cites Argent 1959 | Table 6, p. 4, row 1 report | |
| -22.45 kJ/mol-atom | μ-Nb7Ni6 + µ-Nb7Ni6 | 298.15 | experimental | Nb–Ni | [2] Sun 2023 cites Argent 1959 | Table 6, p. 33, row 5 report | ||
| -20.76 kJ/mol-atom | Nb7Ni6 | 298.15 | model | Miedema | Nb–Ni | [1] Santhy 2015 cites Niessen 1988 doi | Table 6, p. 4, row 4 report | |
| -22.5 kJ/mol-atom | Nb7Ni6 | 0 | DFT | First-principle | Nb–Ni | [1] Santhy 2015 | Table 6, p. 4, row 5 report | |
| -20.63 kJ/mol-atom | μ-Nb7Ni6 + µ-Nb7Ni6 | 0 | DFT | DFT and phonon calculations | Nb–Ni | [2] Sun 2023 | Table 6, p. 33, row 3 report | |
| -20.5 kJ/mol-atom | μ-Nb7Ni6 + µ-Nb7Ni6 | 0 | DFT | DFT and phonon calculations | Nb–Ni | [2] Sun 2023 | Table 6, p. 33, row 4 report | |
| -20.43 kJ/mol-atom | μ-Nb7Ni6 + µ-Nb7Ni6 | 298.15 | DFT | DFT and phonon calculations | Nb–Ni | [2] Sun 2023 | Table 6, p. 33, row 4 report | |
| -20.38 kJ/mol-atom | μ-Nb7Ni6 + µ-Nb7Ni6 | 298.15 | DFT | DFT and phonon calculations | Nb–Ni | [2] Sun 2023 | Table 6, p. 33, row 3 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 |
|---|---|---|---|---|---|---|---|---|
| -23 | kJ/mol-atom | 0.5 | 4.1 (experimental_unspecified, cleaned_below_threshold) | 4.1 | ||||
| -23 | kJ/mol-atom | 3 | 0.5 | 4.1 (experimental_unspecified, cleaned_below_threshold) | 4.1 | |||
| -22.47 | kJ/mol-atom | 2.2 | 0.005 | 4.1 (experimental_unspecified, cleaned_below_threshold) | 4.1 | |||
| -22.45 | kJ/mol-atom | 0.005 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -20.76 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -22.5 | kJ/mol-atom | 0.05 | 3.929 (dft, calibrated) | 3.929 | ||||
| -20.63 | kJ/mol-atom | 0.005 | 3.929 (dft, calibrated) | 3.929 | ||||
| -20.5 | kJ/mol-atom | 0.05 | 3.929 (dft, calibrated) | 3.929 | ||||
| -20.43 | kJ/mol-atom | 0.005 | 3.929 (dft, calibrated) | 3.929 | ||||
| -20.38 | 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-aaackvmr | -19.894 | -0.206183 | R-3m | 0 | 0 | no |
| OQMD | oqmd-30782 | -19.955 | -0.206825 | R-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
- K. Santhy, K.C. Hari Kumar, Thermodynamic reassessment of Nb-Ni-Ti system with order–disorder model, Journal of Alloys and Compounds 619, 733-747 (2015). doi:10.1016/j.jallcom.2014.08.200
- Hui Sun, Shun-Li Shang, Rushi Gong, Brandon J. Bocklund, Allison M. Beese, Zi-Kui Liu, Thermodynamic modeling of the Nb-Ni system with uncertainty quantification using PyCalphad and ESPEI, Calphad 82, 102563 (2023). doi:10.1016/j.calphad.2023.102563