NiYb: enthalpy of formation
7 accepted literature formation-enthalpy value(s) (experimental 3, model 4); experimental median -23.4 kJ/mol-atom (n = 2); OQMD -27.289 kJ/mol-atom (oqmd-30880).
Systems: Ni–Yb
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -28 unspecified ± 2 | α-YbNi | 298.15 | experimental | DSC | Ni–Yb | [1] Hu 2017 cites Brutti 2002 doi | p. 17 report | Based on Eq. 16, the enthalpy of formation of the α-YbNi phase at 298K is calculated to be -27.2 kJ/mol-atom, a value which agrees well with the recent experimental results from DSC measurements (-28±2.0 kJ/molatom) by Brutti et al. [13]. |
| -28 kJ/mol-atom ± 2 | NiYb_LT | 298.15 | experimental | Synthèse directe Calo. | Ni–Yb | [2] Kardellass 2016 cites Brutti 2002 doi | Table 2, p. 5, row 21 report | |
| -18.8 kJ/mol-atom | NiYb_LT | 298.15 | experimental | Calorimetry | Ni–Yb | [2] Kardellass 2016 cites Berezutskii 2014 doi | Table 2, p. 5, row 23 report | |
| -27.8 kJ/mol-atom | NiYb_LT | 298.15 | model | Prediction | Ni–Yb | [2] Kardellass 2016 cites De 1988 | Table 2, p. 5, row 20 report | |
| -27.2 kJ/mol-atom | α-YbNi | 298.15 | model | Ni–Yb | [1] Hu 2017 | p. 17 report | Based on Eq. 16, the enthalpy of formation of the α-YbNi phase at 298K is calculated to be -27.2 kJ/mol-atom, a value which agrees well with the recent experimental results from DSC measurements (-28±2.0 kJ/molatom) by Brutti et al. [13]. | |
| -17.28 kJ/mol-atom | NiYb | 298.15 | model | Optimization | Ni–Yb | [2] Kardellass 2016 | Table 4, p. 7, row 12 report | |
| -17.28 kJ/mol-atom | NiYb_LT | 298.15 | model | Optimization | Ni–Yb | [2] Kardellass 2016 | Table 2, p. 5, row 22 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 |
|---|---|---|---|---|---|---|---|---|
| -28 | unspecified | 2 | 0.05 | unit 'unspecified' not convertible to kJ/mol-atom | 2 | |||
| -28 | kJ/mol-atom | 2 | 0.05 | 3.2 (solution_reaction_calorimetry, calibrated) | 3.2 | |||
| -18.8 | kJ/mol-atom | 0.05 | 3.2 (solution_reaction_calorimetry, calibrated) | 3.2 | ||||
| -27.8 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -27.2 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -17.28 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -17.28 | kJ/mol-atom | 0.005 | 3.9 (model_calculated, calibrated) | 3.9 |
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 |
|---|---|---|---|---|---|---|---|
| OQMD | oqmd-30880 | -27.289 | -0.282833 | Pnma | 3.8304 | 0.0397 | 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
- Yong-Jie Hu, Yi Wang, Samad A. Firdosy, Kurt E. Star, Jean-Pierre Fleurial, Vilupanur A. Ravi et al., First-principles calculations and thermodynamic modeling of the Yb-Ni binary system, Calphad 59, 207-217 (2017). doi:10.1016/j.calphad.2017.09.004
- Saïd Kardellass, Colette Servant, Najim Selhaoui, Thermodynamic description of the Ni–Yb and Ni–Eu binary systems, J Therm Anal Calorim 125, 255-269 (2016). doi:10.1007/s10973-016-5380-3