Mo2N: enthalpy of formation
20 accepted literature formation-enthalpy value(s) (model 12, unspecified 8); Materials Project -34.8 kJ/mol-atom (mp-aaaabpjd); OQMD -32.521 kJ/mol-atom (oqmd-2032475).
Systems: Mo–N
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -35.989 kJ/mol-atom | Mo2N-beta | model | Mo–N | [1] Daclan 2023 cites JARVIS 2020 | Table 2, p. 6, row 3 report | |||
| -35.989 kJ/mol-atom | Mo2N-beta | 0 | model | Mo–N | [1] Daclan 2023 cites JARVIS 2020 | Table 2, p. 6, row 3 report | ||
| -35.989 kJ/mol-atom | Mo2N-beta | model | Mo–N | [1] Daclan 2023 cites JARVIS 2020 | Table 2, p. 6, row 3 report | |||
| -35.989 kJ/mol-atom | Mo2N-beta | 0 | model | Mo–N | [1] Daclan 2023 cites JARVIS 2020 | Table 2, p. 6, row 3 report | ||
| -25.953 kJ/mol-atom | Mo2N-beta | 0 | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 2 report | ||
| -25.953 kJ/mol-atom | Mo2N-beta | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 2 report | |||
| -25.9526 kJ/mol-atom | Mo2N-beta | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 2 report | |||
| -25.9526 kJ/mol-atom | Mo2N-beta | 0 | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 2 report | ||
| -22.0797 kJ/mol-atom | Mo2N-gamma | 0 | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 5 report | ||
| -22.0797 kJ/mol-atom | Mo2N-gamma | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 5 report | |||
| -22.079 kJ/mol-atom | Mo2N-gamma | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 5 report | |||
| -22.079 kJ/mol-atom | Mo2N-gamma | 0 | model | Mo–N | [1] Daclan 2023 cites Klimashin 2016 doi | Table 2, p. 6, row 5 report | ||
| -26.0974 kJ/mol-atom | Mo2N-beta | 0 | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 1 report | ||
| -26.0974 kJ/mol-atom | Mo2N-beta | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 1 report | |||
| -26.097 kJ/mol-atom | Mo2N-beta | 0 | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 1 report | ||
| -26.097 kJ/mol-atom | Mo2N-beta | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 1 report | |||
| -21.1081 kJ/mol-atom | Mo2N-gamma | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 4 report | |||
| -21.1081 kJ/mol-atom | Mo2N-gamma | 0 | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 4 report | ||
| -21.108 kJ/mol-atom | Mo2N-gamma | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 4 report | |||
| -21.108 kJ/mol-atom | Mo2N-gamma | 0 | unspecified | Mo–N | [1] Daclan 2023 | Table 2, p. 6, row 4 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 |
|---|---|---|---|---|---|---|---|---|
| -35.989 | kJ/mol-atom | 0.04824 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -35.989 | kJ/mol-atom | 0.04824 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -35.989 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -35.989 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -25.953 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -25.953 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -25.9526 | kJ/mol-atom | 4.824e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -25.9526 | kJ/mol-atom | 4.824e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -22.0797 | kJ/mol-atom | 4.824e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -22.0797 | kJ/mol-atom | 4.824e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -22.079 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -22.079 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -26.0974 | kJ/mol-atom | 4.824e-4 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -26.0974 | kJ/mol-atom | 4.824e-4 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -26.097 | kJ/mol-atom | 5.000e-5 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -26.097 | kJ/mol-atom | 5.000e-4 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -21.1081 | kJ/mol-atom | 4.824e-4 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -21.1081 | kJ/mol-atom | 4.824e-4 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -21.108 | kJ/mol-atom | 5.000e-4 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -21.108 | kJ/mol-atom | 5.000e-5 | 3.5 (unknown, calibrated) | 3.5 |
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-aaaabpjd | -34.8 | -0.360678 | I4_1/amd | 0.3921 | 0.0041 | no |
| OQMD | oqmd-2032475 | -32.521 | -0.337055 | Pmmn | 0.5753 | 0.006 | 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
- R.A. Daclan, M.G. Mena, M.R. Vasquez, W. Gierlotka, Ab-initio combined the Calphad approach to the phase equilibria in the ternary Ti-Mo-N system, J min metall B Metall 59, 125-136 (2023). doi:10.2298/jmmb210330011d