HfB2: enthalpy of formation
7 accepted literature formation-enthalpy value(s) (experimental 6, model 1); experimental median -105.8 kJ/mol-atom (n = 6); Materials Project -98.211 kJ/mol-atom (mp-aaaaacys); OQMD -98.749 kJ/mol-atom (oqmd-5848).
Systems: B–Hf
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -117.633 kJ/mol-atom | HfB2 | 298.15 | experimental | Langmuir vaporization | B–Hf | [1] Bittermann 1997 cites Krupka 1962 | Table 3, p. 4, row 13 report | |
| -109.633 kJ/mol-atom ± 2.93333 | HfB2 | 298.15 | experimental | Fluorine bomb calorimetry | B–Hf | [1] Bittermann 1997 cites ref. 67Joh | Table 3, p. 4, row 15 report | |
| -106.567 kJ/mol-atom | HfB2 | 298.15 | experimental | Langmuir vaporization | B–Hf | [1] Bittermann 1997 cites ref. 64 | Table 3, p. 4, row 14 report | |
| -105.033 kJ/mol-atom | HfB2 | 298.15 | experimental | Tensimetric (reduction of HfO2 to HfB2 with B and B4C) | B–Hf | [1] Bittermann 1997 cites Paderno 1959 | Table 3, p. 4, row 12 report | |
| -87.3 kJ/mol-atom ± 1.66667 | HfB2 | 298.15 | experimental | Self-sustaining high-temperature synthesis calorimetry | B–Hf | [1] Bittermann 1997 cites Maslov 1978 | Table 3, p. 4, row 17 report | |
| -83.1333 kJ/mol-atom ± 1.96667 | HfB2 | 298.15 | experimental | Self-sustaining high-temperature synthesis calorimetry | B–Hf | [1] Bittermann 1997 cites Kitpichev 1979 | Table 3, p. 4, row 18 report | |
| -106.567 kJ/mol-atom | HfB2 | model | B–Hf | [1] Bittermann 1997 | Table 3, p. 4, row 20 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 |
|---|---|---|---|---|---|---|---|---|
| -117.633 | kJ/mol-atom | 0.01667 | 4.2 (kems_vapour, calibrated) | 4.2 | ||||
| -109.633 | kJ/mol-atom | 2.933 | 0.01667 | 1 (combustion_calorimetry, cleaned_below_threshold) | 2.933 | |||
| -106.567 | kJ/mol-atom | 0.01667 | 4.2 (kems_vapour, calibrated) | 4.2 | ||||
| -105.033 | kJ/mol-atom | 0.01667 | 4.1 (experimental_unspecified, cleaned_below_threshold) | 4.1 | ||||
| -87.3 | kJ/mol-atom | 1.667 | 0.01667 | 3.2 (solution_reaction_calorimetry, calibrated) | 3.2 | |||
| -83.1333 | kJ/mol-atom | 1.967 | 0.01667 | 3.2 (solution_reaction_calorimetry, calibrated) | 3.2 | |||
| -106.567 | kJ/mol-atom | 0.01667 | 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 |
|---|---|---|---|---|---|---|---|
| Materials Project | mp-aaaaacys | -98.211 | -1.01789 | P6/mmm | 0 | 0 | no |
| OQMD | oqmd-5848 | -98.749 | -1.02347 | P6/mmm | 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
- H. Bittermann, P. Rogl, Critical assessment and thermodynamic calculation of the ternary system boron-hafnium-titanium (B-Hf-Ti), JPE 18, 24-47 (1997). doi:10.1007/bf02646757