Al2Te3: enthalpy of formation
7 accepted literature formation-enthalpy value(s) (experimental 5, model 2); experimental median -63.6 kJ/mol-atom (n = 5); Materials Project -67.973 kJ/mol-atom (mp-aaaabrqs); OQMD -43.474 kJ/mol-atom (oqmd-648344).
Systems: Al–Te
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -63.8 kJ/mol-atom | Al2Te3 | 298.15 | experimental | Al–Te | [1] Shi 2019 cites Joel 1967 | p. 9 report | However, the enthalpy of formation of bAl2Te3 at 25 C obtained in this work (-85.9 kJ/mol-atoms) is less negative than experimental results (-63.8 kJ/mol-atoms[46] and [47] -52.0 kJ/mol-atoms ). | |
| -63.8 kJ/mol-atom | βAl2Te3 | 298.15 | experimental | Direct synthesis calorimetry | Al–Te | [1] Shi 2019 cites Joel 1967 | Table 3, p. 3, row 15 report | |
| -63.6 kJ/mol-atom | βAl2Te3 | 298.15 | experimental | Evaluation | Al–Te | [1] Shi 2019 cites Mills 1974 | Table 3, p. 3, row 17 report | |
| -52 kJ/mol-atom | βAl2Te3 | 298.15 | experimental | Torsion-effusion method for temperature | Al–Te | [1] Shi 2019 cites Balducci 1997 | Table 3, p. 3, row 16 report | |
| -52 kJ/mol-atom | Al2Te3 | 298.15 | experimental | Al–Te | [1] Shi 2019 cites Balducci 1997 | p. 9 report | However, the enthalpy of formation of bAl2Te3 at 25 C obtained in this work (-85.9 kJ/mol-atoms) is less negative than experimental results (-63.8 kJ/mol-atoms[46] and [47] -52.0 kJ/mol-atoms ). | |
| -85.9 kJ/mol-atom | Al2Te3 | 298.15 | model | Al–Te | [1] Shi 2019 | p. 9 report | However, the enthalpy of formation of bAl2Te3 at 25 C obtained in this work (-85.9 kJ/mol-atoms) is less negative than experimental results (-63.8 kJ/mol-atoms[46] and [47] -52.0 kJ/mol-atoms ). | |
| -85.9 kJ/mol-atom | βAl2Te3 | 298.15 | model | CALPHAD | Al–Te | [1] Shi 2019 | Table 3, p. 3, row 18 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 |
|---|---|---|---|---|---|---|---|---|
| -63.8 | kJ/mol-atom | 0.05 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -63.8 | kJ/mol-atom | 0.05 | 3.2 (solution_reaction_calorimetry, calibrated) | 3.2 | ||||
| -63.6 | kJ/mol-atom | 0.05 | 3.5 (evaluated_compilation, calibrated) | 3.5 | ||||
| -52 | kJ/mol-atom | 0.05 | 4.2 (kems_vapour, calibrated) | 4.2 | ||||
| -52 | kJ/mol-atom | 0.05 | 3.5 (unknown, calibrated) | 3.5 | ||||
| -85.9 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -85.9 | kJ/mol-atom | 0.05 | 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-aaaabrqs | -67.973 | -0.704498 | P2_1/c | 0 | 0 | no |
| OQMD | oqmd-648344 | -43.474 | -0.450581 | P21/c | 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
- Chenying Shi, Biaobiao Yang, Biao Hu, Yong Du, Sheng Yao, Thermodynamic Description of the Al–X (X = S, Se, Te) Systems, J. Phase Equilib. Diffus. 40, 392-402 (2019). doi:10.1007/s11669-019-00733-z