Selected ATcT [1, 2] enthalpy of formation based on version 1.140 of the Thermochemical Network [3]

This version of ATcT results[3] was generated by additional expansion of version 1.130 to fully include the highest-level electronic structure computations described in reference [4].

Trihydrogen

Formula: (H)(HH) (g, vdW)

CAS RN: 12184-91-7

ATcT ID: 12184-91-7*100

SMILES: [H]1[H][H]1

InChI: InChI=1S/H3/c1-2-3-1

InChIKey: FVJJEQURJXHDEY-UHFFFAOYSA-N

SMILES: [H][H][H]

InChI: InChI=1S/H3/h1H2

InChIKey: ZBZUJTMZUGLJFB-UHFFFAOYSA-N

Hills Formula: H3

2D Image:

Aliases: H3; Trihydrogen; Trihydrogen radical; Triatomic hydrogen; Triatomic hydrogen radical; Hyzone

Relative Molecular Mass: 3.02382 ± 0.00021

Δ_fH°(0 K)	Δ_fH°(298.15 K)	Uncertainty	Units
215.9	218.3	± 1.1	kJ/mol

3D Image of (H)(HH) (g, vdW)

spin ON spin OFF

Top contributors to the provenance of Δ_fH° of (H)(HH) (g, vdW)

The 14 contributors listed below account for 90.0% of the provenance of Δ_fH° of (H)(HH) (g, vdW).

Please note: The list is limited to 20 most important contributors or, if less, a number sufficient to account for 90% of the provenance. The Reference acts as a further link to the relevant references and notes for the measurement. The Measured Quantity is normaly given in the original units; in cases where we have reinterpreted the original measurement, the listed value may differ from that given by the authors. The quoted uncertainty is the a priori uncertainty used as input when constructing the initial Thermochemical Network, and corresponds either to the value proposed by the original authors or to our estimate; if an additional multiplier is given in parentheses immediately after the prior uncertainty, it corresponds to the factor by which the prior uncertainty needed to be multiplied during the ATcT analysis in order to make that particular measurement consistent with the prevailing knowledge contained in the Thermochemical Network.

Contribution (%)	TN ID	Reaction	Measured Quantity	Reference
20.2	87.7	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -55 ± 200 cm-1	Pavanello 2009b, Cafiero 2001, Ruscic anh, est unc
20.2	88.1	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 74759 ± 200 cm-1	Pavanello 2009b, Matyus 2007, est unc
8.9	87.9	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -52 ± 300 cm-1	Mielke 2002, est unc
8.9	87.8	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -55 ± 300 cm-1	Partridge 1993, est unc
7.7	88.6	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.261 ± 0.040 eV	Ruscic W1RO
2.9	87.6	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.15 ± 1.5 kcal/mol	Truhlar 1978, Siegbahn 1978, Liu 1973, est unc
2.9	87.5	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.24 ± 1.50 kcal/mol	Ruscic W1RO
2.9	86.5	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 103.10 ± 1.50 kcal/mol	Ruscic W1RO
2.5	87.4	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.03 ± 1.60 kcal/mol	Ruscic CBS-n
2.5	87.2	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = 0.03 ± 1.60 kcal/mol	Ruscic G4
2.5	86.2	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 103.68 ± 1.60 kcal/mol	Ruscic G4
2.5	86.4	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 103.76 ± 1.60 kcal/mol	Ruscic CBS-n
2.3	88.3	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.327 ± 0.073 eV	Ruscic G4
2.2	87.1	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = 0.49 ± 1.72 kcal/mol	Ruscic G3X

Most Influential reactions involving (H)(HH) (g, vdW)

Please note: The list, which is based on a hat (projection) matrix analysis, is limited to no more than 20 largest influences.

Influence Coefficient	TN ID	Reaction	Measured Quantity	Reference
0.202	88.1	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 74759 ± 200 cm-1	Pavanello 2009b, Matyus 2007, est unc
0.202	87.7	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -55 ± 200 cm-1	Pavanello 2009b, Cafiero 2001, Ruscic anh, est unc
0.090	87.8	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -55 ± 300 cm-1	Partridge 1993, est unc
0.090	87.9	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -52 ± 300 cm-1	Mielke 2002, est unc
0.077	88.6	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.261 ± 0.040 eV	Ruscic W1RO
0.029	86.5	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 103.10 ± 1.50 kcal/mol	Ruscic W1RO
0.029	87.6	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.15 ± 1.5 kcal/mol	Truhlar 1978, Siegbahn 1978, Liu 1973, est unc
0.029	87.5	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.24 ± 1.50 kcal/mol	Ruscic W1RO
0.025	86.4	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 103.76 ± 1.60 kcal/mol	Ruscic CBS-n
0.025	86.2	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 103.68 ± 1.60 kcal/mol	Ruscic G4
0.025	87.2	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = 0.03 ± 1.60 kcal/mol	Ruscic G4
0.025	87.4	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.03 ± 1.60 kcal/mol	Ruscic CBS-n
0.023	88.3	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.327 ± 0.073 eV	Ruscic G4
0.022	86.1	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 104.20 ± 1.72 kcal/mol	Ruscic G3X
0.022	87.1	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = 0.49 ± 1.72 kcal/mol	Ruscic G3X
0.022	88.5	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.270 ± 0.075 eV	Ruscic CBS-n
0.014	88.2	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.342 ± 0.093 eV	Ruscic G3X
0.014	86.3	(H)(HH) (g, vdW) → 3 H (g)	Δ_rH°(0 K) = 104.15 ± 2.16 kcal/mol	Ruscic CBS-n
0.014	87.3	(H)(HH) (g, vdW) → H2 (g) + H (g)	Δ_rH°(0 K) = -0.29 ± 2.16 kcal/mol	Ruscic CBS-n
0.012	88.4	(H)(HH) (g, vdW) → [H3]+ (g)	Δ_rH°(0 K) = 9.291 ± 0.099 eV	Ruscic CBS-n

References

1 B. Ruscic, R. E. Pinzon, M. L. Morton, G. von Laszewski, S. Bittner, S. G. Nijsure, K. A. Amin, M. Minkoff, and A. F. Wagner,
Introduction to Active Thermochemical Tables: Several "Key" Enthalpies of Formation Revisited.
J. Phys. Chem. A 108, 9979-9997 (2004) [DOI: 10.1021/jp047912y]

2 B. Ruscic, R. E. Pinzon, G. von Laszewski, D. Kodeboyina, A. Burcat, D. Leahy, D. Montoya, and A. F. Wagner,
Active Thermochemical Tables: Thermochemistry for the 21^st Century.
J. Phys. Conf. Ser. 16, 561-570 (2005) [DOI: 10.1088/1742-6596/16/1/078]

3 B. Ruscic and D. H. Bross,
Active Thermochemical Tables (ATcT) values based on ver. 1.140 of the Thermochemical Network (2024); available at ATcT.anl.gov

4 J. H. Thorpe, J. L. Kilburn, D. Feller, P. B. Changala, D. H. Bross, B. Ruscic, and J. F. Stanton,
Elaborated Thermochemical Treatment of HF, CO, N2, and H2O: Insight into HEAT and Its Extensions
J. Chem. Phys. 155, 184109 (2021) [DOI: 10.1063/5.0069322]

5 B. Ruscic,
Uncertainty Quantification in Thermochemistry, Benchmarking Electronic Structure Computations, and Active Thermochemical Tables.
Int. J. Quantum Chem. 114, 1097-1101 (2014) [DOI: 10.1002/qua.24605]

6 B. Ruscic and D. H. Bross,
Thermochemistry
Computer Aided Chem. Eng. 45, 3-114 (2019) [DOI: 10.1016/B978-0-444-64087-1.00001-2]

Formula The aggregate state is given in parentheses following the formula, such as: g - gas-phase, cr - crystal, l - liquid, etc.
Uncertainties The listed uncertainties correspond to estimated 95% confidence limits, as customary in thermochemistry (see, for example, Ruscic [5] and Ruscic and Bross[6]).
Note that an uncertainty of ± 0.000 kJ/mol indicates that the estimated uncertainty is < ± 0.000₅ kJ/mol.
Website Functionality Credits The reorganization of the website was developed and implemented by David H. Bross (ANL).
The find function is based on the complete Species Dictionary entries for the appropriate version of the ATcT TN.
The molecule images are rendered by Indigo-depict.
The XYZ renderings are based on Jmol: an open-source Java viewer for chemical structures in 3D. http://www.jmol.org/.
Acknowledgement This work was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences and Biosciences under Contract No. DE-AC02-06CH11357.