Selected ATcT [1, 2] enthalpy of formation based on version 1.122b of the Thermochemical Network [3]

This version of ATcT results was generated from an expansion of version 1.122 [4][5] to include the best possible isomerization of HCN and HNC [6].

Species Name Formula Image    ΔfH°(0 K)    ΔfH°(298.15 K) Uncertainty Units Relative
Molecular
Mass
ATcT ID
Tribromide ion[Br3]- (aq)Br[Br-]Br-129.38± 0.26kJ/mol239.7125 ±
0.0030
14522-80-6*800

Top contributors to the provenance of ΔfH° of [Br3]- (aq)

The 20 contributors listed below account only for 85.6% of the provenance of ΔfH° of [Br3]- (aq).
A total of 40 contributors would be needed to account for 90% of the provenance.

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
61.0799.1 Br2 (cr,l) → Br2 (aq) ΔrH°(298.15 K) = -2.17 ± 0.20 kJ/molVasilev 1973, as quoted by CODATA Key Vals
3.0800.1 Cl2 (g) + 2 Br- (aq) → Br2 (cr,l) + 2 Cl- (aq) ΔrH°(298.15 K) = -91.29 ± 0.40 (×2.768) kJ/molJohnson 1963, as quoted by CODATA Key Vals
3.0800.2 Cl2 (g) + 2 Br- (aq) → Br2 (cr,l) + 2 Cl- (aq) ΔrH°(298.15 K) = -91.29 ± 0.80 (×1.384) kJ/molSunner 1964, as quoted by CODATA Key Vals
2.5752.2 Br2 (cr,l) → Br2 (g) ΔrH°(298.15 K) = 7.386 ± 0.027 kcal/molHildenbrand 1958
2.3803.1 [HBr]+ (g) → H (g) Br+ (g) ΔrH°(0 K) = 31394.5 ± 20 (×2.229) cm-1Haugh 1971, Norling 1935
1.7784.1 HBr (g) → HBr (aq, 2570 H2O) ΔrH°(298.15 K) = -20.286 ± 0.012 kcal/molVanderzee 1963
1.4780.1 1/2 H2 (g) + 1/2 Br2 (cr,l) → HBr (aq) ΔrG°(298.15 K) = -102.81 ± 0.80 kJ/molJones 1934, as quoted by CODATA Key Vals
1.0778.1 1/2 H2 (g) + 1/2 Br2 (g) → HBr (g) ΔrH°(376.15 K) = -12.470 ± 0.170 (×1.139) kcal/molLacher 1956a, Lacher 1956
0.9801.1 Br2 (aq) Br- (aq) → [Br3]- (aq) ΔrG°(298.15 K) = -7.150 ± 0.025 kJ/molMussini 1966, as quoted by CODATA Key Vals
0.9771.12 HBr (g) → H (g) Br (g) ΔrH°(0 K) = 86.47 ± 0.2 kcal/molFeller 2008
0.9772.6 HBr (g) Cl (g) → HCl (g) Br (g) ΔrH°(0 K) = -15.68 ± 0.2 kcal/molFeller 2008
0.9887.1 HI (g) Br (g) → HBr (g) I (g) ΔrH°(0 K) = -16.14 ± 0.2 kcal/molFeller 2008
0.9800.3 Cl2 (g) + 2 Br- (aq) → Br2 (cr,l) + 2 Cl- (aq) ΔrH°(298.15 K) = -91.55 ± 2.00 kJ/molThomsen 1882, as quoted by CODATA Key Vals
0.8891.1 Br2 (cr,l) + 3 I- (aq) → [I3]- (aq) + 2 Br- (aq) ΔrH°(298.15 K) = -29.355 ± 0.364 kcal/molWu 1963
0.73739.2 CH3CH2Br (g) → [CH3CH2]+ (g) Br (g) ΔrH°(0 K) = 11.130 ± 0.005 eVBaer 2000
0.7803.3 [HBr]+ (g) → H (g) Br+ (g) ΔrH°(0 K) = 31358 ± 15 (×5.187) cm-1Penno 1998, Norling 1935, est unc
0.71666.1 CH4 (g) Br (g) → CH3 (g) HBr (g) ΔrH°(0 K) = 5929 ± 80 cm-1Czako 2013
0.52212.2 HCO (g) HBr (g) → H2CO (g) Br (g) ΔrG°(385 K) = 6.79 ± 0.64 (×1.756) kJ/molBecerra 1997, Nava 1981, 3rd Law, note unc
0.43872.1 COBr2 (l) H2O (cr,l) → CO2 (g) + 2 HBr (aq, 5000 H2O) ΔrH°(298.15 K) = -49.06 ± 0.32 kcal/molAnthoney 1970, as quoted by Pedley 1986
0.43407.3 CH3Br (g) HBr (g) → Br2 (g) CH4 (g) ΔrG°(712.2 K) = 35.8 ± 1.6 (×1.242) kJ/molFerguson 1973, 3rd Law

Top 10 species with enthalpies of formation correlated to the ΔfH° of [Br3]- (aq)

Please note: The correlation coefficients are obtained by renormalizing the off-diagonal elements of the covariance matrix by the corresponding variances.
The correlation coefficient is a number from -1 to 1, with 1 representing perfectly correlated species, -1 representing perfectly anti-correlated species, and 0 representing perfectly uncorrelated species.


Correlation
Coefficent
(%)
Species Name Formula Image    ΔfH°(0 K)    ΔfH°(298.15 K) Uncertainty Units Relative
Molecular
Mass
ATcT ID
78.1 DibromineBr2 (aq)BrBr-2.16± 0.20kJ/mol159.8080 ±
0.0020
7726-95-6*800
61.7 BromideBr- (aq)[Br-]-120.80± 0.16kJ/mol79.90455 ±
0.00100
24959-67-9*800
61.7 Hydrogen bromideHBr (aq)Br-120.80± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*800
61.6 Hydrogen bromideHBr (aq, 3000 H2O)Br-120.56± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*842
61.6 Hydrogen bromideHBr (aq, 2570 H2O)Br-120.54± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*952
61.6 Hydrogen bromideHBr (aq, 2000 H2O)Br-120.51± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*841
61.6 Hydrogen bromideHBr (aq, 1000 H2O)Br-120.41± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*839
61.5 Hydrogen bromideHBr (aq, 5000 H2O)Br-120.61± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*844
61.5 Hydrogen bromideHBr (aq, 600 H2O)Br-120.32± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*834
58.6 Hydrogen bromideHBr (g)Br-27.81-35.66± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*0

Most Influential reactions involving [Br3]- (aq)

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
0.999801.1 Br2 (aq) Br- (aq) → [Br3]- (aq) ΔrG°(298.15 K) = -7.150 ± 0.025 kJ/molMussini 1966, as quoted by CODATA Key Vals
0.000801.2 Br2 (aq) Br- (aq) → [Br3]- (aq) ΔrH°(298.15 K) = -7.53 ± 0.30 (×3.748) kJ/molVasilev 1973, as quoted by CODATA Key Vals


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 21st 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. 1.122b of the Thermochemical Network (2016); available at ATcT.anl.gov
4   B. Ruscic,
Active Thermochemical Tables: Sequential Bond Dissociation Enthalpies of Methane, Ethane, and Methanol and the Related Thermochemistry.
J. Phys. Chem. A 119, 7810-7837 (2015) [DOI: 10.1021/acs.jpca.5b01346]
5   S. J. Klippenstein, L. B. Harding, and B. Ruscic,
Ab initio Computations and Active Thermochemical Tables Hand in Hand: Heats of Formation of Core Combustion Species.
J. Phys. Chem. A 121, 6580-6602 (2017) [DOI: 10.1021/acs.jpca.7b05945]
6   T. L. Nguyen, J. H. Baraban, B. Ruscic, and J. F. Stanton,
On the HCN – HNC Energy Difference.
J. Phys. Chem. A 119, 10929-10934 (2015) [DOI: 10.1021/acs.jpca.5b08406]
7   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]

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 [7]).
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.