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
BromideBr- (g)[Br-]-206.620-212.683± 0.056kJ/mol79.90455 ±
0.00100
24959-67-9*0

Representative Geometry of Br- (g)

spin ON           spin OFF
          

Top contributors to the provenance of ΔfH° of Br- (g)

The 1 contributors listed below account for 95.7% of the provenance of ΔfH° of Br- (g).

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
95.7752.2 Br2 (cr,l) → Br2 (g) ΔrH°(298.15 K) = 7.386 ± 0.027 kcal/molHildenbrand 1958

Top 10 species with enthalpies of formation correlated to the ΔfH° of Br- (g)

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
100.0 Bromine atomBr (g)[Br]117.917111.854± 0.056kJ/mol79.90400 ±
0.00100
10097-32-2*0
100.0 Bromine atomBr (g, 2P3/2)[Br]117.917111.854± 0.056kJ/mol79.90400 ±
0.00100
10097-32-2*1
100.0 Bromine atomBr (g, 2P1/2)[Br]162.001155.938± 0.056kJ/mol79.90400 ±
0.00100
10097-32-2*2
100.0 DibromineBr2 (g)BrBr45.6830.89± 0.11kJ/mol159.8080 ±
0.0020
7726-95-6*0
99.4 BromoniumBr+ (g)[Br+]1257.7771251.714± 0.056kJ/mol79.90345 ±
0.00100
22541-56-6*0
93.6 Bromine monochlorideBrCl (g)BrCl21.88014.437± 0.060kJ/mol115.3567 ±
0.0013
13863-41-7*0
83.5 Iodine monobromideIBr (g)IBr49.71740.770± 0.067kJ/mol206.8085 ±
0.0010
7789-33-5*0
49.2 Diatomic bromine cation[Br2]+ (g)Br[Br+]1060.331045.38± 0.23kJ/mol159.8075 ±
0.0020
12595-71-0*0
29.9 DibromophosgeneCOBr2 (g)C(Br)(Br)=O-97.98-113.91± 0.37kJ/mol187.8181 ±
0.0022
593-95-3*0
27.6 Hydrogen bromideHBr (g)Br-27.81-35.66± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*0

Most Influential reactions involving Br- (g)

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
1.000762.1 Br- (g) → Br (g) ΔrH°(0 K) = 27129.170 ± 0.015 cm-1Blondel 1989
0.4511439.2 [NO3]- (g) HBr (g) → Br- (g) HNO3 (g) ΔrH°(391 K) = -1.03 ± 0.21 kcal/molDavidson 1977, 2nd Law
0.444768.1 Br- (g) Br2 (g) → [Br2]- (g) Br (g) ΔrH°(0 K) = 0.84 ± 0.03 eVChupka 1971b
0.1661439.1 [NO3]- (g) HBr (g) → Br- (g) HNO3 (g) ΔrH°(0 K) = -0.045 ± 0.015 eVFerguson 1972b
0.159769.1 Br- (g) Cl2 (g) → [Cl2]- (g) Br (g) ΔrH°(0 K) = 1.01 ± 0.03 (×1.164) eVChupka 1971b
0.104823.1 [BrO]- (g) → Br- (g) O (g) ΔrH°(0 K) = 32.46 ± 0.4 kcal/molPeterson 2006
0.0941439.3 [NO3]- (g) HBr (g) → Br- (g) HNO3 (g) ΔrG°(391 K) = 0.76 ± 0.45 (×1.022) kcal/molDavidson 1977, 3rd Law
0.058926.4 HOI (g) Br- (g) → HOBr (g) I- (g) ΔrH°(0 K) = 5.81 ± 2 kcal/molRen 2002, est unc
0.040760.1 [Br2]- (g) → Br (g) Br- (g) ΔrH°(0 K) = 1.15 ± 0.10 eVBaede 1973
0.030915.1 [IO]- (g) Br- (g) → [BrO]- (g) I- (g) ΔrH°(0 K) = 32.0 ± 6 (×1.189) kJ/molHassanzadeh 1997, est unc
0.029767.1 Br- (g) F2 (g) → [F2]- (g) Br (g) ΔrH°(0 K) = 0.27 ± 0.03 (×2.709) eVChupka 1971b
0.024926.2 HOI (g) Br- (g) → HOBr (g) I- (g) ΔrH°(0 K) = 4.48 ± 3.1 kcal/molRuscic unpub
0.024926.3 HOI (g) Br- (g) → HOBr (g) I- (g) ΔrH°(0 K) = 4.52 ± 3.1 kcal/molRuscic unpub
0.020926.1 HOI (g) Br- (g) → HOBr (g) I- (g) ΔrH°(0 K) = 4.78 ± 3.4 kcal/molRuscic unpub
0.018928.1 HOI (g) Br- (g) → HOBr (g) I- (g) ΔrH°(0 K) = 22.6 ± 15 kJ/molHassanzadeh 1997, est unc
0.010766.1 [Br2]- (g) → Br- (g) Br (g) ΔrH°(0 K) = 1.08 ± 0.20 eVDispert 1977
0.010768.2 Br- (g) Br2 (g) → [Br2]- (g) Br (g) ΔrH°(0 K) = 0.70 ± 0.20 eVHughes 1973
0.004871.1 Br- (g) I2 (g) → [I2]- (g) Br (g) ΔrH°(0 K) = 0.77 ± 0.03 (×2.327) eVChupka 1971b
0.004850.4 HOBr (g) Cl- (g) → HOCl (g) Br- (g) ΔrH°(0 K) = 1.43 ± 2 kcal/molRen 2002, est unc
0.0043414.2 CH3Br (g) F- (g) → CH3F (g) Br- (g) ΔrH°(0 K) = -39.27 ± 1.1 kcal/molParthiban 2001a, Parthiban 2002, Oren 2004


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.