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].
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Species Name |
Formula |
Image |
ΔfH°(0 K) |
ΔfH°(298.15 K) |
Uncertainty |
Units |
Relative Molecular Mass |
ATcT ID |
Ethyl bromide | CH3CH2Br (l) | | -55.54 | -91.07 | ± 0.27 | kJ/mol | 108.9651 ± 0.0019 | 74-96-4*500 |
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Top contributors to the provenance of ΔfH° of CH3CH2Br (l)The 20 contributors listed below account only for 66.4% of the provenance of ΔfH° of CH3CH2Br (l). A total of 240 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.
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Contribution (%) | TN ID | Reaction | Measured Quantity | Reference | 34.6 | 3738.1 | C2H4 (g) + HBr (g) → CH3CH2Br (g)  | ΔrG°(546 K) = -8.340 ± 0.203 kJ/mol | Lane 1953, 3rd Law | 5.0 | 3739.2 | CH3CH2Br (g) → [CH3CH2]+ (g) + Br (g)  | ΔrH°(0 K) = 11.130 ± 0.005 eV | Baer 2000 | 4.0 | 3740.9 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrG°(298.236 K) = 1.263 ± 0.109 kJ/mol | ThermoData 2004, 3rd Law | 2.5 | 752.2 | Br2 (cr,l) → Br2 (g)  | ΔrH°(298.15 K) = 7.386 ± 0.027 kcal/mol | Hildenbrand 1958 | 1.9 | 1779.1 | C2H4 (g) + 3 O2 (g) → 2 CO2 (g) + 2 H2O (cr,l)  | ΔrH°(298.15 K) = -1411.18 ± 0.30 kJ/mol | Rossini 1937 | 1.9 | 3739.1 | CH3CH2Br (g) → [CH3CH2]+ (g) + Br (g)  | ΔrH°(0 K) = 11.133 ± 0.008 eV | Borkar 2010 | 1.7 | 800.1 | Cl2 (g) + 2 Br- (aq) → Br2 (cr,l) + 2 Cl- (aq)  | ΔrH°(298.15 K) = -91.29 ± 0.40 (×2.768) kJ/mol | Johnson 1963, as quoted by CODATA Key Vals | 1.7 | 800.2 | Cl2 (g) + 2 Br- (aq) → Br2 (cr,l) + 2 Cl- (aq)  | ΔrH°(298.15 K) = -91.29 ± 0.80 (×1.384) kJ/mol | Sunner 1964, as quoted by CODATA Key Vals | 1.5 | 803.1 | [HBr]+ (g) → H (g) + Br+ (g)  | ΔrH°(0 K) = 31394.5 ± 20 (×2.229) cm-1 | Haugh 1971, Norling 1935 | 1.2 | 1722.1 | C2H6 (g) + 7/2 O2 (g) → 2 CO2 (g) + 3 H2O (cr,l)  | ΔrH°(298.15 K) = -1560.68 ± 0.25 kJ/mol | Pittam 1972 | 1.2 | 3740.5 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(311.9 K) = 27.29 ± 0.20 kJ/mol | Svoboda 1977, Majer 1985, est unc | 1.2 | 3740.4 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(304.6 K) = 27.77 ± 0.20 kJ/mol | Svoboda 1977, Majer 1985, est unc | 1.1 | 117.2 | 1/2 O2 (g) + H2 (g) → H2O (cr,l)  | ΔrH°(298.15 K) = -285.8261 ± 0.040 kJ/mol | Rossini 1939, Rossini 1931, Rossini 1931b, note H2Oa, Rossini 1930 | 1.0 | 3740.7 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(305.99 K) = 6.632 ± 0.05 kcal/mol | de Kolossowsky 1934, ThermoData 2004, est unc | 1.0 | 1741.1 | CH3CH2 (g) → [CH3CH2]+ (g)  | ΔrH°(0 K) = 8.117 ± 0.008 (×1.215) eV | Ruscic 1989b | 1.0 | 1741.14 | CH3CH2 (g) → [CH3CH2]+ (g)  | ΔrH°(0 K) = 8.124 ± 0.010 eV | Lau 2005 | 0.8 | 780.1 | 1/2 H2 (g) + 1/2 Br2 (cr,l) → HBr (aq)  | ΔrG°(298.15 K) = -102.81 ± 0.80 kJ/mol | Jones 1934, as quoted by CODATA Key Vals | 0.7 | 1759.1 | [CH3CH2]+ (g) + H2O (g) → [H3O]+ (g) + C2H4 (g)  | ΔrG°(298.15 K) = -1.8 ± 0.2 kcal/mol | Bohme 1981, 3rd Law | 0.6 | 778.1 | 1/2 H2 (g) + 1/2 Br2 (g) → HBr (g)  | ΔrH°(376.15 K) = -12.470 ± 0.170 (×1.139) kcal/mol | Lacher 1956a, Lacher 1956 | 0.6 | 771.12 | HBr (g) → H (g) + Br (g)  | ΔrH°(0 K) = 86.47 ± 0.2 kcal/mol | Feller 2008 |
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Top 10 species with enthalpies of formation correlated to the ΔfH° of CH3CH2Br (l) |
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.
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Correlation Coefficent (%) | Species Name | Formula | Image | ΔfH°(0 K) | ΔfH°(298.15 K) | Uncertainty | Units | Relative Molecular Mass | ATcT ID | 95.8 | Ethyl bromide | CH3CH2Br (g) | | -41.14 | -63.09 | ± 0.26 | kJ/mol | 108.9651 ± 0.0019 | 74-96-4*0 | 49.2 | Hydrogen bromide | HBr (g) | | -27.81 | -35.66 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*0 | 49.2 | Bromoniumyl | [HBr]+ (g) | | 1097.86 | 1090.01 | ± 0.16 | kJ/mol | 80.9114 ± 0.0010 | 12258-64-9*0 | 46.9 | Hydrogen bromide | HBr (aq, 2570 H2O) | | | -120.54 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*952 | 46.8 | Hydrogen bromide | HBr (aq, 3000 H2O) | | | -120.56 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*842 | 46.8 | Hydrogen bromide | HBr (aq, 2000 H2O) | | | -120.51 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*841 | 46.8 | Hydrogen bromide | HBr (aq) | | | -120.80 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*800 | 46.8 | Bromide | Br- (aq) | | | -120.80 | ± 0.16 | kJ/mol | 79.90455 ± 0.00100 | 24959-67-9*800 | 46.8 | Hydrogen bromide | HBr (aq, 1000 H2O) | | | -120.41 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*839 | 46.8 | Hydrogen bromide | HBr (aq, 5000 H2O) | | | -120.61 | ± 0.16 | kJ/mol | 80.9119 ± 0.0010 | 10035-10-6*844 |
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Most Influential reactions involving CH3CH2Br (l)Please note: The list, which is based on a hat (projection) matrix analysis, is limited to no more than 20 largest influences.
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Influence Coefficient | TN ID | Reaction | Measured Quantity | Reference | 0.500 | 3740.9 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrG°(298.236 K) = 1.263 ± 0.109 kJ/mol | ThermoData 2004, 3rd Law | 0.148 | 3740.4 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(304.6 K) = 27.77 ± 0.20 kJ/mol | Svoboda 1977, Majer 1985, est unc | 0.148 | 3740.5 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(311.9 K) = 27.29 ± 0.20 kJ/mol | Svoboda 1977, Majer 1985, est unc | 0.135 | 3740.7 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(305.99 K) = 6.632 ± 0.05 kcal/mol | de Kolossowsky 1934, ThermoData 2004, est unc | 0.042 | 3740.6 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(322.7 K) = 26.54 ± 0.20 (×1.874) kJ/mol | Svoboda 1977, Majer 1985, est unc | 0.017 | 3740.3 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(298.15 K) = 27.88 ± 0.59 kJ/mol | ThermoData 2004 | 0.003 | 3740.1 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(298.15 K) = 6.6 ± 0.3 kcal/mol | Cox 1970, as quoted by Pedley 1986 | 0.002 | 3740.8 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(298.236 K) = 28.350 ± 1.718 kJ/mol | ThermoData 2004, 2nd Law | 0.001 | 3741.1 | 2 CH3CH2Br (l) + H2 (g) → 2 C2H6 (g) + Br2 (cr,l)  | ΔrH°(298.15 K) = 5.6 ± 3.0 kcal/mol | Ashcroft 1965, Cox 1970 | 0.000 | 3740.2 | CH3CH2Br (l) → CH3CH2Br (g)  | ΔrH°(298.15 K) = 28.26 ± 2.83 kJ/mol | Majer 1985 |
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References
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1
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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]
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2
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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]
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3
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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
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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]
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5
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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]
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6
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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]
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7
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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]
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Formula
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The aggregate state is given in parentheses following the formula, such as: g - gas-phase, cr - crystal, l - liquid, etc.
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Uncertainties
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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.
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Website Functionality Credits
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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/.
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Acknowledgement
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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.
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