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

This version of ATcT results was generated from an expansion of version 1.122b [4][5] to include the enthalpies of formation of methylamine, dimethylamine and trimethylamine that were used as reference values to derive the bond dissociation energies of 20 diatomic molecules containing 3d transition metals.[6].

Species Name Formula Image    ΔfH°(0 K)    ΔfH°(298.15 K) Uncertainty Units Relative
Molecular
Mass
ATcT ID
Chloromethane cation[CH3Cl]+ (g)C[Cl+]1015.111008.34± 0.25kJ/mol50.4867 ±
0.0012
12538-71-5*0

Representative Geometry of [CH3Cl]+ (g)

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Top contributors to the provenance of ΔfH° of [CH3Cl]+ (g)

The 20 contributors listed below account only for 50.4% of the provenance of ΔfH° of [CH3Cl]+ (g).
A total of 231 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
20.33912.1 CH3Cl (g) + 3/2 O2 (g) → CO2 (g) H2O (cr,l) HCl (aq, 600 H2O) ΔrH°(298.15 K) = -764.00 ± 0.50 (×1.067) kJ/molFletcher 1971
4.63929.1 CH3Br (g) → [CH3]+ (g) Br (g) ΔrH°(0 K) = 12.834 ± 0.002 (×4.967) eVSong 2001
3.03932.1 CH3Br (g) H2 (g) → CH4 (g) HBr (g) ΔrH°(523.15 K) = -18.062 ± 0.321 kcal/molFowell 1965
2.33916.10 CH3Cl (g) H (g) → CH4 (g) Cl (g) ΔrH°(0 K) = -7296 ± 100 (×1.297) cm-1Czako 2012
2.03908.4 CH3Cl (g) → C (g) + 3 H (g) Cl (g) ΔrH°(0 K) = 371.34 ± 0.4 kcal/molFeller 2008
1.74136.1 CH3Cl (g) → CHCl3 (g) + 2 CH4 (g) ΔrH°(0 K) = -2.71 ± 1.2 kcal/molRuscic G3B3
1.54136.2 CH3Cl (g) → CHCl3 (g) + 2 CH4 (g) ΔrH°(0 K) = -3.16 ± 1.2 (×1.044) kcal/molRuscic G3
1.53944.4 CH3Br (g) → CBr4 (g) + 3 CH4 (g) ΔrH°(0 K) = 2.77 ± 1.0 kcal/molRuscic G4
1.31852.1 H2 (g) C (graphite) → CH4 (g) ΔrG°(1165 K) = 37.521 ± 0.068 kJ/molSmith 1946, note COf, 3rd Law
1.33948.1 CH3Br (l) H2 (g) → 2 CH4 (g) Br2 (cr,l) ΔrH°(298.15 K) = -6.60 ± 0.60 (×1.445) kcal/molAdams 1966, as quoted by Cox 1970
1.23944.3 CH3Br (g) → CBr4 (g) + 3 CH4 (g) ΔrH°(0 K) = 2.69 ± 1.1 kcal/molRuscic G3X
1.24105.6 CH4 (g) CH2Cl2 (g) → 2 CH3Cl (g) ΔrH°(0 K) = 0.80 ± 0.9 kcal/molRuscic W1RO
1.23931.3 CH3Br (g) HBr (g) → Br2 (g) CH4 (g) ΔrG°(712.2 K) = 35.8 ± 1.6 kJ/molFerguson 1973, 3rd Law
1.13929.3 CH3Br (g) → [CH3]+ (g) Br (g) ΔrH°(0 K) = 12.82 ± 0.02 eVTraeger 1981, AE corr, note unc2
1.04105.4 CH4 (g) CH2Cl2 (g) → 2 CH3Cl (g) ΔrH°(0 K) = 1.37 ± 1.0 kcal/molRuscic G4
0.93909.1 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 91057.0 ± 2.0 cm-1Grutter 2011
0.83946.2 CH3Br (g) CCl4 (g) → 4 CH3Cl (g) CBr4 (g) ΔrH°(0 K) = 3.39 ± 1.0 kcal/molRuscic G4
0.83916.9 CH3Cl (g) H (g) → CH4 (g) Cl (g) ΔrH°(0 K) = -21.11 ± 0.6 kcal/molFeller 2008, note unc2
0.83945.2 CH3Br (g) CF4 (g) → 4 CH3F (g) CBr4 (g) ΔrH°(0 K) = 54.31 ± 1.0 (×1.067) kcal/molRuscic G4
0.84105.3 CH4 (g) CH2Cl2 (g) → 2 CH3Cl (g) ΔrH°(0 K) = 1.66 ± 1.1 kcal/molRuscic G3X

Top 10 species with enthalpies of formation correlated to the ΔfH° of [CH3Cl]+ (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
99.5 ChloromethaneCH3Cl (g)CCl-74.17-82.10± 0.25kJ/mol50.4872 ±
0.0012
74-87-3*0
98.6 ChloromethaneCH3Cl (l)CCl-105.96-101.99± 0.25kJ/mol50.4872 ±
0.0012
74-87-3*590
81.4 Methyl bromideCH3Br (g)CBr-20.18-35.58± 0.27kJ/mol94.9385 ±
0.0013
74-83-9*0
80.2 Methyl bromide cation[CH3Br]+ (g)C[Br+]996.93982.01± 0.27kJ/mol94.9380 ±
0.0013
12538-70-4*0
79.2 Methyl bromideCH3Br (l)CBr-55.90-58.92± 0.28kJ/mol94.9385 ±
0.0013
74-83-9*590
25.1 TetrabromomethaneCBr4 (g)C(Br)(Br)(Br)Br133.2103.5± 1.3kJ/mol331.6267 ±
0.0041
558-13-4*0
22.5 TetrabromomethaneCBr4 (cr, monoclinic)C(Br)(Br)(Br)Br49.0± 1.4kJ/mol331.6267 ±
0.0041
558-13-4*500
20.4 BromoformCBr3H (g)C(Br)(Br)Br75.249.1± 1.3kJ/mol252.7306 ±
0.0031
75-25-2*0
20.3 BromoformCBr3H (l)C(Br)(Br)Br3.0± 1.3kJ/mol252.7306 ±
0.0031
75-25-2*590
-17.7 Hydrogen bromideHBr (g)Br-27.72-35.57± 0.16kJ/mol80.9119 ±
0.0010
10035-10-6*0

Most Influential reactions involving [CH3Cl]+ (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
0.9863909.1 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 91057.0 ± 2.0 cm-1Grutter 2011
0.0063909.2 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.289 ± 0.003 eVKarlsson 1977
0.0023909.3 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.290 ± 0.005 eVLocht 2001a, est unc, Locht 2001
0.0013910.4 [CH3Cl]+ (g) → C (g) + 3 H (g) Cl (g) ΔrH°(0 K) = 111.90 ± 1.50 kcal/molRuscic W1RO
0.0013910.2 [CH3Cl]+ (g) → C (g) + 3 H (g) Cl (g) ΔrH°(0 K) = 112.02 ± 1.60 kcal/molRuscic G4
0.0013910.1 [CH3Cl]+ (g) → C (g) + 3 H (g) Cl (g) ΔrH°(0 K) = 111.80 ± 1.72 kcal/molRuscic G3X
0.0003909.6 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.01 eVWerner 1974
0.0003909.5 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.01 eVLocht 2001, est unc
0.0003909.4 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.296 ± 0.010 eVLocht 2001, est unc
0.0003909.13 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.01 eVWatanabe 1957
0.0003909.7 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.01 eVWatanabe 1962
0.0003909.8 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.01 eVDibeler 1965, est unc
0.0003909.9 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.02 eVTurner 1970, est unc
0.0003909.10 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.29 ± 0.02 eVRagle 1970, est unc
0.0003909.11 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.29 ± 0.02 eVFrost 1970
0.0003909.12 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.28 ± 0.02 eVPotts 1970, est unc
0.0003909.14 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 11.26 ± 0.02 (×1.509) eVDewar 1969a, est unc
0.0003909.15 CH3Cl (g) → [CH3Cl]+ (g) ΔrH°(0 K) = 90500 ± 500 (×1.114) cm-1Price 1936, est unc


References (for your convenience, also available in RIS and BibTex format)
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. 1.122d of the Thermochemical Network, Argonne National Laboratory (2018); 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   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]
6   L. Cheng, J. Gauss, B. Ruscic, P. Armentrout, and J. Stanton,
Bond Dissociation Energies for Diatomic Molecules Containing 3d Transition Metals: Benchmark Scalar-Relativistic Coupled-Cluster Calculations for Twenty Molecules.
J. Chem. Theory Comput. 13, 1044-1056 (2017) [DOI: 10.1021/acs.jctc.6b00970]
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.