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].

Acetonitrile

Formula: CH3CN (g)
CAS RN: 75-05-8
ATcT ID: 75-05-8*0
SMILES: CC#N
InChI: InChI=1S/C2H3N/c1-2-3/h1H3
InChIKey: WEVYAHXRMPXWCK-UHFFFAOYSA-N
Hills Formula: C2H3N1

2D Image:

CC#N
Aliases: CH3CN; Acetonitrile; Methyl cyanide; Cyanomethane; Ethanenitrile; Ethyl nitrile; Methanecarbonitrile; H3CCN; H3C-C~N; MeCN; NSC 7593; UN 1648; RCRA U003
Relative Molecular Mass: 41.0520 ± 0.0016

   ΔfH°(0 K)   ΔfH°(298.15 K)UncertaintyUnits
81.1574.09± 0.24kJ/mol

3D Image of CH3CN (g)

spin ON           spin OFF
          

Top contributors to the provenance of ΔfH° of CH3CN (g)

The 20 contributors listed below account only for 85.3% of the provenance of ΔfH° of CH3CN (g).
A total of 41 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
34.62725.1 CH3CN (cr,l) + 11/2 O2 (g) → 4 CO2 (g) + 3 H2O (l) N2 (g) ΔrH°(298.15 K) = -2512.56 ± 0.60 kJ/molAn 1983
22.72725.2 CH3CN (cr,l) + 11/2 O2 (g) → 4 CO2 (g) + 3 H2O (l) N2 (g) ΔrH°(298.15 K) = -2512.76 ± 0.74 kJ/molBarnes 1976, An 1983
5.92724.3 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.50 ± 0.20 kJ/molAn 1983
5.42724.4 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.45 ± 0.21 kJ/molHoward 1970, An 1983
4.92722.9 CH3CN (g) → 2 C (g) + 3 H (g) N (g) ΔrH°(0 K) = 2460.19 ± 1.00 kJ/molNguyen 2018
3.52724.2 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.42 ± 0.26 kJ/molThermoData 2004
1.62731.1 CH4 (g) NH3 (g) → CH3NC (g) + 4 H2 (g) ΔrH°(0 K) = 355.35 ± 1.5 kJ/molKlippenstein 2017
0.92724.1 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.40 ± 0.50 kJ/molMajer 1985
0.82735.6 CH2CN (g) → 2 C (g) + 2 H (g) N (g) ΔrH°(0 K) = 492.78 ± 0.35 kcal/molKarton 2017
0.72740.1 CH4 (g) NH3 (g) → CH2CN (g) + 9/2 H2 (g) ΔrH°(0 K) = 435.33 ± 1.5 kJ/molKlippenstein 2017
0.5125.2 1/2 O2 (g) H2 (g) → H2O (cr,l) ΔrH°(298.15 K) = -285.8261 ± 0.040 kJ/molRossini 1939, Rossini 1931, Rossini 1931b, note H2Oa, Rossini 1930
0.42287.1 H2 (g) C (graphite) → CH4 (g) ΔrG°(1165 K) = 37.521 ± 0.068 kJ/molSmith 1946, note COf, 3rd Law
0.42729.1 CH3CN (g) F- (g) → CH3F (g) [CN]- (g) ΔrH°(0 K) = 1.37 ± 0.8 kcal/molGonzales 2003, est unc
0.32142.7 C (graphite) O2 (g) → CO2 (g) ΔrH°(298.15 K) = -393.464 ± 0.024 kJ/molHawtin 1966, note CO2e
0.32726.5 CH3CN (g) HCCH (g) → HCN (g) CH3CCH (g) ΔrH°(0 K) = 2.92 ± 0.85 kcal/molRuscic W1RO
0.32727.5 CH3CN (g) CH3CCH (g) → HCN (g) CH3CCCH3 (g) ΔrH°(0 K) = 3.82 ± 0.85 kcal/molRuscic W1RO
0.32726.4 CH3CN (g) HCCH (g) → HCN (g) CH3CCH (g) ΔrH°(0 K) = 2.66 ± 0.90 kcal/molRuscic CBS-n
0.32726.2 CH3CN (g) HCCH (g) → HCN (g) CH3CCH (g) ΔrH°(0 K) = 2.93 ± 0.90 kcal/molRuscic G4
0.32726.1 CH3CN (g) HCCH (g) → HCN (g) CH3CCH (g) ΔrH°(0 K) = 3.16 ± 0.90 kcal/molRuscic G3X
0.32727.4 CH3CN (g) CH3CCH (g) → HCN (g) CH3CCCH3 (g) ΔrH°(0 K) = 4.16 ± 0.90 kcal/molRuscic CBS-n

Top 10 species with enthalpies of formation correlated to the ΔfH° of CH3CN (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
86.0 AcetonitrileCH3CN (cr,l)CC#N40.64± 0.22kJ/mol41.0520 ±
0.0016
75-05-8*500
44.5 IsocyanomethaneCH3NC (g)C[N+]#[C-]183.85177.31± 0.46kJ/mol41.0520 ±
0.0016
593-75-9*0
26.8 Cyanomethanide[CH2CN]- (g)[CH2-]C#N113.69110.87± 0.53kJ/mol40.0446 ±
0.0016
21438-99-3*0
26.8 CyanomethylCH2CN (g)[CH2]C#N262.84259.96± 0.53kJ/mol40.0440 ±
0.0016
2932-82-3*0
23.6 Cyanomethylium[CH2CN]+ (g)[CH2+]C#N1256.231253.59± 0.61kJ/mol40.0435 ±
0.0016
34430-18-7*0
17.7 Isocyanomethanide[CH2NC]- (g)[CH2-][N+]#[C-]254.05251.01± 0.89kJ/mol40.0446 ±
0.0016
81704-80-5*0
15.9 Carbonic acidC(O)(OH)2 (aq, undissoc)OC(=O)O-698.665± 0.028kJ/mol62.0248 ±
0.0012
463-79-6*1000
13.8 BenzonitrileC6H5CN (g)c1ccc(cc1)C#N230.03215.84± 0.92kJ/mol103.1213 ±
0.0056
100-47-0*0
13.0 WaterH2O (l)O-285.798± 0.022kJ/mol18.01528 ±
0.00033
7732-18-5*590
13.0 WaterH2O (l, eq.press.)O-285.799± 0.022kJ/mol18.01528 ±
0.00033
7732-18-5*589

Most Influential reactions involving CH3CN (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
0.8485673.1 CH2NN (g) [CH2CN]- (g) → [HCNN]- (g) CH3CN (g) ΔrH°(298.15 K) = -0.40 ± 0.12 kcal/molClifford 1998a
0.3562724.3 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.50 ± 0.20 kJ/molAn 1983
0.3422733.12 CH3CN (g) → CH3NC (g) ΔrH°(0 K) = 103.26 ± 0.7 kJ/molNguyen 2018
0.3232724.4 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.45 ± 0.21 kJ/molHoward 1970, An 1983
0.2102724.2 CH3CN (cr,l) → CH3CN (g) ΔrH°(298.15 K) = 33.42 ± 0.26 kJ/molThermoData 2004
0.1576806.5 C6H5NC (g) CH3CN (g) → C6H5CN (g) CH3NC (g) ΔrH°(0 K) = 2.77 ± 0.85 kcal/molRuscic W1RO
0.1406806.1 C6H5NC (g) CH3CN (g) → C6H5CN (g) CH3NC (g) ΔrH°(0 K) = 2.42 ± 0.90 kcal/molRuscic G3X
0.1406806.4 C6H5NC (g) CH3CN (g) → C6H5CN (g) CH3NC (g) ΔrH°(0 K) = 3.10 ± 0.90 kcal/molRuscic CBS-n
0.1406806.2 C6H5NC (g) CH3CN (g) → C6H5CN (g) CH3NC (g) ΔrH°(0 K) = 2.35 ± 0.90 kcal/molRuscic G4
0.1137723.5 [CH2CCN]- (g) CH3CN (g) → CH2CHCN (g, singlet) [CH2CN]- (g) ΔrH°(0 K) = 0.38 ± 0.8 kcal/molRuscic W1RO
0.1136806.3 C6H5NC (g) CH3CN (g) → C6H5CN (g) CH3NC (g) ΔrH°(0 K) = 2.64 ± 1.00 kcal/molRuscic CBS-n
0.0922734.7 CH3NC (g) HCN (g) → CH3CN (g) HNC (g) ΔrH°(0 K) = -40.9 ± 1.5 kJ/molVogiatzis 2014, est unc
0.0922734.8 CH3NC (g) HCN (g) → CH3CN (g) HNC (g) ΔrH°(0 K) = -40.97 ± 1.5 kJ/molKlippenstein 2017
0.0927664.5 CH3CCN (g, singlet) CH4 (g) → CH3CH (g, singlet) CH3CN (g) ΔrH°(0 K) = 10.35 ± 0.85 kcal/molRuscic W1RO
0.0827664.4 CH3CCN (g, singlet) CH4 (g) → CH3CH (g, singlet) CH3CN (g) ΔrH°(0 K) = 11.29 ± 0.90 kcal/molRuscic CBS-n
0.0827664.2 CH3CCN (g, singlet) CH4 (g) → CH3CH (g, singlet) CH3CN (g) ΔrH°(0 K) = 10.94 ± 0.90 kcal/molRuscic G4
0.0827664.1 CH3CCN (g, singlet) CH4 (g) → CH3CH (g, singlet) CH3CN (g) ΔrH°(0 K) = 11.20 ± 0.90 kcal/molRuscic G3X
0.0817765.5 HCCN (g, triplet) CH4 (g) → CH2 (g, triplet) CH3CN (g) ΔrH°(0 K) = 13.72 ± 0.9 kcal/molRuscic W1RO
0.0752757.5 CH3NC (g) CH2CN (g) → CH2NC (g) CH3CN (g) ΔrH°(0 K) = -0.56 ± 0.85 kcal/molRuscic W1RO
0.0742733.13 CH3CN (g) → CH3NC (g) ΔrH°(0 K) = 103.52 ± 1.5 kJ/molKlippenstein 2017


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. 1.140 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.