Selected ATcT [1, 2] enthalpy of formation based on version 1.122r of the Thermochemical Network [3] This version of ATcT results was generated from an expansion of version 1.122q [4, 5] to include a non-rigid rotor anharmonic oscillator (NRRAO) partition function for hydroxymethyl [6], as well as data on 42 additional species, some of which are related to soot formation mechanisms.
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Species Name |
Formula |
Image |
ΔfH°(0 K) |
ΔfH°(298.15 K) |
Uncertainty |
Units |
Relative Molecular Mass |
ATcT ID |
2-Cyanovinyl | CHCHCN (g, syn) | | 448.0 | 445.5 | ± 1.2 | kJ/mol | 52.0547 ± 0.0024 | 189141-20-6*2 |
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Representative Geometry of CHCHCN (g, syn) |
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spin ON spin OFF |
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Top contributors to the provenance of ΔfH° of CHCHCN (g, syn)The 9 contributors listed below account for 43.1% of the provenance of ΔfH° of CHCHCN (g, syn).
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 | 13.5 | 5988.1 | 3 CH4 (g) + NH3 (g) → CHCHCN (g, syn) + 13/2 H2 (g)  | ΔrH°(0 K) = 685.45 ± 3.0 kJ/mol | Klippenstein 2017 | 9.5 | 5991.1 | CHCHCN (g, syn) → CH2CCN (g)  | ΔrH°(0 K) = -30.90 ± 3.0 kJ/mol | Klippenstein 2017 | 3.0 | 5990.5 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = -2 ± 300 cm-1 | Ruscic W1RO | 3.0 | 5979.5 | CHCHCN (g, syn) → 3 C (g) + 2 H (g) + N (g)  | ΔrH°(0 K) = 618.78 ± 1.50 kcal/mol | Ruscic W1RO | 2.8 | 5990.4 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = 98 ± 310 cm-1 | Ruscic CBS-n | 2.8 | 5990.2 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = -22 ± 310 cm-1 | Ruscic G4 | 2.7 | 5990.1 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = -11 ± 315 cm-1 | Ruscic G3X | 2.6 | 5979.4 | CHCHCN (g, syn) → 3 C (g) + 2 H (g) + N (g)  | ΔrH°(0 K) = 617.59 ± 1.60 kcal/mol | Ruscic CBS-n | 2.6 | 5979.2 | CHCHCN (g, syn) → 3 C (g) + 2 H (g) + N (g)  | ΔrH°(0 K) = 619.69 ± 1.60 kcal/mol | Ruscic G4 |
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Top 10 species with enthalpies of formation correlated to the ΔfH° of CHCHCN (g, syn) |
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 | 100.0 | 2-Cyanovinyl | CHCHCN (g) | | 448.0 | 445.5 | ± 1.2 | kJ/mol | 52.0547 ± 0.0024 | 189141-20-6*0 | 44.5 | 2-Cyanovinyl | CHCHCN (g, anti) | | 448.0 | 445.5 | ± 1.1 | kJ/mol | 52.0547 ± 0.0024 | 189141-20-6*1 | 32.5 | 2-Isocyanovinyl | CHCHNC (g, syn) | | 544.6 | 542.6 | ± 1.7 | kJ/mol | 52.0547 ± 0.0024 | 225798-14-1*2 | 28.7 | 2-Cyanovinylium | [CHCHCN]+ (g, syn triplet) | | 1517.4 | 1515.2 | ± 1.8 | kJ/mol | 52.0542 ± 0.0024 | 85398-67-0*22 | 26.3 | 2-Isocyanovinyl | CHCHNC (g) | | 543.2 | 541.8 | ± 1.7 | kJ/mol | 52.0547 ± 0.0024 | 225798-14-1*0 | 26.3 | 2-Isocyanovinyl | CHCHNC (g, anti) | | 543.2 | 541.2 | ± 1.7 | kJ/mol | 52.0547 ± 0.0024 | 225798-14-1*1 | 26.2 | 2-Cyanovinyl anion | [CHCHCN]- (g, syn) | | 263.8 | 260.8 | ± 1.8 | kJ/mol | 52.0553 ± 0.0024 | *85398-67-0*2 | 26.2 | 2-Cyanovinyl anion | [CHCHCN]- (g) | | 263.8 | 261.4 | ± 1.8 | kJ/mol | 52.0553 ± 0.0024 | *85398-67-0*0 | 23.6 | 2-Cyanovinylium | [CHCHCN]+ (g, anti triplet) | | 1517.2 | 1515.1 | ± 1.8 | kJ/mol | 52.0542 ± 0.0024 | 85398-67-0*21 | 23.6 | 2-Cyanovinylium | [CHCHCN]+ (g, triplet) | | 1517.2 | 1515.1 | ± 1.8 | kJ/mol | 52.0542 ± 0.0024 | 85398-67-0*2 |
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Most Influential reactions involving CHCHCN (g, syn)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 | 1.000 | 5989.1 | CHCHCN (g) → CHCHCN (g, syn)  | ΔrH°(0 K) = 0 ± 0 cm-1 | Ruscic CBS-n, Ruscic G3X | 0.219 | 5991.1 | CHCHCN (g, syn) → CH2CCN (g)  | ΔrH°(0 K) = -30.90 ± 3.0 kJ/mol | Klippenstein 2017 | 0.209 | 5981.5 | CHCHCN (g, syn) → [CHCHCN]+ (g, syn triplet)  | ΔrH°(0 K) = 11.090 ± 0.040 eV | Ruscic W1RO | 0.143 | 5983.5 | [CHCHCN]- (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = 1.895 ± 0.050 eV | Ruscic W1RO | 0.137 | 5988.1 | 3 CH4 (g) + NH3 (g) → CHCHCN (g, syn) + 13/2 H2 (g)  | ΔrH°(0 K) = 685.45 ± 3.0 kJ/mol | Klippenstein 2017 | 0.111 | 6004.5 | CHCHNC (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = -23.42 ± 1.2 kcal/mol | Ruscic W1RO | 0.103 | 5990.5 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = -2 ± 300 cm-1 | Ruscic W1RO | 0.096 | 5990.2 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = -22 ± 310 cm-1 | Ruscic G4 | 0.096 | 5990.4 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = 98 ± 310 cm-1 | Ruscic CBS-n | 0.096 | 5983.2 | [CHCHCN]- (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = 1.916 ± 0.061 eV | Ruscic G4 | 0.095 | 6004.4 | CHCHNC (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = -22.76 ± 1.3 kcal/mol | Ruscic CBS-n | 0.095 | 6004.2 | CHCHNC (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = -22.89 ± 1.3 kcal/mol | Ruscic G4 | 0.093 | 5990.1 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = -11 ± 315 cm-1 | Ruscic G3X | 0.082 | 6004.1 | CHCHNC (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = -23.46 ± 1.4 kcal/mol | Ruscic G3X | 0.076 | 5990.3 | CHCHCN (g, syn) → CHCHCN (g, anti)  | ΔrH°(0 K) = 13 ± 350 cm-1 | Ruscic CBS-n | 0.062 | 5981.2 | CHCHCN (g, syn) → [CHCHCN]+ (g, syn triplet)  | ΔrH°(0 K) = 11.116 ± 0.073 eV | Ruscic G4 | 0.062 | 6004.3 | CHCHNC (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = -22.90 ± 1.6 kcal/mol | Ruscic CBS-n | 0.059 | 5981.4 | CHCHCN (g, syn) → [CHCHCN]+ (g, syn triplet)  | ΔrH°(0 K) = 11.045 ± 0.075 eV | Ruscic CBS-n | 0.049 | 5983.1 | [CHCHCN]- (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = 1.927 ± 0.085 eV | Ruscic G3X | 0.044 | 5983.4 | [CHCHCN]- (g, syn) → CHCHCN (g, syn)  | ΔrH°(0 K) = 1.922 ± 0.090 eV | Ruscic CBS-n |
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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,
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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,
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[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. 1.122r of the Thermochemical Network, Argonne National Laboratory, Lemont, Illinois 2021 [DOI: 10.17038/CSE/1822363]; available at ATcT.anl.gov
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4
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D. Feller, D. H. Bross, and B. Ruscic,
Enthalpy of Formation of C2H2O4 (Oxalic Acid) from High-Level Calculations and the Active Thermochemical Tables Approach.
J. Phys. Chem. A 123, 3481-3496 (2019)
[DOI: 10.1021/acs.jpca.8b12329]
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5
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B. K. Welch, R. Dawes, D. H. Bross, and B. Ruscic,
An Automated Thermochemistry Protocol Based on Explicitly Correlated Coupled-Cluster Theory: The Methyl and Ethyl Peroxy Families.
J. Phys. Chem. A 123, 5673-5682 (2019)
[DOI: 10.1021/acs.jpca.8b12329]
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6
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D. H. Bross, H.-G. Yu, L. B. Harding, and B. Ruscic,
Active Thermochemical Tables: The Partition Function of Hydroxymethyl (CH2OH) Revisited.
J. Phys. Chem. A 123, 4212-4231 (2019)
[DOI: 10.1021/acs.jpca.9b02295]
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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)
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