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.

Species Name Formula Image    ΔfH°(0 K)    ΔfH°(298.15 K) Uncertainty Units Relative
Molecular
Mass		 ATcT ID
Ethyl iodideCH3CH2I (l)CCI-9.41-39.28± 0.49kJ/mol155.9656 ±
0.0016		75-03-6*500

Top contributors to the provenance of ΔfH° of CH3CH2I (l)

The 9 contributors listed below account for 94.2% of the provenance of ΔfH° of CH3CH2I (l).

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
67.05006.1 2 CH3CH2I (l) + 13/2 O2 (g) → 4 CO2 (g) + 5 H2O (cr,l) + I2 (cr,l) ΔrH°(298.15 K) = -2925.00 ± 1.16 kJ/molCarson 1994
7.95007.1 2 CH3CH2I (l) + H2 (g) → 2 CH3CH3 (g) + I2 (cr,l) ΔrH°(298.15 K) = -21.2 ± 0.8 kcal/molAshcroft 1965, Cox 1970
7.35004.2 CH3CH2I (g) → [CH3CH2]+ (g) + I (g) ΔrH°(0 K) = 10.52 ± 0.01 (×1.682) eVRosenstock 1982
5.15004.4 CH3CH2I (g) → [CH3CH2]+ (g) + I (g) ΔrH°(0 K) = 10.52 ± 0.02 eVTraeger 1981, AE corr, note unc2
2.15004.1 CH3CH2I (g) → [CH3CH2]+ (g) + I (g) ΔrH°(0 K) = 10.534 ± 0.008 (×3.914) eVBorkar 2010
1.35009.2 CH3CH2I (l) + CH3 (g) → CH3I (l) + CH3CH2 (g) ΔrG°(298.15 K) = -7.5 ± 4 kJ/molCastelhano 1982, note unc3
1.25004.3 CH3CH2I (g) → [CH3CH2]+ (g) + I (g) ΔrH°(0 K) = 10.49 ± 0.04 eVBaer 1980
1.25006.3 2 CH3CH2I (l) + 13/2 O2 (g) → 4 CO2 (g) + 5 H2O (cr,l) + I2 (cr,l) ΔrH°(298.15 K) = -701.0 ± 2.0 (×1.022) kcal/molSpringall 1949, Cox 1970
0.85004.5 CH3CH2I (g) → [CH3CH2]+ (g) + I (g) ΔrH°(0 K) = 10.50 ± 0.05 eVAkopyan 1970, Rosenstock 1982

Top 10 species with enthalpies of formation correlated to the ΔfH° of CH3CH2I (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.

Correlation
Coefficent
(%)		Species Name Formula Image    ΔfH°(0 K)    ΔfH°(298.15 K) Uncertainty Units Relative
Molecular
Mass		 ATcT ID
99.2 Ethyl iodideCH3CH2I (g)CCI8.70-7.18± 0.49kJ/mol155.9656 ±
0.0016		75-03-6*0
14.7 Ethylium[CH3CH2]+ (g)[CH2+]1[CH2][H]1914.95902.88± 0.30kJ/mol29.0606 ±
0.0016		14936-94-8*0
11.6 WaterH2O (g, para)O-238.929-241.832± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*2
11.6 WaterH2O (g)O-238.929-241.832± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*0
11.6 WaterH2O (cr, l, eq.press.)O-286.300-285.828± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*499
11.6 WaterH2O (l, eq.press.)O-285.828± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*589
11.6 Oxonium[H3O]+ (aq)[OH3+]-285.826± 0.026kJ/mol19.02267 ±
0.00037		13968-08-6*800
11.6 WaterH2O (l)O-285.826± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*590
11.6 WaterH2O (cr,l)O-286.298-285.826± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*500
11.6 WaterH2O (g, ortho)O-238.644-241.832± 0.026kJ/mol18.01528 ±
0.00033		7732-18-5*1

Most Influential reactions involving CH3CH2I (l)

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
0.9285005.1 CH3CH2I (l) → CH3CH2I (g) ΔrH°(298.15 K) = 32.08 ± 0.06 kJ/molWadso 1968, Pedley 1986
0.6845006.1 2 CH3CH2I (l) + 13/2 O2 (g) → 4 CO2 (g) + 5 H2O (cr,l) + I2 (cr,l) ΔrH°(298.15 K) = -2925.00 ± 1.16 kJ/molCarson 1994
0.0845007.1 2 CH3CH2I (l) + H2 (g) → 2 CH3CH3 (g) + I2 (cr,l) ΔrH°(298.15 K) = -21.2 ± 0.8 kcal/molAshcroft 1965, Cox 1970
0.0335005.4 CH3CH2I (l) → CH3CH2I (g) ΔrH°(302.530 K) = 7.697 ± 0.044 (×1.719) kcal/molde Kolossowsky 1934, ThermoData 2004, est unc
0.0245005.3 CH3CH2I (l) → CH3CH2I (g) ΔrH°(298.15 K) = 32.47 ± 0.34 (×1.091) kJ/molThermoData 2004
0.0195009.2 CH3CH2I (l) + CH3 (g) → CH3I (l) + CH3CH2 (g) ΔrG°(298.15 K) = -7.5 ± 4 kJ/molCastelhano 1982, note unc3
0.0125006.3 2 CH3CH2I (l) + 13/2 O2 (g) → 4 CO2 (g) + 5 H2O (cr,l) + I2 (cr,l) ΔrH°(298.15 K) = -701.0 ± 2.0 (×1.022) kcal/molSpringall 1949, Cox 1970
0.0105005.5 CH3CH2I (l) → CH3CH2I (g) ΔrH°(344.482 K) = 7.285 ± 0.10 (×1.354) kcal/molKahlenberg 1901, ThermoData 2004, est unc
0.0045008.2 CH3CH2I (l) + CH4 (g) → CH3I (l) + CH3CH3 (g) ΔrH°(298.15 K) = 4.32 ± 1.80 kcal/molCastelhano 1982, note unc
0.0005005.6 CH3CH2I (l) → CH3CH2I (g) ΔrH°(341.250 K) = 30.242 ± 3.058 kJ/molWilson 1989, 2nd Law, ThermoData 2004
0.0005005.8 CH3CH2I (l) → CH3CH2I (g) ΔrH°(298.426 K) = 33.441 ± 3.104 kJ/molThermoData 2004, 2nd Law
0.0005006.4 2 CH3CH2I (l) + 13/2 O2 (g) → 4 CO2 (g) + 5 H2O (cr,l) + I2 (cr,l) ΔrH°(298.15 K) = -712.0 ± 20 kcal/molBerthelot 1900, Springall 1949, est unc
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. 1.122r of the Thermochemical Network, Argonne National Laboratory, Lemont, Illinois 2021 [DOI: 10.17038/CSE/1822363]; available at ATcT.anl.gov
4   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]
5   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]
6   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]
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.