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 |
Iodomethane | CH3I (g) | | 24.51 | 14.98 | ± 0.18 | kJ/mol | 141.93899 ± 0.00083 | 74-88-4*0 |
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Representative Geometry of CH3I (g) |
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spin ON spin OFF |
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Top contributors to the provenance of ΔfH° of CH3I (g)The 9 contributors listed below account for 91.3% of the provenance of ΔfH° of CH3I (g).
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 | 45.7 | 4693.2 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.251 ± 0.0024 eV | Lee 2007 | 25.6 | 4693.1 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.248 ± 0.003 (×1.067) eV | Bodi 2009 | 4.1 | 1936.1 | 2 H2 (g) + C (graphite) → CH4 (g)  | ΔrG°(1165 K) = 37.521 ± 0.068 kJ/mol | Smith 1946, note COf, 3rd Law | 4.1 | 4693.3 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.243 ± 0.008 eV | Lee 2007, Bodi 2009 | 3.6 | 4695.4 | CH3I (g) + HI (g) → I2 (g) + CH4 (g)  | ΔrG°(669 K) = -10.34 ± 0.09 (×2.181) kcal/mol | Goy 1965, 3rd Law | 3.4 | 4695.2 | CH3I (g) + HI (g) → I2 (g) + CH4 (g)  | ΔrG°(630.5 K) = -10.48 ± 0.08 (×2.538) kcal/mol | Golden 1965, 3rd Law, Cox 1970 | 2.4 | 4693.5 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.24 ± 0.01 (×1.044) eV | Mintz 1976 | 1.3 | 4707.1 | 2 CH3I (l) + 7/2 O2 (g) → 2 CO2 (g) + 3 H2O (l) + I2 (cr,l)  | ΔrH°(298.15 K) = -1617.2 ± 0.6 (×4.861) kJ/mol | Carson 1993 | 0.8 | 4708.1 | 2 CH3I (l) + H2 (g) → 2 CH4 (g) + I2 (cr,l)  | ΔrH°(298.15 K) = -30.0 ± 0.8 kcal/mol | Carson 1961, note unc, Cox 1970 |
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Top 10 species with enthalpies of formation correlated to the ΔfH° of CH3I (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.
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Correlation Coefficent (%) | Species Name | Formula | Image | ΔfH°(0 K) | ΔfH°(298.15 K) | Uncertainty | Units | Relative Molecular Mass | ATcT ID | 99.7 | Iodomethane cation | [CH3I]+ (g) | | 944.80 | 935.40 | ± 0.18 | kJ/mol | 141.93844 ± 0.00083 | 12538-72-6*0 | 89.5 | Iodomethane | CH3I (l) | | | -12.17 | ± 0.19 | kJ/mol | 141.93899 ± 0.00083 | 74-88-4*590 | 28.9 | Methylium | [CH3]+ (g) | | 1099.339 | 1095.396 | ± 0.050 | kJ/mol | 15.03397 ± 0.00083 | 14531-53-4*0 | 28.2 | Methane | CH4 (g) | | -66.557 | -74.526 | ± 0.049 | kJ/mol | 16.04246 ± 0.00085 | 74-82-8*0 | 26.2 | Methyl | CH3 (g) | | 149.866 | 146.452 | ± 0.055 | kJ/mol | 15.03452 ± 0.00083 | 2229-07-4*0 | 22.8 | Methane cation | [CH4]+ (g) | | 1150.673 | 1144.290 | ± 0.062 | kJ/mol | 16.04191 ± 0.00085 | 20741-88-2*0 | 9.6 | Carbon | C (g) | | 711.398 | 716.883 | ± 0.045 | kJ/mol | 12.01070 ± 0.00080 | 7440-44-0*0 | 9.6 | Carbon | C (g, triplet) | | 711.398 | 716.883 | ± 0.045 | kJ/mol | 12.01070 ± 0.00080 | 7440-44-0*1 | 9.6 | Carbon | C (g, singlet) | | 833.329 | 838.475 | ± 0.045 | kJ/mol | 12.01070 ± 0.00080 | 7440-44-0*2 | 9.6 | Carbon | C (g, quintuplet) | | 1114.961 | 1120.107 | ± 0.045 | kJ/mol | 12.01070 ± 0.00080 | 7440-44-0*3 |
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Most Influential reactions involving CH3I (g)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 | 0.904 | 4692.3 | CH3I (g) → [CH3I]+ (g)  | ΔrH°(0 K) = 76930.0 ± 1.0 cm-1 | Baig 1981 | 0.500 | 4693.2 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.251 ± 0.0024 eV | Lee 2007 | 0.458 | 4706.3 | CH3I (l) → CH3I (g)  | ΔrG°(299.19 K) = 1.484 ± 0.125 kJ/mol | Boublik 1972, Fogg 1953, Zaalishvili 1962, Raetzsch 1965, ThermoData 2004 | 0.281 | 4693.1 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.248 ± 0.003 (×1.067) eV | Bodi 2009 | 0.279 | 4706.5 | CH3I (l) → CH3I (g)  | ΔrG°(287.05 K) = 2.578 ± 0.160 kJ/mol | Boublik 1972, Fogg 1953, Zaalishvili 1962, Raetzsch 1965, ThermoData 2004 | 0.247 | 4706.7 | CH3I (l) → CH3I (g)  | ΔrG°(285.78 K) = 2.69 ± 0.17 kJ/mol | Thompson 1936, Fogg 1953, Zaalishvili 1962, Raetzsch 1965, ThermoData 2004 | 0.159 | 2472.2 | ICN (g) + CH3Br (g) → BrCN (g) + CH3I (g)  | ΔrH°(0 K) = 2.43 ± 1.0 kcal/mol | Ruscic unpub | 0.132 | 2472.3 | ICN (g) + CH3Br (g) → BrCN (g) + CH3I (g)  | ΔrH°(0 K) = 2.43 ± 1.1 kcal/mol | Ruscic unpub | 0.116 | 4626.1 | CI4 (g) + 3 CH4 (g) → 4 CH3I (g)  | ΔrH°(298.15 K) = -39.9 ± 12 kJ/mol | Marshall 2005 | 0.111 | 2472.1 | ICN (g) + CH3Br (g) → BrCN (g) + CH3I (g)  | ΔrH°(0 K) = 2.40 ± 1.2 kcal/mol | Ruscic unpub | 0.056 | 4692.1 | CH3I (g) → [CH3I]+ (g)  | ΔrH°(0 K) = 76932 ± 4 cm-1 | Urban 2002 | 0.045 | 4693.3 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.243 ± 0.008 eV | Lee 2007, Bodi 2009 | 0.041 | 4695.4 | CH3I (g) + HI (g) → I2 (g) + CH4 (g)  | ΔrG°(669 K) = -10.34 ± 0.09 (×2.181) kcal/mol | Goy 1965, 3rd Law | 0.038 | 4695.2 | CH3I (g) + HI (g) → I2 (g) + CH4 (g)  | ΔrG°(630.5 K) = -10.48 ± 0.08 (×2.538) kcal/mol | Golden 1965, 3rd Law, Cox 1970 | 0.036 | 4692.2 | CH3I (g) → [CH3I]+ (g)  | ΔrH°(0 K) = 76934 ± 5 cm-1 | Strobel 1994, Strobel 1993 | 0.026 | 4693.5 | CH3I (g) → [CH3]+ (g) + I (g)  | ΔrH°(0 K) = 12.24 ± 0.01 (×1.044) eV | Mintz 1976 | 0.015 | 2469.2 | ICN (g) + CH4 (g) → HCN (g) + CH3I (g)  | ΔrH°(0 K) = -1.03 ± 3.1 kcal/mol | Ruscic unpub | 0.014 | 2469.3 | ICN (g) + CH4 (g) → HCN (g) + CH3I (g)  | ΔrH°(0 K) = -0.97 ± 3.2 kcal/mol | Ruscic unpub | 0.012 | 2469.1 | ICN (g) + CH4 (g) → HCN (g) + CH3I (g)  | ΔrH°(0 K) = -0.05 ± 3.4 kcal/mol | Ruscic unpub | 0.008 | 4695.5 | CH3I (g) + HI (g) → I2 (g) + CH4 (g)  | ΔrH°(669 K) = -12.65 ± 0.39 (×1.139) kcal/mol | Goy 1965, 2nd Law |
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References
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1
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