Selected ATcT [1, 2] enthalpy of formation based on version 1.124 of the Thermochemical Network [3] This version of ATcT results was generated by additional expansion of version 1.122x [4] to include additional information relevant to the study of thermophysical and thermochemical properties of CH2 and CH3 using nonrigid rotor anharmonic oscillator (NRRAO) partition functions [5], the development and benchmarking of a state-of-the-art computational approach that aims to reproduce total atomization energies of small molecules within 10–15 cm-1 [6], as well as the study of the reversible reaction C2H3 + H2 ⇌ C2H4 + H ⇌ C2H5 [7]
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Diazene anion |
Formula: [HNNH]- (g, trans-cis equilib) |
CAS RN: 100429-75-2 |
ATcT ID: 100429-75-2*1 |
SMILES: N=[NH-] |
InChI: InChI=1S/H2N2/c1-2/h1-2H/q-1 |
InChIKey: YPQDUMCQFFJGOA-UHFFFAOYSA-N |
Hills Formula: H2N2- |
2D Image: |
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Aliases: [HNNH]-; Diazene anion; Diazene ion (1-); Diimide anion; Diimide ion (1-); Diimine anion; Diimine ion (1-); HNNH- g, trans-cis-iso equilib; HNNH- g,trans-cis-iso equilib; [HNNH]- g, trans-cis-iso equilib; [HNNH]- g,trans-cis-iso equilib; N2H2- g, trans-cis-iso equilib; N2H2- g,trans-cis-iso equilib; [N2H2]- g, trans-cis-iso equilib; [N2H2]- g,trans-cis-iso equilib; HNNH- g, trans-cis equilib; HNNH- g,trans-cis equilib; [HNNH]- g, trans-cis equilib; [HNNH]- g,trans-cis equilib; N2H2- g, trans-cis equilib; N2H2- g,trans-cis equilib; [N2H2]- g, trans-cis equilib; [N2H2]- g,trans-cis equilib |
Relative Molecular Mass: 30.02991 ± 0.00020 |
ΔfH°(0 K) | ΔfH°(298.15 K) | Uncertainty | Units |
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265.5 | 258.7 | ± 2.0 | kJ/mol |
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3D Image of [HNNH]- (g, trans-cis equilib) |
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Top contributors to the provenance of ΔfH° of [HNNH]- (g, trans-cis equilib)The 20 contributors listed below account only for 88.2% of the provenance of ΔfH° of [HNNH]- (g, trans-cis equilib). A total of 22 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.
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Contribution (%) | TN ID | Reaction | Measured Quantity | Reference | 15.7 | 1764.8 | [HNNH]- (g, trans) → HNNH (g, trans)  | ΔrH°(0 K) = -0.592 ± 0.050 eV | Ruscic W1RO | 10.5 | 1764.4 | [HNNH]- (g, trans) → HNNH (g, trans)  | ΔrH°(0 K) = -0.608 ± 0.061 eV | Ruscic G4 | 8.0 | 1770.8 | [HNNH]- (g, cis) → HNNH (g, cis)  | ΔrH°(0 K) = -0.516 ± 0.050 eV | Ruscic W1RO | 6.2 | 1779.8 | [NNH2]- (g) → NNH2 (g)  | ΔrH°(0 K) = -0.732 ± 0.050 eV | Ruscic W1RO | 5.4 | 1764.3 | [HNNH]- (g, trans) → HNNH (g, trans)  | ΔrH°(0 K) = -0.644 ± 0.085 eV | Ruscic G3X | 5.4 | 1770.4 | [HNNH]- (g, cis) → HNNH (g, cis)  | ΔrH°(0 K) = -0.535 ± 0.061 eV | Ruscic G4 | 4.8 | 1764.7 | [HNNH]- (g, trans) → HNNH (g, trans)  | ΔrH°(0 K) = -0.593 ± 0.090 eV | Ruscic CBS-n | 4.6 | 1764.6 | [HNNH]- (g, trans) → HNNH (g, trans)  | ΔrH°(0 K) = -0.598 ± 0.092 eV | Ruscic CBS-n | 4.1 | 1779.4 | [NNH2]- (g) → NNH2 (g)  | ΔrH°(0 K) = -0.752 ± 0.061 eV | Ruscic G4 | 2.7 | 1770.3 | [HNNH]- (g, cis) → HNNH (g, cis)  | ΔrH°(0 K) = -0.569 ± 0.085 eV | Ruscic G3X | 2.4 | 1770.7 | [HNNH]- (g, cis) → HNNH (g, cis)  | ΔrH°(0 K) = -0.518 ± 0.090 eV | Ruscic CBS-n | 2.3 | 1770.6 | [HNNH]- (g, cis) → HNNH (g, cis)  | ΔrH°(0 K) = -0.526 ± 0.092 eV | Ruscic CBS-n | 2.1 | 1779.3 | [NNH2]- (g) → NNH2 (g)  | ΔrH°(0 K) = -0.810 ± 0.085 eV | Ruscic G3X | 2.0 | 1800.8 | [HNNH]- (g, trans) → [HNNH]- (g, cis)  | ΔrH°(0 K) = 1158 ± 300 cm-1 | Ruscic W1RO | 1.9 | 1800.7 | [HNNH]- (g, trans) → [HNNH]- (g, cis)  | ΔrH°(0 K) = 1214 ± 310 cm-1 | Ruscic CBS-n | 1.9 | 1800.4 | [HNNH]- (g, trans) → [HNNH]- (g, cis)  | ΔrH°(0 K) = 1210 ± 310 cm-1 | Ruscic G4 | 1.9 | 1779.7 | [NNH2]- (g) → NNH2 (g)  | ΔrH°(0 K) = -0.782 ± 0.090 eV | Ruscic CBS-n | 1.8 | 1800.3 | [HNNH]- (g, trans) → [HNNH]- (g, cis)  | ΔrH°(0 K) = 1268 ± 315 cm-1 | Ruscic G3X | 1.8 | 1801.8 | [HNNH]- (g, trans) → [NNH2]- (g)  | ΔrH°(0 K) = 9424 ± 420 cm-1 | Ruscic W1RO | 1.8 | 1779.6 | [NNH2]- (g) → NNH2 (g)  | ΔrH°(0 K) = -0.824 ± 0.092 eV | Ruscic CBS-n |
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Top 10 species with enthalpies of formation correlated to the ΔfH° of [HNNH]- (g, trans-cis equilib) |
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 | (E)-Diazene anion | [HNNH]- (g, trans) | | 265.5 | 258.7 | ± 2.0 | kJ/mol | 30.02991 ± 0.00020 | *59952-06-6*0 | 100.0 | Diazene anion | [HNNH]- (g, trans-cis-iso equilib) | | 265.5 | 258.7 | ± 2.0 | kJ/mol | 30.02991 ± 0.00020 | 100429-75-2*0 | 73.7 | (Z)-Diazene anion | [HNNH]- (g, cis) | | 280.0 | 273.3 | ± 2.0 | kJ/mol | 30.02991 ± 0.00020 | *86631-37-0*0 | 62.6 | Isodiazene anion | [NNH2]- (g) | | 380.9 | 374.1 | ± 2.1 | kJ/mol | 30.02991 ± 0.00020 | *63986-30-1*0 | 16.7 | Diazene | HNNH (g, trans-cis equilib) | | 207.12 | 199.98 | ± 0.41 | kJ/mol | 30.02936 ± 0.00020 | 3618-05-1*1 | 16.7 | Diazene | HNNH (g, trans-cis-iso equilib) | | 207.12 | 199.98 | ± 0.41 | kJ/mol | 30.02936 ± 0.00020 | 3618-05-1*0 | 16.7 | (E)-Diazene | HNNH (g, trans) | | 207.12 | 199.98 | ± 0.41 | kJ/mol | 30.02936 ± 0.00020 | 15626-43-4*0 | 15.4 | (Z)-Diazene | HNNH (g, cis) | | 228.83 | 221.69 | ± 0.63 | kJ/mol | 30.02936 ± 0.00020 | 15626-42-3*0 | 14.9 | Isodiazene | NNH2 (g) | | 307.54 | 300.46 | ± 0.63 | kJ/mol | 30.02936 ± 0.00020 | 28647-38-3*0 | 10.1 | (E)-Diazene cation | [HNNH]+ (g, trans) | | 1132.49 | 1125.55 | ± 0.64 | kJ/mol | 30.02881 ± 0.00020 | 59952-06-6*0 |
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Most Influential reactions involving [HNNH]- (g, trans-cis equilib)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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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,
Introduction to Active Thermochemical Tables: Several "Key" Enthalpies of Formation Revisited.
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,
Active Thermochemical Tables: Thermochemistry for the 21st Century.
J. Phys. Conf. Ser. 16, 561-570 (2005)
[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. 1.124 of the Thermochemical Network, Argonne National Laboratory, Lemont, Illinois 2022; available at ATcT.anl.gov [DOI: 10.17038/CSE/1885923]
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4
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Y. Ren, L. Zhou, A. Mellouki, V. Daële, M. Idir, S. S. Brown, B. Ruscic, Robert S. Paton, M. R. McGillen, and A. R. Ravishankara,
Reactions of NO3 with Aromatic Aldehydes: Gas-Phase Kinetics and Insights into the Mechanism of the Reaction.
Atmos. Chem. Phys. 21, 13537-13551 (2021)
[DOI: 10.5194/acp2021-228]
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5
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B. Ruscic and D. H. Bross,
Active Thermochemical Tables: The Thermophysical and Thermochemical Properties of Methyl, CH3, and Methylene, CH2, Corrected for Nonrigid Rotor and Anharmonic Oscillator Effects.
Mol. Phys. e1969046 (2021)
[DOI: 10.1080/00268976.2021.1969046]
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6
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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]
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7
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T. L. Nguyen, D. H. Bross, B. Ruscic, G. B. Ellison, and J. F. Stanton,
Mechanism, Thermochemistry, and Kinetics of the Reversible Reactions: C2H3 + H2 ⇌ C2H4 + H ⇌ C2H5.
Faraday Discuss. , (Advance Article) (2022)
[DOI: 10.1039/D1FD00124H]
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8
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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)
[DOI: 10.1002/qua.24605]
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9
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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]
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Formula
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The aggregate state is given in parentheses following the formula, such as: g - gas-phase, cr - crystal, l - liquid, etc.
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Uncertainties
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The listed uncertainties correspond to estimated 95% confidence limits, as customary in thermochemistry (see, for example, Ruscic [8,9]).
Note that an uncertainty of ± 0.000 kJ/mol indicates that the estimated uncertainty is < ± 0.0005 kJ/mol.
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Website Functionality Credits
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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/.
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Acknowledgement
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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.
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