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Dinitrogen dioxide
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3D model (JSmol)
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PubChem CID
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| Properties | |
| N2O2 | |
| Molar mass | 60.012 g·mol−1 |
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
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Dinitrogen dioxide is an inorganic compound having molecular formula N
2O
2. Many structural isomers are possible. The covalent bonding pattern O=N–N=O (a non-cyclic dimer of nitric oxide (NO)) is predicted to be the most stable isomer based on ab initio calculations and is the only one that has been experimentally produced.[1] In the solid form, the molecules have C2v symmetry: the entire structure is planar, with the two oxygen atoms cis across the N–N bond. The O–N distance is 1.15 Å, the N–N distance is 2.33 Å, and the O=N–N angle is 95°.[2]
References
[edit]- ^ Nguyen, Kiet A.; Gordon, Mark S.; Montgomery, John A. Jr.; Michels, H. Harvey (October 1994). "Structures, Bonding, and Energetics of N2O2 Isomers". The Journal of Physical Chemistry. 98 (40): 10072–10078. doi:10.1021/j100091a021.
- ^ Park, Jong Keun; Sun, Hosung (1999). "Theoretical Determination of Geometrical Structures of the Nitric Oxide Dimer, (NO)2". Bulletin of the Korean Chemical Society (in Korean). 20 (12): 1399–1408. ISSN 0253-2964.
- East, Allan L. L. (August 8, 1998). "The 16 valence electronic states of nitric oxide dimer (NO)2". Journal of Chemical Physics. 109 (6): 2185–2193. Bibcode:1998JChPh.109.2185E. doi:10.1063/1.476786.
- Harcourt, Richard D. (April 1990). "The origin of the long N–N bond in N2O2: an ab initio valence bond study". Journal of Molecular Structure: THEOCHEM. 206 (3–4): 253–264. doi:10.1016/0166-1280(90)85140-I.[1]
- Dkhissi, Ahmed; Soulard, Pascale; Perrin, Agnès; Lacome, Nelly (May 1997). "The NO Dimer". Journal of Molecular Spectroscopy. 183 (1): 12–17. Bibcode:1997JMoSp.183...12D. doi:10.1006/jmsp.1996.7249.
Dinitrogen dioxide
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Structure
Molecular geometry
Dinitrogen dioxide, (NO)₂, adopts a cis-planar structure as the primary observed isomer, characterized by the covalent bonding pattern O=N–N=O, with double bonds linking each nitrogen to its oxygen and a single bond connecting the two nitrogens. This arrangement arises from the dimerization of nitric oxide molecules, where the unpaired electrons on nitrogen atoms form the central linkage. Multiple isomers are possible, but the cis form predominates under typical experimental conditions.[6] In the gas phase, microwave spectroscopy reveals O–N bond lengths of 1.161 Å, an N–N bond length of 2.236 Å, and an O=N–N bond angle of 99.6°. In the solid state, X-ray crystallography confirms a similar planar cis configuration with N–O distances of approximately 1.12 Å, N–N of 2.18 Å, and O=N–N angle of 95°. The molecule exhibits C_{2v} point group symmetry in its planar cis form, as observed in the solid state, with the plane of symmetry bisecting the N–N bond and perpendicular to the molecular plane. The N–N bond is particularly weak, with a bond order of about 0.5, due to partial multiple bonding character from resonance delocalization involving contributing structures such as ⁻O–N≡N–O⁺ alongside the primary O=N–N=O form.[6]Isomers
Dinitrogen dioxide, N₂O₂, exists in several structural isomers, primarily the cis and trans forms of the (NO)₂ dimer, denoted as cis-ONNO and trans-ONNO, where the nitrogen atoms are connected by a bond with the oxygen atoms oriented accordingly. Additional possible isomers include non-planar twisted configurations and bridged structures, such as the O=N-O-N=O form, which features an oxygen bridge between the two nitrogen atoms. These isomers arise from the weak bonding interactions in the dimerization of nitric oxide, leading to a variety of low-energy arrangements.[5] Theoretical studies have investigated the relative stabilities of these isomers, with ab initio calculations revealing that the cis-ONNO isomer is the most stable in the gas phase, while the trans form lies higher in energy by approximately 1-3 kcal/mol according to advanced methods like CASPT2 and CCSD(T); early MP2 computations showed conflicting results. However, in the solid state, the cis isomer is favored due to intermolecular packing effects that stabilize its planar structure. More advanced multiconfigurational second-order perturbation theory (CASPT2) calculations describe eight low-lying electronic states (four singlets and four triplets) for both cis and trans isomers, highlighting the complex electronic landscape and low barriers for isomerization, often below 1 kcal/mol, which facilitates rapid interconversion under experimental conditions.[7][6] Experimental evidence confirms the existence primarily of the cis-ONNO isomer, characterized by its O=N–N=O connectivity with a central N–N bond. Matrix isolation spectroscopy at low temperatures has identified vibrational signatures unique to this cis form, while solid-state studies of condensed nitric oxide also reveal the cis structure through X-ray diffraction and infrared spectra. No direct spectroscopic observation of the trans or bridged isomers has been reported in neutral N₂O₂, likely due to their higher energy and rapid conversion to the cis form.[1][8]Physical properties
Thermodynamic data
Dinitrogen dioxide (N₂O₂), the dimer of nitric oxide (NO), has a molar mass of 60.012 g/mol.[9] The compound is weakly bound, with the dissociation reaction N₂O₂ (g, cis) ⇌ 2 NO (g) exhibiting an enthalpy change Δ_rH°(0 K) of 697 ± 4 cm⁻¹, equivalent to approximately 2.0 kcal/mol (8.4 kJ/mol).[2] This low dissociation energy underscores the instability of the dimer in the gas phase at ambient conditions, where it predominantly exists as monomers. The standard enthalpy of formation for gaseous cis-N₂O₂ at 298.15 K is 171.12 ± 0.14 kJ/mol (40.91 ± 0.03 kcal/mol).[2] The equilibrium for the dimerization 2 NO (g) ⇌ N₂O₂ (g) is characterized by an equilibrium constant K_p (in atm⁻¹) that decreases with increasing temperature, favoring the dimer at low temperatures (below approximately 200 K) and high pressures.[3] For instance, at 276 K, the dissociation constant K_p (diss) ≈ 3.99 atm, corresponding to a dimerization K_p ≈ 0.25 atm⁻¹, with the equilibrium shifting toward monomers as temperature rises.[10] N₂O₂ exists primarily in the gas phase or as a solid at low temperatures; its pure liquid form is unstable due to the weak N–N bond, but dimers contribute significantly to the properties of liquid nitric oxide, where up to 78% of molecules form N₂O₂ at 120 K under moderate pressure, decreasing to 43% at 144 K.[6]Spectroscopic characteristics
Dinitrogen dioxide, N₂O₂, primarily exists as the cis isomer in low-temperature matrices, exhibiting C_{2v} symmetry that renders its symmetric vibrational modes Raman active. This symmetry facilitates the observation of the symmetric N=O stretch in Raman spectroscopy, providing complementary data to infrared measurements for structural confirmation. Theoretical calculations and experimental spectra confirm that the cis form dominates under isolation conditions, with the trans isomer being less stable and rarely observed.[11] Infrared spectroscopy reveals characteristic absorption bands for the cis isomer in argon matrices at approximately 10 K, including the asymmetric N=O stretch at ~1,740 cm⁻¹ and the N–N stretch at ~300 cm⁻¹. These low-temperature matrix isolation studies, using Fourier transform infrared techniques, provide evidence for the cis configuration through isotopic substitution and band assignments, distinguishing it from monomeric NO absorptions. The N–N stretch, being a low-frequency mode, requires far-infrared detection and reflects the weak bonding in the dimer. Ultraviolet-visible spectroscopy of N₂O₂ shows weak absorption in the visible region, consistent with its overall colorless nature in pure form. However, in liquid nitric oxide, where dimers are present in equilibrium with monomers, charge-transfer bands from the N₂O₂ contribute to the observed pale blue tint. This subtle coloration arises from electronic transitions involving the dimer's weak N–N interaction, as confirmed by mass spectrometric and spectroscopic analyses of condensed-phase samples.[12]Synthesis
Dimerization of nitric oxide
Dinitrogen dioxide (N₂O₂) forms primarily through the reversible association of two nitric oxide (NO) molecules in the gas phase, according to the equilibrium reaction
This process is endergonic at room temperature but shifts toward the dimer upon cooling NO gas to temperatures below 150 K, where the exothermic nature of the association becomes dominant.[13]
Dimerization in the gas phase requires low temperatures (100–150 K) and moderate pressures (1–10 atm) to achieve measurable yields, as higher pressures favor the equilibrium due to the decrease in the number of moles; under these conditions, N₂O₂ constitutes only a small fraction (~1–3%) of the total gaseous species along the saturation curve.[13]
The existence of the NO dimer was first inferred in the 1920s from deviations in the measured vapor pressure of liquid and gaseous NO, which could not be explained by monomeric behavior alone.[14] Spectroscopic confirmation came in the 1950s through infrared studies that identified characteristic vibrational bands attributable to N₂O₂.[15]
The association mechanism involves a weak intermolecular bond between the nitrogen atoms of the two NO radicals, exhibiting van der Waals-like characteristics with partial covalent bonding due to overlap of their singly occupied π* orbitals, resulting in a relatively long N–N distance of approximately 1.75 Å in the cis isomer.[16]
