supplementary materials


Acta Cryst. (2009). E65, o497    [ doi:10.1107/S1600536809003675 ]

4-Chloro-2-[(E)-(4-nitrophenyl)diazenyl]phenol

L. A. Aslanov, K. A. Paseshnichenko and A. V. Yatsenko

Abstract top

The title compound, C12H8ClN3O3, in the crystalline state and in solution, exists in the azo form, as predicted by density functional theory (DFT) calculations. The molecule is approximately planar [the dihedral angle between the rings is 1.83 (8)°], with the nitro group slightly twisted [13.4 (2)°] relative to the benzene ring. Translationally related molecules form stacks along [010] with an interplanar distance of 3.400 (2) Å. The hydroxy group forms an intramolecular hydrogen bond with the azo N atom.

Comment top

The present work was fulfilled in the course of study of the hydroxyazo-ketohydrazone tautomerism in phenylazophenols. The title compound, (I), exists in crystals as the azo form (Fig. 1). It is evidenced, firstly, by the fact that the H atom was found and refined in the vicinity of O atom, and secondly, by comparison of the molecular geometry with numerous structures of azo tautomers found in the Cambridge Structural Database (Allen, 2002). Since the UV–visible spectra of the crystalline title compound resemble its spectra in solutions, the azo tautomer has to predominate in solutions as well.

However, recently it has been reported that (1Z)-4-hydroxybenzo-1,2-quinone 1-[(2-chloro-4-nitrophenyl)hydrazone (II), the compound closely related to (I), exists in crystals as the hydrazone tautomer (You et al., 2004).

The azo–hydrazone equilibrium is known to be shifted by the effect of donor and acceptor substituents and also by intra- and intermolecular hydrogen bonds. In order to evaluate the relative importance of these factors, we have performed the DFT calculations of azo and hydrazone tautomers of (I) and (II). Calculations were carried out using GAMESS (Schmidt et al., 1993) with B3LYP exchange-correlation functional (Becke, 1993; Lee et al., 1988) and 6-311G** basis set (Krishnan et al., 1980). After geometry of an isolated molecule has been optimized, molecular structure was fixed, and the effect of nonspecific intermolecular interactions was accounted by COSMO method (Klamt & Schüürmann, 1993), taking the dielectric permeability equal to 10. The results indicate that for 2-phenyldiazenylphenol (III), the azo form is by 10.5 kJ/mol more stable than the hydrazone form. For compound (I), this difference decreases to 7.5 kJ/mol and for (II) - to 6.8 kJ/mol, but nonetheless the azo form is still preferable.

Thus, the difference between (I) and (II) most probably arises from specific intermolecular interactions. In (I), there is the only worthnoting intermolecular contact C15—H15···O2 (-x, -1 - y, -z) (H15···O2 2.56 Å, C15···O2 3.452 (2) Å, C15—H15···O2 161°), which cannot have any effect on the relative stability of tautomers. In (II), the keto group forms a strong hydrogen bond with the hydroxy group of a neighboring molecule (O···H 1.74 Å, O···O 2.581 (2) Å, O—H···O 173°). This interaction stabilizes the hydrazone tautomer, according to the conception of resonance-assisted hydrogen bonds (Gilli et al., 1989). So, the shift of tautomeric equilibrium in (II) towards the hydrazone form should be most probably rationalized by formation of intermolecular hydrogen bonds.

Related literature top

For the crystal structure of a closely related molecule, (1Z)-4-hydroxybenzo-1,2-quinone-1-[(2-chloro-4-nitrophenyl)hydrazone, that crystallizes as a hydrazone tautomer, see: You et al., 2004). For reference structural data, see: Allen (2002). For details of the synthetic procedure, see: Fierz-David & Blangey (1949). For background on DFT calculations, see: Becke (1993); Klamt & Schüürmann (1993); Krishnan et al. (1980); Lee et al. (1988); Schmidt et al. (1993). For the concept of resonance-assisted hydrogen bonds, see: Gilli et al. (1989).

Experimental top

The title compound was prepared by coupling of p-nitrophenyldiazonium chloride with p-chlorphenol. For details of the synthetic procedure, see Fierz-David & Blangey (1949). Single crystals were grown by slow evaporation of ethanol solution.

Refinement top

H atoms were located in a difference map and refined freely, but at final stage they were positioned geometrically and refined using a riding model with C—H = 0.93 Å, O—H = 0.82 Å and with Uiso(H) = 1.2 times Ueq(C), Uiso(H) = 1.5 times Ueq(O)

Computing details top

Data collection: CAD-4 Software (Enraf–Nonius, 1989); cell refinement: CAD-4 Software (Enraf–Nonius, 1989); data reduction: PROFIT (Streltsov & Zavodnik, 1989) routine of WinGX (Farrugia, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with atomic labels and 50% probability displacement ellipsoids for non-H atoms.
[Figure 2] Fig. 2. Chemical diagrams of (II) and (III).
4-Chloro-2-[(E)-(4-nitrophenyl)diazenyl]phenol top
Crystal data top
C12H8ClN3O3F(000) = 568
Mr = 277.66Dx = 1.568 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 19.008 (5) Åθ = 16.8–18.8°
b = 4.817 (2) ŵ = 0.33 mm1
c = 12.862 (4) ÅT = 291 K
β = 92.65 (2)°Prism, red
V = 1176.4 (7) Å30.40 × 0.20 × 0.15 mm
Z = 4
Data collection top
Enraf–Nonius CAD-4
diffractometer
Rint = 0.0
Radiation source: fine-focus sealed tubeθmax = 27.0°, θmin = 1.1°
graphiteh = 2424
nonprofiled ω scansk = 06
2567 measured reflectionsl = 016
2567 independent reflections3 standard reflections every 90 min
2110 reflections with I > 2σ(I) intensity decay: 4%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.037Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.098H-atom parameters constrained
S = 1.56 w = 1/[σ2(Fo2) + (0.04P)2]
where P = (Fo2 + 2Fc2)/3
2567 reflections(Δ/σ)max = 0.001
173 parametersΔρmax = 0.25 e Å3
0 restraintsΔρmin = 0.14 e Å3
Crystal data top
C12H8ClN3O3V = 1176.4 (7) Å3
Mr = 277.66Z = 4
Monoclinic, P21/cMo Kα radiation
a = 19.008 (5) ŵ = 0.33 mm1
b = 4.817 (2) ÅT = 291 K
c = 12.862 (4) Å0.40 × 0.20 × 0.15 mm
β = 92.65 (2)°
Data collection top
Enraf–Nonius CAD-4
diffractometer
Rint = 0.0
2567 measured reflectionsθmax = 27.0°
2567 independent reflections3 standard reflections every 90 min
2110 reflections with I > 2σ(I) intensity decay: 4%
Refinement top
R[F2 > 2σ(F2)] = 0.037H-atom parameters constrained
wR(F2) = 0.098Δρmax = 0.25 e Å3
S = 1.56Δρmin = 0.14 e Å3
2567 reflectionsAbsolute structure: ?
173 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.463076 (19)1.28010 (9)0.16237 (3)0.06275 (16)
O10.27449 (6)0.7166 (3)0.14202 (8)0.0703 (4)
H10.24910.60450.11380.105*
O20.00077 (6)0.4250 (3)0.11633 (9)0.0665 (3)
O30.05796 (6)0.4261 (2)0.26393 (8)0.0592 (3)
N10.27334 (5)0.5696 (2)0.07974 (9)0.0436 (3)
N20.23136 (6)0.4462 (2)0.01583 (9)0.0450 (3)
N30.04760 (6)0.3453 (2)0.17452 (10)0.0468 (3)
C10.31710 (7)0.8384 (3)0.07021 (11)0.0496 (4)
C20.31686 (6)0.7693 (3)0.03656 (10)0.0420 (3)
C30.36225 (7)0.9076 (3)0.10740 (11)0.0444 (3)
H30.36200.86420.17780.053*
C40.40705 (7)1.1065 (3)0.07365 (12)0.0475 (3)
C50.40778 (8)1.1751 (3)0.03104 (12)0.0556 (4)
H50.43871.30970.05340.067*
C60.36281 (8)1.0440 (4)0.10150 (12)0.0589 (4)
H60.36291.09350.17140.071*
C110.18678 (6)0.2481 (3)0.06134 (10)0.0402 (3)
C120.18713 (7)0.1938 (3)0.16816 (11)0.0472 (3)
H120.21770.28840.21430.057*
C130.14144 (7)0.0020 (3)0.20368 (10)0.0473 (3)
H130.14120.04280.27430.057*
C140.09613 (6)0.1372 (3)0.13447 (10)0.0401 (3)
C150.09456 (7)0.0863 (3)0.02927 (10)0.0456 (3)
H150.06340.18010.01610.055*
C160.14084 (7)0.1087 (3)0.00691 (11)0.0469 (3)
H160.14110.14650.07780.056*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0544 (2)0.0552 (3)0.0784 (3)0.00993 (18)0.00095 (19)0.0052 (2)
O10.0844 (8)0.0812 (9)0.0452 (6)0.0262 (7)0.0024 (5)0.0036 (6)
O20.0716 (7)0.0648 (8)0.0636 (7)0.0297 (6)0.0068 (6)0.0067 (6)
O30.0716 (7)0.0500 (6)0.0570 (7)0.0031 (5)0.0129 (5)0.0118 (5)
N10.0437 (6)0.0373 (6)0.0502 (6)0.0005 (5)0.0071 (5)0.0018 (5)
N20.0460 (6)0.0406 (6)0.0486 (6)0.0002 (5)0.0054 (5)0.0021 (5)
N30.0548 (7)0.0348 (6)0.0518 (7)0.0001 (5)0.0128 (5)0.0031 (5)
C10.0523 (8)0.0494 (8)0.0477 (8)0.0001 (7)0.0095 (6)0.0004 (7)
C20.0418 (6)0.0367 (7)0.0482 (8)0.0030 (6)0.0092 (6)0.0027 (6)
C30.0452 (7)0.0382 (7)0.0502 (7)0.0040 (6)0.0072 (6)0.0035 (6)
C40.0432 (7)0.0373 (7)0.0626 (9)0.0023 (6)0.0067 (6)0.0042 (7)
C50.0551 (8)0.0473 (9)0.0663 (10)0.0056 (7)0.0214 (7)0.0042 (8)
C60.0663 (9)0.0596 (10)0.0522 (9)0.0060 (8)0.0176 (7)0.0075 (8)
C110.0402 (6)0.0351 (7)0.0456 (7)0.0033 (5)0.0055 (5)0.0018 (6)
C120.0478 (7)0.0485 (8)0.0451 (8)0.0054 (6)0.0000 (6)0.0017 (6)
C130.0537 (8)0.0501 (8)0.0384 (7)0.0021 (7)0.0041 (6)0.0024 (6)
C140.0419 (6)0.0296 (6)0.0492 (7)0.0025 (5)0.0081 (5)0.0005 (6)
C150.0505 (7)0.0426 (8)0.0432 (7)0.0058 (6)0.0015 (6)0.0025 (6)
C160.0540 (8)0.0472 (8)0.0395 (7)0.0023 (6)0.0030 (6)0.0053 (6)
Geometric parameters (Å, °) top
Cl1—C41.7387 (16)C4—C51.387 (2)
O1—C11.3358 (17)C5—C61.371 (2)
O1—H10.8200C5—H50.9300
O2—N31.2203 (15)C6—H60.9300
O3—N31.2214 (15)C11—C161.3831 (18)
N1—N21.2670 (16)C11—C121.3983 (19)
N1—C21.4001 (17)C12—C131.3743 (19)
N2—C111.4203 (17)C12—H120.9300
N3—C141.4712 (17)C13—C141.3741 (19)
C1—C61.389 (2)C13—H130.9300
C1—C21.413 (2)C14—C151.3741 (19)
C2—C31.3949 (19)C15—C161.3823 (19)
C3—C41.3660 (19)C15—H150.9300
C3—H30.9300C16—H160.9300
C1—O1—H1109.5C5—C6—C1121.06 (14)
N2—N1—C2115.52 (11)C5—C6—H6119.5
N1—N2—C11114.69 (11)C1—C6—H6119.5
O2—N3—O3124.14 (12)C16—C11—C12120.47 (12)
O2—N3—C14117.79 (12)C16—C11—N2115.84 (12)
O3—N3—C14118.06 (12)C12—C11—N2123.69 (12)
O1—C1—C6118.70 (13)C13—C12—C11118.72 (13)
O1—C1—C2122.63 (13)C13—C12—H12120.6
C6—C1—C2118.67 (14)C11—C12—H12120.6
C3—C2—N1115.33 (12)C14—C13—C12119.79 (12)
C3—C2—C1119.50 (13)C14—C13—H13120.1
N1—C2—C1125.17 (13)C12—C13—H13120.1
C4—C3—C2120.21 (13)C13—C14—C15122.53 (12)
C4—C3—H3119.9C13—C14—N3118.73 (12)
C2—C3—H3119.9C15—C14—N3118.75 (12)
C3—C4—C5120.66 (14)C14—C15—C16117.88 (12)
C3—C4—Cl1120.05 (12)C14—C15—H15121.1
C5—C4—Cl1119.29 (11)C16—C15—H15121.1
C6—C5—C4119.88 (14)C15—C16—C11120.61 (12)
C6—C5—H5120.1C15—C16—H16119.7
C4—C5—H5120.1C11—C16—H16119.7
C2—N1—N2—C11178.90 (10)N1—N2—C11—C16179.47 (11)
N2—N1—C2—C3179.08 (11)N1—N2—C11—C121.27 (18)
N2—N1—C2—C10.30 (19)C16—C11—C12—C130.5 (2)
O1—C1—C2—C3179.22 (13)N2—C11—C12—C13179.77 (12)
C6—C1—C2—C30.1 (2)C11—C12—C13—C140.7 (2)
O1—C1—C2—N10.1 (2)C12—C13—C14—C150.4 (2)
C6—C1—C2—N1179.24 (13)C12—C13—C14—N3179.82 (12)
N1—C2—C3—C4179.97 (11)O2—N3—C14—C13166.51 (12)
C1—C2—C3—C40.6 (2)O3—N3—C14—C1313.07 (17)
C2—C3—C4—C50.4 (2)O2—N3—C14—C1513.72 (18)
C2—C3—C4—Cl1179.53 (10)O3—N3—C14—C15166.71 (12)
C3—C4—C5—C60.5 (2)C13—C14—C15—C160.1 (2)
Cl1—C4—C5—C6178.60 (12)N3—C14—C15—C16179.63 (11)
C4—C5—C6—C11.3 (2)C14—C15—C16—C110.3 (2)
O1—C1—C6—C5179.81 (14)C12—C11—C16—C150.0 (2)
C2—C1—C6—C51.1 (2)N2—C11—C16—C15179.28 (12)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1···N20.821.882.5777 (17)143
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1···N20.821.882.5777 (17)143
Acknowledgements top

KAP and AVY thank the ICDD for financial assistance (grant No. 93-05).

references
References top

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