Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807058163/ci2513sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807058163/ci2513Isup2.hkl |
CCDC reference: 672962
The title compound was prepared as described by Özcan and Mirzaoğlu (1988), using p-toluidine and anti-chloroglyoxime as starting materials in absolute ethanol at 263 K (white precipate; yield 45%; m.p. 445 K). Colourless crystals of the title compound suitable for X-ray crystallographic analysis were obtained by slow evaporation of a DMF solution at room temperature.
Atoms H1A and H22 were located in a difference map and refined isotropically. The remaining H atoms were positioned geometrically [N—H = 0.86 Å and C—H = 0.93 Å (aromatic) or 0.96 Å (methyl)] and constrained to ride on their parent atom, with Uiso(H) = xUeq(C), where x = 1.5 for methyl H, and x = 1.2 for other H atoms. 942 Friedel pairs were averaged before the final refinement as the absolute structure could not be determined unambiguously.
Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
C9H11N3O2 | F(000) = 408 |
Mr = 193.21 | Dx = 1.315 Mg m−3 |
Monoclinic, Cc | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: C -2yc | Cell parameters from 24450 reflections |
a = 9.0031 (12) Å | θ = 3.0–27.3° |
b = 19.352 (3) Å | µ = 0.10 mm−1 |
c = 6.9742 (9) Å | T = 296 K |
β = 126.596 (9)° | Prism, pale yellow |
V = 975.6 (3) Å3 | 0.69 × 0.36 × 0.14 mm |
Z = 4 |
STOE IPDS II diffractometer | 1072 independent reflections |
Radiation source: fine-focus sealed tube | 1024 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.060 |
Detector resolution: 6.67 pixels mm-1 | θmax = 27.0°, θmin = 3.0° |
ω scan | h = −11→11 |
Absorption correction: integration (X-RED32; Stoe & Cie, 2002) | k = −24→24 |
Tmin = 0.947, Tmax = 0.987 | l = −8→8 |
9760 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.032 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.082 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.12 | w = 1/[σ2(Fo2) + (0.0457P)2 + 0.1463P] where P = (Fo2 + 2Fc2)/3 |
1072 reflections | (Δ/σ)max = 0.001 |
136 parameters | Δρmax = 0.13 e Å−3 |
3 restraints | Δρmin = −0.14 e Å−3 |
C9H11N3O2 | V = 975.6 (3) Å3 |
Mr = 193.21 | Z = 4 |
Monoclinic, Cc | Mo Kα radiation |
a = 9.0031 (12) Å | µ = 0.10 mm−1 |
b = 19.352 (3) Å | T = 296 K |
c = 6.9742 (9) Å | 0.69 × 0.36 × 0.14 mm |
β = 126.596 (9)° |
STOE IPDS II diffractometer | 1072 independent reflections |
Absorption correction: integration (X-RED32; Stoe & Cie, 2002) | 1024 reflections with I > 2σ(I) |
Tmin = 0.947, Tmax = 0.987 | Rint = 0.060 |
9760 measured reflections |
R[F2 > 2σ(F2)] = 0.032 | 3 restraints |
wR(F2) = 0.082 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.12 | Δρmax = 0.13 e Å−3 |
1072 reflections | Δρmin = −0.14 e Å−3 |
136 parameters |
Experimental. 484 frames, detector distance = 70 mm |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.5005 (3) | 0.26817 (10) | 0.3450 (4) | 0.0396 (4) | |
C2 | 0.4256 (3) | 0.33277 (12) | 0.3234 (4) | 0.0471 (5) | |
H2 | 0.3711 | 0.3418 | 0.3997 | 0.057* | |
C3 | 0.4312 (4) | 0.38366 (12) | 0.1898 (5) | 0.0569 (6) | |
H3 | 0.3815 | 0.4269 | 0.1790 | 0.068* | |
C4 | 0.5096 (4) | 0.37194 (13) | 0.0704 (4) | 0.0539 (6) | |
C5 | 0.5878 (3) | 0.30800 (13) | 0.0987 (4) | 0.0513 (5) | |
H5 | 0.6433 | 0.2991 | 0.0237 | 0.062* | |
C6 | 0.5859 (3) | 0.25656 (11) | 0.2356 (4) | 0.0439 (5) | |
H6 | 0.6420 | 0.2142 | 0.2541 | 0.053* | |
C7 | 0.5105 (5) | 0.42754 (17) | −0.0808 (6) | 0.0820 (10) | |
H7A | 0.4318 | 0.4649 | −0.1019 | 0.123* | |
H7B | 0.4658 | 0.4087 | −0.2339 | 0.123* | |
H7C | 0.6343 | 0.4443 | −0.0028 | 0.123* | |
C8 | 0.4705 (3) | 0.14747 (10) | 0.4385 (3) | 0.0373 (4) | |
C9 | 0.4235 (3) | 0.11959 (10) | 0.2112 (3) | 0.0375 (4) | |
H9 | 0.3545 | 0.1452 | 0.0708 | 0.045* | |
N1 | 0.4869 (3) | 0.21670 (9) | 0.4769 (3) | 0.0441 (4) | |
H1 | 0.4893 | 0.2308 | 0.5957 | 0.053* | |
N2 | 0.4806 (3) | 0.05983 (9) | 0.2152 (3) | 0.0422 (4) | |
N3 | 0.4826 (3) | 0.10245 (9) | 0.5830 (3) | 0.0443 (4) | |
O1 | 0.4217 (3) | 0.03900 (8) | −0.0112 (3) | 0.0513 (4) | |
O2 | 0.5278 (3) | 0.13481 (9) | 0.7934 (3) | 0.0566 (5) | |
H1A | 0.456 (4) | −0.0057 (18) | 0.009 (5) | 0.060 (9)* | |
H2A | 0.497 (5) | 0.1034 (19) | 0.860 (6) | 0.073 (10)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0436 (11) | 0.0315 (10) | 0.0392 (10) | −0.0042 (8) | 0.0223 (9) | −0.0034 (8) |
C2 | 0.0519 (12) | 0.0341 (10) | 0.0535 (12) | −0.0017 (8) | 0.0304 (10) | −0.0061 (8) |
C3 | 0.0571 (14) | 0.0312 (9) | 0.0616 (14) | 0.0013 (9) | 0.0242 (11) | 0.0012 (10) |
C4 | 0.0532 (13) | 0.0446 (12) | 0.0486 (12) | −0.0101 (10) | 0.0221 (11) | 0.0064 (10) |
C5 | 0.0555 (13) | 0.0494 (13) | 0.0501 (12) | −0.0124 (10) | 0.0321 (10) | −0.0033 (10) |
C6 | 0.0503 (12) | 0.0334 (10) | 0.0508 (11) | −0.0016 (9) | 0.0317 (10) | −0.0016 (8) |
C7 | 0.092 (2) | 0.0601 (17) | 0.073 (2) | −0.0113 (16) | 0.0385 (18) | 0.0197 (15) |
C8 | 0.0459 (11) | 0.0324 (10) | 0.0405 (10) | −0.0025 (8) | 0.0295 (9) | −0.0027 (8) |
C9 | 0.0498 (11) | 0.0299 (9) | 0.0367 (9) | −0.0009 (8) | 0.0279 (8) | 0.0018 (7) |
N1 | 0.0645 (11) | 0.0340 (9) | 0.0464 (9) | −0.0022 (8) | 0.0398 (9) | −0.0049 (7) |
N2 | 0.0653 (11) | 0.0339 (8) | 0.0386 (8) | 0.0003 (8) | 0.0371 (8) | −0.0001 (7) |
N3 | 0.0639 (11) | 0.0395 (9) | 0.0427 (9) | −0.0055 (8) | 0.0390 (8) | −0.0043 (7) |
O1 | 0.0877 (13) | 0.0352 (8) | 0.0436 (8) | 0.0018 (8) | 0.0459 (9) | −0.0020 (6) |
O2 | 0.0891 (14) | 0.0523 (10) | 0.0487 (9) | −0.0105 (9) | 0.0521 (10) | −0.0087 (7) |
C1—C2 | 1.386 (3) | C7—H7B | 0.96 |
C1—C6 | 1.387 (3) | C7—H7C | 0.96 |
C1—N1 | 1.410 (3) | C8—N3 | 1.287 (3) |
C2—C3 | 1.377 (4) | C8—N1 | 1.357 (3) |
C2—H2 | 0.93 | C8—C9 | 1.478 (3) |
C3—C4 | 1.394 (4) | C9—N2 | 1.259 (3) |
C3—H3 | 0.93 | C9—H9 | 0.93 |
C4—C5 | 1.378 (4) | N1—H1 | 0.86 |
C4—C7 | 1.510 (4) | N2—O1 | 1.392 (2) |
C5—C6 | 1.387 (3) | N3—O2 | 1.414 (2) |
C5—H5 | 0.93 | O1—H1A | 0.90 (3) |
C6—H6 | 0.93 | O2—H2A | 0.90 (4) |
C7—H7A | 0.96 | ||
C2—C1—C6 | 118.7 (2) | C4—C7—H7B | 109.5 |
C2—C1—N1 | 118.84 (19) | H7A—C7—H7B | 109.5 |
C6—C1—N1 | 122.47 (18) | C4—C7—H7C | 109.5 |
C3—C2—C1 | 120.4 (2) | H7A—C7—H7C | 109.5 |
C3—C2—H2 | 119.8 | H7B—C7—H7C | 109.5 |
C1—C2—H2 | 119.8 | N3—C8—N1 | 124.44 (19) |
C2—C3—C4 | 121.6 (2) | N3—C8—C9 | 115.44 (18) |
C2—C3—H3 | 119.2 | N1—C8—C9 | 120.00 (18) |
C4—C3—H3 | 119.2 | N2—C9—C8 | 117.38 (17) |
C5—C4—C3 | 117.2 (2) | N2—C9—H9 | 121.3 |
C5—C4—C7 | 121.7 (3) | C8—C9—H9 | 121.3 |
C3—C4—C7 | 121.1 (3) | C8—N1—C1 | 127.63 (18) |
C4—C5—C6 | 121.9 (2) | C8—N1—H1 | 116.2 |
C4—C5—H5 | 119.1 | C1—N1—H1 | 116.2 |
C6—C5—H5 | 119.1 | C9—N2—O1 | 111.50 (16) |
C5—C6—C1 | 120.1 (2) | C8—N3—O2 | 110.52 (17) |
C5—C6—H6 | 120.0 | N2—O1—H1A | 104 (2) |
C1—C6—H6 | 120.0 | N3—O2—H2A | 104 (2) |
C4—C7—H7A | 109.5 | ||
C6—C1—C2—C3 | 1.9 (3) | N3—C8—C9—N2 | −32.1 (3) |
N1—C1—C2—C3 | −178.0 (2) | N1—C8—C9—N2 | 151.7 (2) |
C1—C2—C3—C4 | 0.8 (4) | N3—C8—N1—C1 | 170.6 (2) |
C2—C3—C4—C5 | −2.4 (4) | C9—C8—N1—C1 | −13.6 (4) |
C2—C3—C4—C7 | 178.4 (2) | C2—C1—N1—C8 | 147.7 (2) |
C3—C4—C5—C6 | 1.3 (4) | C6—C1—N1—C8 | −32.2 (3) |
C7—C4—C5—C6 | −179.4 (2) | C8—C9—N2—O1 | 177.96 (19) |
C4—C5—C6—C1 | 1.3 (3) | N1—C8—N3—O2 | −4.0 (3) |
C2—C1—C6—C5 | −2.9 (3) | C9—C8—N3—O2 | −179.96 (19) |
N1—C1—C6—C5 | 177.0 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1A···N3i | 0.90 (3) | 1.92 (3) | 2.792 (2) | 162 (3) |
O1—H1A···N2i | 0.90 (3) | 2.43 (3) | 2.965 (2) | 119 (2) |
O2—H2A···O1ii | 0.90 (4) | 1.88 (4) | 2.786 (2) | 177 (3) |
Symmetry codes: (i) x, −y, z−1/2; (ii) x, y, z+1. |
Experimental details
Crystal data | |
Chemical formula | C9H11N3O2 |
Mr | 193.21 |
Crystal system, space group | Monoclinic, Cc |
Temperature (K) | 296 |
a, b, c (Å) | 9.0031 (12), 19.352 (3), 6.9742 (9) |
β (°) | 126.596 (9) |
V (Å3) | 975.6 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.10 |
Crystal size (mm) | 0.69 × 0.36 × 0.14 |
Data collection | |
Diffractometer | STOE IPDS II diffractometer |
Absorption correction | Integration (X-RED32; Stoe & Cie, 2002) |
Tmin, Tmax | 0.947, 0.987 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 9760, 1072, 1024 |
Rint | 0.060 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.032, 0.082, 1.12 |
No. of reflections | 1072 |
No. of parameters | 136 |
No. of restraints | 3 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.13, −0.14 |
Computer programs: X-AREA (Stoe & Cie, 2002), X-AREA, X-RED32 (Stoe & Cie, 2002), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), WinGX (Farrugia, 1999).
N2—O1 | 1.392 (2) | N3—O2 | 1.414 (2) |
C9—N2—O1 | 111.50 (16) | C8—N3—O2 | 110.52 (17) |
C8—C9—N2—O1 | 177.96 (19) | C9—C8—N3—O2 | −179.96 (19) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1A···N3i | 0.90 (3) | 1.92 (3) | 2.792 (2) | 162 (3) |
O1—H1A···N2i | 0.90 (3) | 2.43 (3) | 2.965 (2) | 119 (2) |
O2—H2A···O1ii | 0.90 (4) | 1.88 (4) | 2.786 (2) | 177 (3) |
Symmetry codes: (i) x, −y, z−1/2; (ii) x, y, z+1. |
Intermolecular hydrogen bonding combines moderate strength and directionally (Karle et al., 1996) in linking molecules to form supramolecular structures; this has received considerable attention with respect to directional non-covalent intermolecular interactions (Etter et al., 1990). The oxime (–C=N—OH) moiety is potentially ambidentate, with possibilities of coordination through the N and/or O atoms. It is a functional group that has not been extensively explored in crystal engineering. In the solid state, oximes are usually associated via O—H···N hydrogen bonds of length 2.8 Å. Oxime groups posses stronger hydrogen-bonding capabilities than alcohols, phenols and carboxylic acids (Marsman et al., 1999). The hydrogen-bond systems in the crystals of oximes have been analysed and a correlation between a pattern of hydrogen bonding and N—O bond lengths has been suggested (Bertolasi et al., 1982). The configurational and/or conformational isomers of glyoxime derivatives (dioximes) have also been analysed (Chertanova et al., 1994).
The crystal structures of oxime and dioxime derivatives, viz. 2,3-dimethylquinoxaline-dimethylglyoxime (1/1) (Hökelek, Batı et al., 2001), 1-(2,6-dimethylphenlamino)propane-1,2-dione dioxime (Hökelek, Zülfikaroğlu et al., 2001) and N-hydroxy-2-oxo-2,N\'-diphenylacetamidine (Büyükgüngör et al., 2003) have been reported. The structure determination of the title compound (Fig.1) was carried out in order to investigate the strength of the hydrogen bonding capability of the oxime group.
The dihedral angles between the glyoxime planes A (O2/N3/C8), B (O1/N2/C9) and benzene ring C (C1—C6) are A/B= 33.0 (2)°, A/C=42.1 (2)° and B/C=45.1 (2)°. In the glyoxime moiety, the O2—N3 [1.414 (2) Å] bond length is longer than O1—N2 [1.392 (2) Å], while the O1—N2—C9 [111.5 (2)°] bond angle is larger than O2—N3—C8 [110.5 (2)°], reflecting the types and electron-withdrawing or -donating properties of the substituents bonded to C atoms of the glyoxime moiety.
The glyoxime moiety has an E configuration [C9—C8—N3—O2 = -180.0 (2)° and C8—C9—N2—O1 = 178.0 (2)°] (Chertanova et al., 1994). In this configuration, both oxime groups are involved as donors in intermolecular hydrogen bonds (Table 2).
In the crystal structure, the molecules are linked into a ribbon-like structure (Fig. 2) along the c axis by intermolecular O—H···N and O—H···O hydrogen bonds (Fig. 2).