Abstract
In the title compound, C20H22N2O5, the central 1,3,4-oxadiazole ring is essentially planar [r.m.s. deviation from the best plane of 0.0011 Å] and makes dihedral angles of 4.10 (3) and 13.32 (4)° with the two benzene rings. In the crystal structure, the packing is stabilized by weak non-classical intermolecular C—H⋯N hydrogen bonds, which link the molecules into an extended network.
Related literature
For the optical and electronic properties of 1,3,4-oxadizole and its dericatives, see: Emi & Toru (2006 ▶). Liu et al. (1997 ▶); Peng et al. (2006 ▶); Satoshi et al. (2000 ▶). For reference geometrical data: see: Tian et al. (2009 ▶). For related structures, see: Orgzall et al. (2005 ▶).
Experimental
Crystal data
C20H22N2O5
M r = 370.40
Monoclinic,
a = 7.7264 (15) Å
b = 13.886 (3) Å
c = 16.911 (3) Å
β = 96.42 (3)°
V = 1803.0 (6) Å3
Z = 4
Mo Kα radiation
μ = 0.10 mm−1
T = 293 K
0.16 × 0.14 × 0.10 mm
Data collection
Rigaku Saturn diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.984, T max = 0.990
13017 measured reflections
4290 independent reflections
3635 reflections with I > 2σ(I)
R int = 0.030
Refinement
R[F 2 > 2σ(F 2)] = 0.040
wR(F 2) = 0.110
S = 1.04
4290 reflections
246 parameters
H-atom parameters constrained
Δρmax = 0.25 e Å−3
Δρmin = −0.23 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809028931/pv2184sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028931/pv2184Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C5—H5⋯N2i | 0.93 | 2.62 | 3.385 (2) | 140 |
Symmetry code: (i)
.
Acknowledgments
This work was supported by the Foundation of Hebei University of Science & Technology (No. XL200746).
supplementary crystallographic information
Comment
The optical and electronic properties of 1,3,4-oxadizole have received great attention in the field of electroluminescence (Emi et al., 2006). A well known derivative of 1,3,4-oxadiazole, 2-(4-biphenyl)-5-(tert-butylphenyl)-1,3,4-oxadiazole (PBD), has been used as electron-injection material to improve the balance of charge carrier and to increase the photon/electron quantum efficiency (Liu et al., 1997) and the electron-transporting material in organic electroluminescence device (Satoshi et al., 2000). It has been demonstrated that modifying the side chains or inserting other heterocycles in 1,3,4-oxadizole system could result in good electroluminescent molecules as organic electroluminescence materials (Peng et al., 2006). As part of an investigation on potential electroluminescent molecules by modifying the side chains of 2,5-diaryl-1,3,4-oxadizole, we reporte here the synthesis and structure of the title compound, (I).
The molecular structure of (I) is presented in Fig. 1. The oxadizole ring (O3/C10/N1/N2/C11) is essentially planar, with an r.m.s. deviation for fitted atoms of 0.0011 Å. It makes dihedral angles of, 13.32 (4) and 4.10 (3)°, respectively, with the benzene rings (C4—C9) and (C12—C17). The crystal packing is stabilized by weak non-classical intermolecular C—H···N hydrogen bonds which link the molecules into an infinite network. The bond lengths and angles in (I) are within their normal ranges (Tian et al. 2009). The crystal structure of a 2,5-diaryl-1,3,4-oxadiazole derivative have been reported (Orgzall et al., 2005).
Experimental
2,5-Di(o-hydroxyphenyl)-1,3,4-oxadiazole (0.8 g, 3.0 mmol), NaH (0.5 g, 20 mmol) and 1-chloro-2-methoxyethane (0.75 g, 8 mmol) were added and dissolved in 50 ml of THF, the mixture was stirred refluxing for 10 h. giving a colourless precipitate. The product was isolated, recrystallized from ethyl acetate then dried in a vacuum to give the pure compound in 81% yield. colourless single crystals of (I) suitable for X-ray analysis were obtained by slow evaporation of ethyl acetate solution at room temperature.
Refinement
The H atoms were included in calculated positions (C—H = 0.93–0.97 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) for aromatic and methylene H atoms and Uiso(H) = 1.5Ueq(methyl C).
Figures
Fig. 1.
The molecular structure of (I) with displacement ellipsoids for non-H atoms drawn at the 30% probability level.
Fig. 2.
Packing diagram for (I), with H bonds drawn as dashed lines; H-atom not involved in interactions have been excludeed
Crystal data
| C20H22N2O5 | F(000) = 784 |
| Mr = 370.40 | Dx = 1.364 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 4968 reflections |
| a = 7.7264 (15) Å | θ = 2.4–27.9° |
| b = 13.886 (3) Å | µ = 0.10 mm−1 |
| c = 16.911 (3) Å | T = 293 K |
| β = 96.42 (3)° | Prism, colourless |
| V = 1803.0 (6) Å3 | 0.16 × 0.14 × 0.10 mm |
| Z = 4 |
Data collection
| Rigaku Saturn diffractometer | 4290 independent reflections |
| Radiation source: rotating anode | 3635 reflections with I > 2σ(I) |
| confocal | Rint = 0.030 |
| ω scans | θmax = 27.9°, θmin = 2.4° |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | h = −9→10 |
| Tmin = 0.984, Tmax = 0.990 | k = −13→18 |
| 13017 measured reflections | l = −20→22 |
Refinement
| 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)] = 0.040 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.110 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0696P)2 + 0.0999P] where P = (Fo2 + 2Fc2)/3 |
| 4290 reflections | (Δ/σ)max < 0.001 |
| 246 parameters | Δρmax = 0.25 e Å−3 |
| 0 restraints | Δρmin = −0.23 e Å−3 |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| O1 | 0.88655 (10) | 0.03469 (6) | 0.35096 (5) | 0.0284 (2) | |
| O2 | 0.63462 (10) | 0.15549 (5) | 0.25616 (5) | 0.02362 (19) | |
| O3 | 0.35245 (9) | 0.06943 (5) | 0.04514 (4) | 0.01871 (17) | |
| O4 | 0.23221 (10) | 0.04689 (5) | −0.10258 (4) | 0.02263 (18) | |
| O5 | 0.18138 (11) | 0.24756 (6) | −0.15011 (6) | 0.0307 (2) | |
| N1 | 0.40253 (12) | 0.02963 (6) | 0.17243 (6) | 0.0230 (2) | |
| N2 | 0.30539 (12) | −0.04406 (6) | 0.13138 (6) | 0.0228 (2) | |
| C1 | 0.89595 (18) | −0.05579 (9) | 0.38968 (8) | 0.0337 (3) | |
| H1A | 0.9211 | −0.0464 | 0.4460 | 0.051* | |
| H1B | 0.9865 | −0.0937 | 0.3706 | 0.051* | |
| H1C | 0.7866 | −0.0886 | 0.3787 | 0.051* | |
| C2 | 0.76278 (15) | 0.09686 (9) | 0.38010 (7) | 0.0265 (3) | |
| H2A | 0.8027 | 0.1161 | 0.4342 | 0.032* | |
| H2B | 0.6524 | 0.0636 | 0.3804 | 0.032* | |
| C3 | 0.73965 (15) | 0.18388 (8) | 0.32781 (7) | 0.0245 (2) | |
| H3A | 0.6825 | 0.2348 | 0.3543 | 0.029* | |
| H3B | 0.8519 | 0.2073 | 0.3156 | 0.029* | |
| C4 | 0.60454 (14) | 0.22178 (7) | 0.19721 (7) | 0.0207 (2) | |
| C5 | 0.66365 (15) | 0.31641 (8) | 0.20354 (7) | 0.0251 (2) | |
| H5 | 0.7257 | 0.3378 | 0.2506 | 0.030* | |
| C6 | 0.62996 (15) | 0.37886 (8) | 0.13967 (8) | 0.0281 (3) | |
| H6 | 0.6681 | 0.4423 | 0.1445 | 0.034* | |
| C7 | 0.53997 (16) | 0.34777 (8) | 0.06861 (8) | 0.0280 (3) | |
| H7 | 0.5217 | 0.3894 | 0.0254 | 0.034* | |
| C8 | 0.47746 (15) | 0.25413 (8) | 0.06264 (7) | 0.0235 (2) | |
| H8 | 0.4158 | 0.2335 | 0.0153 | 0.028* | |
| C9 | 0.50575 (14) | 0.19043 (7) | 0.12671 (6) | 0.0197 (2) | |
| C10 | 0.42605 (13) | 0.09472 (7) | 0.11946 (6) | 0.0182 (2) | |
| C11 | 0.27775 (13) | −0.01706 (7) | 0.05765 (6) | 0.0176 (2) | |
| C12 | 0.17690 (13) | −0.06928 (7) | −0.00691 (6) | 0.0177 (2) | |
| C13 | 0.09329 (14) | −0.15339 (7) | 0.01298 (7) | 0.0219 (2) | |
| H13 | 0.1025 | −0.1731 | 0.0658 | 0.026* | |
| C14 | −0.00307 (15) | −0.20810 (8) | −0.04446 (7) | 0.0250 (2) | |
| H14 | −0.0577 | −0.2642 | −0.0304 | 0.030* | |
| C15 | −0.01745 (15) | −0.17859 (8) | −0.12307 (7) | 0.0245 (2) | |
| H15 | −0.0796 | −0.2161 | −0.1620 | 0.029* | |
| C16 | 0.05963 (14) | −0.09390 (8) | −0.14445 (7) | 0.0219 (2) | |
| H16 | 0.0471 | −0.0741 | −0.1973 | 0.026* | |
| C17 | 0.15615 (13) | −0.03817 (7) | −0.08668 (6) | 0.0185 (2) | |
| C18 | 0.20669 (15) | 0.08174 (8) | −0.18286 (6) | 0.0238 (2) | |
| H18A | 0.0833 | 0.0859 | −0.2010 | 0.029* | |
| H18B | 0.2607 | 0.0385 | −0.2179 | 0.029* | |
| C19 | 0.28879 (15) | 0.17939 (8) | −0.18332 (7) | 0.0248 (2) | |
| H19A | 0.4026 | 0.1780 | −0.1526 | 0.030* | |
| H19B | 0.3040 | 0.1977 | −0.2375 | 0.030* | |
| C20 | 0.25736 (17) | 0.34043 (8) | −0.14647 (9) | 0.0329 (3) | |
| H20A | 0.3644 | 0.3391 | −0.1117 | 0.049* | |
| H20B | 0.1787 | 0.3855 | −0.1265 | 0.049* | |
| H20C | 0.2805 | 0.3597 | −0.1988 | 0.049* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0249 (4) | 0.0240 (4) | 0.0367 (5) | 0.0018 (3) | 0.0058 (4) | 0.0001 (3) |
| O2 | 0.0248 (4) | 0.0227 (4) | 0.0218 (4) | −0.0033 (3) | −0.0042 (3) | −0.0033 (3) |
| O3 | 0.0215 (4) | 0.0161 (4) | 0.0181 (4) | −0.0008 (3) | 0.0002 (3) | −0.0014 (3) |
| O4 | 0.0308 (4) | 0.0193 (4) | 0.0175 (4) | −0.0038 (3) | 0.0014 (3) | 0.0012 (3) |
| O5 | 0.0235 (4) | 0.0208 (4) | 0.0497 (6) | 0.0002 (3) | 0.0120 (4) | 0.0026 (4) |
| N1 | 0.0257 (5) | 0.0205 (5) | 0.0215 (5) | −0.0025 (4) | −0.0034 (4) | −0.0006 (3) |
| N2 | 0.0259 (5) | 0.0198 (5) | 0.0216 (5) | −0.0030 (4) | −0.0028 (4) | 0.0002 (3) |
| C1 | 0.0361 (7) | 0.0287 (6) | 0.0355 (7) | 0.0017 (5) | −0.0001 (6) | 0.0022 (5) |
| C2 | 0.0234 (6) | 0.0327 (6) | 0.0227 (6) | 0.0019 (5) | −0.0003 (4) | −0.0062 (4) |
| C3 | 0.0203 (5) | 0.0274 (6) | 0.0243 (6) | 0.0003 (4) | −0.0035 (4) | −0.0091 (4) |
| C4 | 0.0174 (5) | 0.0205 (5) | 0.0248 (6) | 0.0020 (4) | 0.0043 (4) | −0.0037 (4) |
| C5 | 0.0204 (5) | 0.0236 (6) | 0.0314 (6) | −0.0018 (4) | 0.0031 (5) | −0.0082 (4) |
| C6 | 0.0266 (6) | 0.0173 (5) | 0.0413 (7) | −0.0023 (4) | 0.0079 (5) | −0.0040 (5) |
| C7 | 0.0300 (6) | 0.0213 (6) | 0.0335 (7) | 0.0003 (4) | 0.0070 (5) | 0.0028 (4) |
| C8 | 0.0247 (6) | 0.0208 (5) | 0.0252 (6) | 0.0008 (4) | 0.0033 (4) | −0.0009 (4) |
| C9 | 0.0172 (5) | 0.0186 (5) | 0.0234 (6) | 0.0012 (4) | 0.0030 (4) | −0.0029 (4) |
| C10 | 0.0166 (5) | 0.0197 (5) | 0.0178 (5) | 0.0022 (4) | −0.0001 (4) | −0.0025 (4) |
| C11 | 0.0169 (5) | 0.0141 (5) | 0.0218 (5) | 0.0019 (4) | 0.0025 (4) | 0.0000 (4) |
| C12 | 0.0168 (5) | 0.0156 (5) | 0.0205 (5) | 0.0032 (4) | 0.0013 (4) | −0.0026 (4) |
| C13 | 0.0221 (5) | 0.0191 (5) | 0.0242 (6) | 0.0020 (4) | 0.0013 (4) | 0.0016 (4) |
| C14 | 0.0238 (6) | 0.0181 (5) | 0.0328 (6) | −0.0025 (4) | 0.0015 (5) | −0.0006 (4) |
| C15 | 0.0212 (5) | 0.0218 (6) | 0.0295 (6) | 0.0004 (4) | −0.0022 (5) | −0.0075 (4) |
| C16 | 0.0221 (5) | 0.0235 (5) | 0.0199 (5) | 0.0036 (4) | 0.0010 (4) | −0.0039 (4) |
| C17 | 0.0180 (5) | 0.0167 (5) | 0.0212 (5) | 0.0024 (4) | 0.0038 (4) | −0.0015 (4) |
| C18 | 0.0278 (6) | 0.0263 (6) | 0.0170 (5) | 0.0018 (4) | 0.0008 (4) | 0.0022 (4) |
| C19 | 0.0227 (6) | 0.0262 (6) | 0.0260 (6) | 0.0028 (4) | 0.0051 (5) | 0.0057 (4) |
| C20 | 0.0271 (6) | 0.0227 (6) | 0.0492 (8) | −0.0015 (5) | 0.0058 (6) | 0.0042 (5) |
Geometric parameters (Å, °)
| O1—C1 | 1.4149 (15) | C6—H6 | 0.9300 |
| O1—C2 | 1.4171 (14) | C7—C8 | 1.3868 (16) |
| O2—C4 | 1.3577 (13) | C7—H7 | 0.9300 |
| O2—C3 | 1.4360 (13) | C8—C9 | 1.3969 (15) |
| O3—C11 | 1.3593 (12) | C8—H8 | 0.9300 |
| O3—C10 | 1.3663 (13) | C9—C10 | 1.4641 (15) |
| O4—C17 | 1.3594 (13) | C11—C12 | 1.4611 (14) |
| O4—C18 | 1.4341 (13) | C12—C13 | 1.3940 (15) |
| O5—C20 | 1.4154 (14) | C12—C17 | 1.4085 (15) |
| O5—C19 | 1.4158 (14) | C13—C14 | 1.3833 (15) |
| N1—C10 | 1.2996 (14) | C13—H13 | 0.9300 |
| N1—N2 | 1.4057 (13) | C14—C15 | 1.3837 (17) |
| N2—C11 | 1.2967 (14) | C14—H14 | 0.9300 |
| C1—H1A | 0.9600 | C15—C16 | 1.3845 (16) |
| C1—H1B | 0.9600 | C15—H15 | 0.9300 |
| C1—H1C | 0.9600 | C16—C17 | 1.3952 (15) |
| C2—C3 | 1.4963 (17) | C16—H16 | 0.9300 |
| C2—H2A | 0.9700 | C18—C19 | 1.4973 (16) |
| C2—H2B | 0.9700 | C18—H18A | 0.9700 |
| C3—H3A | 0.9700 | C18—H18B | 0.9700 |
| C3—H3B | 0.9700 | C19—H19A | 0.9700 |
| C4—C5 | 1.3913 (15) | C19—H19B | 0.9700 |
| C4—C9 | 1.4108 (15) | C20—H20A | 0.9600 |
| C5—C6 | 1.3870 (17) | C20—H20B | 0.9600 |
| C5—H5 | 0.9300 | C20—H20C | 0.9600 |
| C6—C7 | 1.3882 (18) | ||
| C1—O1—C2 | 112.44 (10) | N1—C10—O3 | 112.30 (9) |
| C4—O2—C3 | 117.88 (9) | N1—C10—C9 | 131.57 (10) |
| C11—O3—C10 | 102.96 (8) | O3—C10—C9 | 116.00 (9) |
| C17—O4—C18 | 117.63 (8) | N2—C11—O3 | 112.21 (9) |
| C20—O5—C19 | 111.58 (9) | N2—C11—C12 | 126.29 (9) |
| C10—N1—N2 | 105.90 (9) | O3—C11—C12 | 121.50 (9) |
| C11—N2—N1 | 106.62 (9) | C13—C12—C17 | 118.81 (10) |
| O1—C1—H1A | 109.5 | C13—C12—C11 | 117.27 (10) |
| O1—C1—H1B | 109.5 | C17—C12—C11 | 123.89 (9) |
| H1A—C1—H1B | 109.5 | C14—C13—C12 | 121.22 (11) |
| O1—C1—H1C | 109.5 | C14—C13—H13 | 119.4 |
| H1A—C1—H1C | 109.5 | C12—C13—H13 | 119.4 |
| H1B—C1—H1C | 109.5 | C13—C14—C15 | 119.41 (10) |
| O1—C2—C3 | 109.09 (10) | C13—C14—H14 | 120.3 |
| O1—C2—H2A | 109.9 | C15—C14—H14 | 120.3 |
| C3—C2—H2A | 109.9 | C14—C15—C16 | 120.79 (10) |
| O1—C2—H2B | 109.9 | C14—C15—H15 | 119.6 |
| C3—C2—H2B | 109.9 | C16—C15—H15 | 119.6 |
| H2A—C2—H2B | 108.3 | C15—C16—C17 | 120.01 (10) |
| O2—C3—C2 | 107.21 (9) | C15—C16—H16 | 120.0 |
| O2—C3—H3A | 110.3 | C17—C16—H16 | 120.0 |
| C2—C3—H3A | 110.3 | O4—C17—C16 | 123.53 (10) |
| O2—C3—H3B | 110.3 | O4—C17—C12 | 116.78 (9) |
| C2—C3—H3B | 110.3 | C16—C17—C12 | 119.69 (10) |
| H3A—C3—H3B | 108.5 | O4—C18—C19 | 107.28 (9) |
| O2—C4—C5 | 123.78 (10) | O4—C18—H18A | 110.3 |
| O2—C4—C9 | 116.32 (9) | C19—C18—H18A | 110.3 |
| C5—C4—C9 | 119.90 (10) | O4—C18—H18B | 110.3 |
| C6—C5—C4 | 119.94 (11) | C19—C18—H18B | 110.3 |
| C6—C5—H5 | 120.0 | H18A—C18—H18B | 108.5 |
| C4—C5—H5 | 120.0 | O5—C19—C18 | 109.63 (9) |
| C5—C6—C7 | 120.79 (11) | O5—C19—H19A | 109.7 |
| C5—C6—H6 | 119.6 | C18—C19—H19A | 109.7 |
| C7—C6—H6 | 119.6 | O5—C19—H19B | 109.7 |
| C8—C7—C6 | 119.43 (11) | C18—C19—H19B | 109.7 |
| C8—C7—H7 | 120.3 | H19A—C19—H19B | 108.2 |
| C6—C7—H7 | 120.3 | O5—C20—H20A | 109.5 |
| C7—C8—C9 | 120.94 (11) | O5—C20—H20B | 109.5 |
| C7—C8—H8 | 119.5 | H20A—C20—H20B | 109.5 |
| C9—C8—H8 | 119.5 | O5—C20—H20C | 109.5 |
| C8—C9—C4 | 118.89 (10) | H20A—C20—H20C | 109.5 |
| C8—C9—C10 | 118.81 (10) | H20B—C20—H20C | 109.5 |
| C4—C9—C10 | 122.26 (10) | ||
| C10—N1—N2—C11 | −0.40 (12) | N1—N2—C11—O3 | 1.21 (12) |
| C1—O1—C2—C3 | −170.86 (10) | N1—N2—C11—C12 | −177.78 (9) |
| C4—O2—C3—C2 | −176.18 (9) | C10—O3—C11—N2 | −1.48 (11) |
| O1—C2—C3—O2 | 76.04 (11) | C10—O3—C11—C12 | 177.56 (9) |
| C3—O2—C4—C5 | −2.69 (15) | N2—C11—C12—C13 | 4.11 (16) |
| C3—O2—C4—C9 | 177.96 (9) | O3—C11—C12—C13 | −174.79 (9) |
| O2—C4—C5—C6 | 178.67 (10) | N2—C11—C12—C17 | −177.65 (10) |
| C9—C4—C5—C6 | −2.00 (17) | O3—C11—C12—C17 | 3.44 (16) |
| C4—C5—C6—C7 | −1.03 (18) | C17—C12—C13—C14 | 2.55 (16) |
| C5—C6—C7—C8 | 2.46 (18) | C11—C12—C13—C14 | −179.12 (10) |
| C6—C7—C8—C9 | −0.83 (18) | C12—C13—C14—C15 | −0.30 (17) |
| C7—C8—C9—C4 | −2.15 (17) | C13—C14—C15—C16 | −1.66 (17) |
| C7—C8—C9—C10 | 175.47 (10) | C14—C15—C16—C17 | 1.30 (17) |
| O2—C4—C9—C8 | −177.06 (9) | C18—O4—C17—C16 | 1.85 (15) |
| C5—C4—C9—C8 | 3.56 (16) | C18—O4—C17—C12 | −177.53 (9) |
| O2—C4—C9—C10 | 5.40 (15) | C15—C16—C17—O4 | −178.37 (10) |
| C5—C4—C9—C10 | −173.98 (10) | C15—C16—C17—C12 | 0.99 (16) |
| N2—N1—C10—O3 | −0.54 (12) | C13—C12—C17—O4 | 176.54 (9) |
| N2—N1—C10—C9 | 174.94 (10) | C11—C12—C17—O4 | −1.68 (15) |
| C11—O3—C10—N1 | 1.22 (11) | C13—C12—C17—C16 | −2.87 (15) |
| C11—O3—C10—C9 | −175.03 (9) | C11—C12—C17—C16 | 178.92 (9) |
| C8—C9—C10—N1 | −165.11 (11) | C17—O4—C18—C19 | 175.03 (9) |
| C4—C9—C10—N1 | 12.43 (18) | C20—O5—C19—C18 | 177.69 (10) |
| C8—C9—C10—O3 | 10.25 (14) | O4—C18—C19—O5 | −75.52 (11) |
| C4—C9—C10—O3 | −172.21 (9) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C5—H5···N2i | 0.93 | 2.62 | 3.385 (2) | 140 |
Symmetry codes: (i) −x+1, y+1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2184).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809028931/pv2184sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028931/pv2184Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


