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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jul 29;65(Pt 8):o2010. doi: 10.1107/S1600536809028931

2,5-Bis[2-(2-methoxy­ethoxy)phen­yl]-1,3,4-oxadiazole

Xia Tian a, Xiao-Li Zhen a, Jian-Rong Han a,*, Chang-Xin Ming a, Shou-Xin Liu b,
PMCID: PMC2977367  PMID: 21583681

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).graphic file with name e-65-o2010-scheme1.jpg

Experimental

Crystal data

  • C20H22N2O5

  • M r = 370.40

  • Monoclinic, Inline graphic

  • 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

e-65-o2010-sup1.cif (21.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028931/pv2184Isup2.hkl

e-65-o2010-Isup2.hkl (210.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C5—H5⋯N2i 0.93 2.62 3.385 (2) 140

Symmetry code: (i) Inline graphic.

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.

Fig. 1.

The molecular structure of (I) with displacement ellipsoids for non-H atoms drawn at the 30% probability level.

Fig. 2.

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 m3
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 mm1
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 Å3
0 restraints Δρmin = −0.23 e Å3

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

e-65-o2010-sup1.cif (21.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028931/pv2184Isup2.hkl

e-65-o2010-Isup2.hkl (210.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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