Abstract
In the title compound, C14H8Cl2N2O, the dihedral angles between the plane of the oxadiazole ring and those of the benzene rings are 2.3 (1) and 9.5 (1)°. In the crystal, molecules are linked into chains along the c axis by C—H⋯Cl interactions. These chains are stacked along the a axis.
Related literature
For the biological properties of heterocyclic compounds including oxadiazoles, see: Andersen et al. (1994 ▶); Showell et al. (1991 ▶); Watjen et al. (1989 ▶); Swain et al. (1991 ▶); Clitherow et al. (1996 ▶). For their pharmacological and medicinal activity, see: Isloor et al. (2010 ▶); Chandrakantha et al. (2010 ▶). For a related structure, see: Wang et al. (2006 ▶). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986 ▶).
Experimental
Crystal data
C14H8Cl2N2O
M r = 291.12
Triclinic,
a = 3.8035 (2) Å
b = 10.9666 (7) Å
c = 14.6949 (9) Å
α = 99.044 (2)°
β = 91.158 (2)°
γ = 98.891 (2)°
V = 597.43 (6) Å3
Z = 2
Mo Kα radiation
μ = 0.53 mm−1
T = 100 K
0.41 × 0.13 × 0.09 mm
Data collection
Bruker SMART APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2005 ▶) T min = 0.809, T max = 0.953
12084 measured reflections
2692 independent reflections
2355 reflections with I > 2σ(I)
R int = 0.035
Refinement
R[F 2 > 2σ(F 2)] = 0.035
wR(F 2) = 0.121
S = 1.14
2692 reflections
204 parameters
All H-atom parameters refined
Δρmax = 0.55 e Å−3
Δρmin = −0.39 e Å−3
Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681000927X/sj2743sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053681000927X/sj2743Isup2.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 |
---|---|---|---|---|
C3—H3A⋯Cl1i | 0.95 (3) | 2.81 (3) | 3.577 (2) | 138.6 (19) |
Symmetry code: (i) .
Acknowledgments
AMI is grateful to Professor Sandeep Sancheti, Director, National Institute of Technology-Karnataka, India for his encouragement and providing research facilities. FHK and MMR thank Universiti Sains Malaysia for the Research University Golden Goose grant (No. 1001/PFIZIK/811012).
supplementary crystallographic information
Comment
Heterocyclic compounds are becoming increasingly important in recent years due to their pharmacological activities (Isloor et al. 2010). Nitrogen- and oxygen-containing five/six membered heterocyclic compounds are of enormous significance in the field of medicinal chemistry (Chandrakantha et al., 2010). Oxadiazoles play a very vital role in the preparation of various biologically active drugs with anti-inflammatory (Andersen et al., 1994), anti-cancer (Showell et al., 1991), anti-HIV (Watjen et al., 1989), anti-diabetic and anti-microbial (Swain et al., 1991) activities. The results of biological studies showed that oxadiazole derivatives also possess maximum anti-inflammatory, analgesic and minimum ulcerogenic and lipid per-oxidation (Clitherow et al., 1996) properties.
The geometrical parameters of (I) are within the normal range and comparable with those for a related structure (Wang et al., 2006). The mean plane of of the oxadiazole ring (C7/C8/N1/N2/O1) is almost coplanar with the C9-C14 benzene ring [dihedral angle = 2.3 (1)°] but slightly twisted with the C1-C6 benzene ring [dihedral angle = 9.5 (1)°].
The C-H···Cl (Table 1) interactions link the molecules into infinite chains along the c-axis and these chains are stacked along the a-axis.
Experimental
The title compound was prepared by heating a solution of 2,4-dichloro- N'-hydroxy-benzamidine (1 g,0.0042 mol) and benzoylchloride (0.65 g.0.004 mol) in pyridine (30 ml). The reaction mixture was heated at 114 °C for 1.5 hour and concentrated under vacuum. Further purification was done by column chromatography. The solid obtained was recrystalised using dichloromethane.Yield: 1 g (76%), Melting point 413-415 K.
Refinement
All H atoms were located in a difference Fourier map and refined freely.
Figures
Fig. 1.
The molecular structure of (I), showing 50% probability displacement ellipsoids and the atom-numbering scheme.
Fig. 2.
The crystal structure of (I), showing infinite chains along the c-axis.
Crystal data
C14H8Cl2N2O | Z = 2 |
Mr = 291.12 | F(000) = 296 |
Triclinic, P1 | Dx = 1.618 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 3.8035 (2) Å | Cell parameters from 7625 reflections |
b = 10.9666 (7) Å | θ = 2.5–36.0° |
c = 14.6949 (9) Å | µ = 0.53 mm−1 |
α = 99.044 (2)° | T = 100 K |
β = 91.158 (2)° | Block, colourless |
γ = 98.891 (2)° | 0.41 × 0.13 × 0.09 mm |
V = 597.43 (6) Å3 |
Data collection
Bruker SMART APEXII CCD area-detector diffractometer | 2692 independent reflections |
Radiation source: fine-focus sealed tube | 2355 reflections with I > 2σ(I) |
graphite | Rint = 0.035 |
φ and ω scans | θmax = 27.5°, θmin = 1.4° |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | h = −4→4 |
Tmin = 0.809, Tmax = 0.953 | k = −14→14 |
12084 measured reflections | l = −19→19 |
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)] = 0.035 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.121 | All H-atom parameters refined |
S = 1.14 | w = 1/[σ2(Fo2) + (0.0727P)2 + 0.3227P] where P = (Fo2 + 2Fc2)/3 |
2692 reflections | (Δ/σ)max = 0.001 |
204 parameters | Δρmax = 0.55 e Å−3 |
0 restraints | Δρmin = −0.39 e Å−3 |
Special details
Experimental. The crystal was placed in the cold stream of an Oxford Cyrosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K. |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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 | ||
Cl1 | 0.67894 (14) | 0.17290 (4) | 0.56305 (3) | 0.02303 (17) | |
Cl2 | 0.74585 (13) | 0.52050 (4) | 0.34575 (3) | 0.01905 (16) | |
O1 | 1.0808 (4) | 0.40239 (12) | 0.07273 (9) | 0.0188 (3) | |
N1 | 1.1293 (4) | 0.22993 (14) | 0.12866 (10) | 0.0152 (3) | |
N2 | 0.9704 (5) | 0.42193 (15) | 0.16440 (11) | 0.0186 (3) | |
C1 | 1.3840 (5) | 0.31992 (18) | −0.09742 (13) | 0.0182 (4) | |
C2 | 1.5167 (6) | 0.27272 (19) | −0.18064 (13) | 0.0207 (4) | |
C3 | 1.5623 (5) | 0.14861 (19) | −0.19917 (13) | 0.0197 (4) | |
C4 | 1.4763 (5) | 0.06975 (18) | −0.13435 (12) | 0.0180 (4) | |
C5 | 1.3476 (5) | 0.11647 (17) | −0.05099 (12) | 0.0157 (4) | |
C6 | 1.3013 (5) | 0.24188 (17) | −0.03204 (12) | 0.0146 (4) | |
C7 | 1.1707 (5) | 0.28734 (17) | 0.05746 (12) | 0.0152 (4) | |
C8 | 1.0052 (5) | 0.31698 (17) | 0.19311 (12) | 0.0141 (4) | |
C9 | 0.9255 (5) | 0.28872 (16) | 0.28577 (12) | 0.0146 (4) | |
C10 | 0.9670 (5) | 0.16979 (17) | 0.30360 (12) | 0.0155 (4) | |
C11 | 0.8962 (5) | 0.13252 (18) | 0.38802 (13) | 0.0172 (4) | |
C12 | 0.7795 (5) | 0.21663 (18) | 0.45703 (12) | 0.0171 (4) | |
C13 | 0.7382 (5) | 0.33600 (18) | 0.44337 (12) | 0.0172 (4) | |
C14 | 0.8094 (5) | 0.37087 (16) | 0.35794 (12) | 0.0155 (4) | |
H1A | 1.360 (7) | 0.402 (3) | −0.0859 (17) | 0.026 (6)* | |
H2A | 1.572 (7) | 0.323 (2) | −0.2233 (18) | 0.024 (6)* | |
H3A | 1.664 (7) | 0.121 (2) | −0.2558 (18) | 0.029 (7)* | |
H4A | 1.483 (6) | −0.015 (2) | −0.1458 (15) | 0.015 (5)* | |
H5A | 1.325 (7) | 0.068 (2) | −0.0091 (17) | 0.020 (6)* | |
H10A | 1.028 (7) | 0.109 (2) | 0.2564 (16) | 0.019 (6)* | |
H11A | 0.922 (6) | 0.054 (2) | 0.3967 (15) | 0.014 (5)* | |
H13A | 0.635 (7) | 0.390 (2) | 0.4924 (17) | 0.022 (6)* |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0276 (3) | 0.0272 (3) | 0.0163 (2) | 0.0063 (2) | 0.00286 (18) | 0.00754 (18) |
Cl2 | 0.0228 (3) | 0.0169 (2) | 0.0191 (2) | 0.00957 (18) | −0.00111 (17) | 0.00205 (17) |
O1 | 0.0261 (8) | 0.0160 (6) | 0.0165 (6) | 0.0086 (5) | 0.0003 (5) | 0.0045 (5) |
N1 | 0.0149 (8) | 0.0165 (7) | 0.0148 (7) | 0.0051 (6) | −0.0008 (6) | 0.0025 (6) |
N2 | 0.0233 (9) | 0.0185 (8) | 0.0160 (7) | 0.0077 (6) | 0.0014 (6) | 0.0043 (6) |
C1 | 0.0180 (10) | 0.0182 (9) | 0.0199 (9) | 0.0044 (7) | −0.0031 (7) | 0.0068 (7) |
C2 | 0.0208 (10) | 0.0256 (10) | 0.0180 (9) | 0.0034 (8) | −0.0013 (7) | 0.0112 (7) |
C3 | 0.0185 (10) | 0.0277 (10) | 0.0139 (8) | 0.0062 (8) | −0.0005 (7) | 0.0039 (7) |
C4 | 0.0174 (10) | 0.0194 (9) | 0.0178 (8) | 0.0050 (7) | −0.0031 (7) | 0.0035 (7) |
C5 | 0.0138 (9) | 0.0173 (8) | 0.0171 (8) | 0.0031 (7) | −0.0019 (6) | 0.0063 (7) |
C6 | 0.0121 (9) | 0.0171 (8) | 0.0148 (8) | 0.0026 (7) | −0.0031 (6) | 0.0037 (6) |
C7 | 0.0128 (9) | 0.0153 (8) | 0.0181 (8) | 0.0037 (7) | −0.0037 (6) | 0.0036 (6) |
C8 | 0.0106 (9) | 0.0157 (8) | 0.0160 (8) | 0.0035 (6) | −0.0028 (6) | 0.0016 (6) |
C9 | 0.0103 (9) | 0.0176 (9) | 0.0157 (8) | 0.0023 (7) | −0.0034 (6) | 0.0026 (6) |
C10 | 0.0137 (9) | 0.0166 (8) | 0.0163 (8) | 0.0040 (7) | −0.0016 (6) | 0.0013 (6) |
C11 | 0.0170 (10) | 0.0163 (9) | 0.0191 (8) | 0.0032 (7) | −0.0021 (7) | 0.0050 (7) |
C12 | 0.0146 (9) | 0.0222 (9) | 0.0150 (8) | 0.0027 (7) | −0.0016 (6) | 0.0049 (7) |
C13 | 0.0150 (9) | 0.0203 (9) | 0.0164 (8) | 0.0050 (7) | −0.0024 (7) | 0.0009 (7) |
C14 | 0.0128 (9) | 0.0157 (8) | 0.0183 (8) | 0.0036 (7) | −0.0029 (6) | 0.0026 (7) |
Geometric parameters (Å, °)
Cl1—C12 | 1.7338 (18) | C4—H4A | 0.92 (2) |
Cl2—C14 | 1.7310 (18) | C5—C6 | 1.399 (3) |
O1—C7 | 1.344 (2) | C5—H5A | 0.87 (2) |
O1—N2 | 1.413 (2) | C6—C7 | 1.457 (2) |
N1—C7 | 1.303 (2) | C8—C9 | 1.470 (2) |
N1—C8 | 1.380 (2) | C9—C10 | 1.401 (3) |
N2—C8 | 1.311 (2) | C9—C14 | 1.405 (3) |
C1—C2 | 1.387 (3) | C10—C11 | 1.385 (3) |
C1—C6 | 1.394 (2) | C10—H10A | 0.94 (2) |
C1—H1A | 0.91 (3) | C11—C12 | 1.388 (3) |
C2—C3 | 1.384 (3) | C11—H11A | 0.91 (2) |
C2—H2A | 0.91 (3) | C12—C13 | 1.387 (3) |
C3—C4 | 1.395 (3) | C13—C14 | 1.389 (3) |
C3—H3A | 0.95 (3) | C13—H13A | 0.99 (3) |
C4—C5 | 1.381 (3) | ||
C7—O1—N2 | 106.71 (14) | O1—C7—C6 | 119.03 (16) |
C7—N1—C8 | 102.57 (15) | N2—C8—N1 | 114.69 (16) |
C8—N2—O1 | 103.00 (15) | N2—C8—C9 | 125.14 (17) |
C2—C1—C6 | 119.53 (18) | N1—C8—C9 | 120.17 (15) |
C2—C1—H1A | 119.2 (16) | C10—C9—C14 | 117.16 (16) |
C6—C1—H1A | 121.2 (16) | C10—C9—C8 | 117.41 (16) |
C3—C2—C1 | 120.30 (17) | C14—C9—C8 | 125.43 (16) |
C3—C2—H2A | 119.8 (16) | C11—C10—C9 | 122.41 (17) |
C1—C2—H2A | 119.9 (16) | C11—C10—H10A | 116.9 (14) |
C2—C3—C4 | 120.40 (18) | C9—C10—H10A | 120.5 (14) |
C2—C3—H3A | 117.6 (16) | C10—C11—C12 | 118.35 (17) |
C4—C3—H3A | 122.0 (16) | C10—C11—H11A | 120.0 (14) |
C5—C4—C3 | 119.60 (18) | C12—C11—H11A | 121.6 (14) |
C5—C4—H4A | 116.9 (14) | C13—C12—C11 | 121.57 (17) |
C3—C4—H4A | 123.3 (14) | C13—C12—Cl1 | 118.49 (15) |
C4—C5—C6 | 120.14 (17) | C11—C12—Cl1 | 119.94 (15) |
C4—C5—H5A | 117.2 (16) | C12—C13—C14 | 118.95 (17) |
C6—C5—H5A | 122.2 (16) | C12—C13—H13A | 118.8 (14) |
C1—C6—C5 | 120.04 (17) | C14—C13—H13A | 121.9 (14) |
C1—C6—C7 | 121.86 (17) | C13—C14—C9 | 121.56 (17) |
C5—C6—C7 | 118.10 (16) | C13—C14—Cl2 | 116.22 (14) |
N1—C7—O1 | 113.04 (16) | C9—C14—Cl2 | 122.21 (14) |
N1—C7—C6 | 127.93 (16) | ||
C7—O1—N2—C8 | −0.24 (19) | C7—N1—C8—N2 | 0.1 (2) |
C6—C1—C2—C3 | 0.8 (3) | C7—N1—C8—C9 | −179.53 (16) |
C1—C2—C3—C4 | −0.2 (3) | N2—C8—C9—C10 | 177.93 (18) |
C2—C3—C4—C5 | −0.5 (3) | N1—C8—C9—C10 | −2.5 (3) |
C3—C4—C5—C6 | 0.5 (3) | N2—C8—C9—C14 | −1.8 (3) |
C2—C1—C6—C5 | −0.9 (3) | N1—C8—C9—C14 | 177.79 (17) |
C2—C1—C6—C7 | 178.25 (17) | C14—C9—C10—C11 | 0.4 (3) |
C4—C5—C6—C1 | 0.2 (3) | C8—C9—C10—C11 | −179.33 (17) |
C4—C5—C6—C7 | −178.94 (17) | C9—C10—C11—C12 | 0.1 (3) |
C8—N1—C7—O1 | −0.2 (2) | C10—C11—C12—C13 | −0.9 (3) |
C8—N1—C7—C6 | 179.12 (18) | C10—C11—C12—Cl1 | 178.69 (14) |
N2—O1—C7—N1 | 0.3 (2) | C11—C12—C13—C14 | 1.2 (3) |
N2—O1—C7—C6 | −179.11 (15) | Cl1—C12—C13—C14 | −178.38 (14) |
C1—C6—C7—N1 | −169.98 (19) | C12—C13—C14—C9 | −0.7 (3) |
C5—C6—C7—N1 | 9.1 (3) | C12—C13—C14—Cl2 | 179.14 (14) |
C1—C6—C7—O1 | 9.4 (3) | C10—C9—C14—C13 | −0.1 (3) |
C5—C6—C7—O1 | −171.53 (16) | C8—C9—C14—C13 | 179.63 (17) |
O1—N2—C8—N1 | 0.1 (2) | C10—C9—C14—Cl2 | −179.90 (14) |
O1—N2—C8—C9 | 179.68 (16) | C8—C9—C14—Cl2 | −0.2 (3) |
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3A···Cl1i | 0.95 (3) | 2.81 (3) | 3.577 (2) | 138.6 (19) |
Symmetry codes: (i) x+1, y, z−1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SJ2743).
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 global, I. DOI: 10.1107/S160053681000927X/sj2743sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053681000927X/sj2743Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report