Abstract
The title molecule, C12H12N2O3S, is composed of two individually planar units, viz. 5-phenyl-1,3,4-oxadiazol-2-yl-sulfanyl and ethyl acetate, which are oriented at almost right angles [80.07 (8)°] with respect to each other. The structure is stabilized by weak intermolecular C—H⋯O and C—H⋯N hydrogen bonds. The phenyl and oxadiazole rings show π–π stacking interactions [centroid–centroid distance = 3.846 (2) Å] and there is also a short π-interaction between the carbonyl O atom and the oxadiazole ring [the distance from this O atom to the centroid of the oxadiazole ring is 3.156 (2) Å].
Related literature
For related literature, see: Cao et al. (2002 ▶); Iqbal et al. (2007 ▶); Kadi et al. (2007 ▶); Mir & Siddiqui (1970 ▶); Zareef et al. (2006 ▶, 2007 ▶).
Experimental
Crystal data
C12H12N2O3S
M r = 264.30
Monoclinic,
a = 8.777 (3) Å
b = 11.008 (5) Å
c = 13.177 (6) Å
β = 103.59 (3)°
V = 1237.5 (9) Å3
Z = 4
Mo Kα radiation
μ = 0.26 mm−1
T = 173 (2) K
0.16 × 0.10 × 0.08 mm
Data collection
Nonius KappaCCD diffractometer
Absorption correction: multi-scan (SORTAV; Blessing, 1997 ▶) T min = 0.959, T max = 0.979
5263 measured reflections
2820 independent reflections
1943 reflections with I > 2σ(I)
R int = 0.046
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.117
S = 1.02
2820 reflections
165 parameters
H-atom parameters constrained
Δρmax = 0.25 e Å−3
Δρmin = −0.27 e Å−3
Data collection: COLLECT (Hooft, 1998 ▶); cell refinement: DENZO (Otwinowski & Minor, 1997 ▶); data reduction: SCALEPACK (Otwinowski & Minor, 1997 ▶); program(s) used to solve structure: SAPI91 (Fan, 1991 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808007125/fb2092sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808007125/fb2092Isup2.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 |
|---|---|---|---|---|
| C4—H4⋯O2i | 0.95 | 2.51 | 3.268 (3) | 137 |
| C9—H9B⋯N1ii | 0.99 | 2.38 | 3.293 (3) | 153 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
Substituted-1,3,4-oxadiazole derivatives are of significant interest due to their chemotherapeutic effects (Kadi et al., 2007; Zareef et al., 2006; Zareef et al., 2007; Cao et al., 2002). Based on the known structures of the 2,5-disubstituted-1,3,4-oxadiazoles with diverse biological activities and their derivatives, we have designed and synthesized several new derivatives of 1,3,4-oxadiazole (Zareef et al., 2007). In this paper, we report the structure of one of these compounds.
The structure of the title compound (Fig. 1) is composed of two essentially planar moieties, C1—C8/N1/N2/O1/S1 and C9—C12/O2/O3 the least-square planes of which are inclined at 80.07 (8)°; the maximum deviations from the respective least square planes are: O1 = 0.037 (2) and C11 = 0.048 (2) Å. The structure is stabilized by two intermolecular interactions C4—H4···O2 and C9—H9B···N1 (Table 1). The shortest distance between the centroids of the phenyl and the oxadiazole rings of the adjacent molecules is 3.846 (2) Å which indicates the existence of π-π stacking interactions. In addition, there is a π-interaction between the carbonyl O-atom and the oxadiazole ring. (The distance from this O atom to the centroid of the oxadiazole ring is 3.156 (2) Å). The bond distances and angles in the title compound are in agreement with the corresponding ones reported in the similar structure of Ethyl 2-({5-[2-(benzoylamino)phenyl]-1,3,4-oxadiazol-2-yl}sulfanyl)acetate (Iqbal et al., 2007).
Experimental
The title compound was prepared according to the procedure reported in the literature (Zareef et al., 2006; Mir & Siddiqui, 1970). To a solution of benzoic acid hydrazide (50 mmol) in ethanol (150 ml) was added carbon disulfide (55 mmol), followed by the addition of KOH (50 mmol) dissolved in 25 ml of water. The reaction mixture was stirred and subjected to reflux for 19 h. After reaction completion, excess ethanol was distilled off. The crude solid obtained was dissolved in water (50 ml) and acidified with 4 N HCl to pH 2–3. The product was filtered, washed with water and recrystallized from aqueous ethanol (20–30%). The resulting 5-phenyl-2-mercapto-1,3,4-oxadiazole (20 mmol) was dissolved in saturated aqueous sodium hydrogencarbonate solution while stirring. The required ethylbromoacetate (20 mmol) in absolute ethanol (10 ml) was added and the reaction mixture was stirred for 7 h at 325–335 K. After reaction completion, the resulting solid was filtered off, washed with water and recrystallized from aqueous ethanol (60%) (Yield = 75%; m.p. = 344–345 K). Prismatic crystals suitable for crystallographic study were grown from ethanol solution by slow evaporation at room temperature.
Refinement
Though all the H atoms could be distinguished in the difference Fouries map the H-atoms were situated at the geometrically idealized positions and refined in riding-model approximation with the following constraints: aryl, methylene and methyl C—H distances were set to 0.95, 0.99 and 0.98 Å, respectively; in all these instances Uiso(H) = 1.2 Ueq(C).
Figures
Fig. 1.
ORTEP-3 (Farrugia, 1997) drawing of the title molecule with displacement ellipsoids plotted at 50% probability level.
Crystal data
| C12H12N2O3S | F000 = 552 |
| Mr = 264.30 | Dx = 1.419 Mg m−3 |
| Monoclinic, P21/c | Melting point = 344–345 K |
| Hall symbol: -P 2ybc | Mo Kα radiation λ = 0.71073 Å |
| a = 8.777 (3) Å | Cell parameters from 5263 reflections |
| b = 11.008 (5) Å | θ = 3.7–27.5º |
| c = 13.177 (6) Å | µ = 0.26 mm−1 |
| β = 103.59 (3)º | T = 173 (2) K |
| V = 1237.5 (9) Å3 | Prism, colourless |
| Z = 4 | 0.16 × 0.10 × 0.08 mm |
Data collection
| Nonius KappaCCD diffractometer | 2820 independent reflections |
| Radiation source: fine-focus sealed tube | 1943 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.046 |
| T = 173(2) K | θmax = 27.5º |
| ω and φ scans | θmin = 3.7º |
| Absorption correction: multi-scan(SORTAV; Blessing, 1997) | h = −11→11 |
| Tmin = 0.959, Tmax = 0.979 | k = −13→14 |
| 5263 measured reflections | l = −17→17 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.045 | H-atom parameters constrained |
| wR(F2) = 0.117 | w = 1/[σ2(Fo2) + (0.058P)2 + 0.1P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.02 | (Δ/σ)max = 0.001 |
| 2820 reflections | Δρmax = 0.25 e Å−3 |
| 165 parameters | Δρmin = −0.27 e Å−3 |
| 47 constraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.021 (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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| S1 | 0.76489 (6) | 0.36024 (5) | 0.69782 (4) | 0.0336 (2) | |
| O1 | 0.67313 (14) | 0.20172 (11) | 0.54296 (10) | 0.0264 (3) | |
| O2 | 0.86894 (16) | 0.19182 (14) | 0.88791 (12) | 0.0412 (4) | |
| O3 | 1.12555 (15) | 0.22664 (13) | 0.90282 (11) | 0.0354 (4) | |
| N1 | 0.87361 (18) | 0.07562 (15) | 0.55872 (13) | 0.0307 (4) | |
| N2 | 0.91309 (18) | 0.16477 (15) | 0.63754 (13) | 0.0319 (4) | |
| C1 | 0.6404 (2) | 0.03494 (16) | 0.41660 (14) | 0.0245 (4) | |
| C2 | 0.7088 (2) | −0.06503 (17) | 0.37915 (15) | 0.0283 (5) | |
| H2 | 0.8131 | −0.0882 | 0.4116 | 0.034* | |
| C3 | 0.6246 (2) | −0.13002 (18) | 0.29499 (16) | 0.0339 (5) | |
| H3 | 0.6717 | −0.1972 | 0.2690 | 0.041* | |
| C4 | 0.4712 (2) | −0.09762 (19) | 0.24806 (16) | 0.0335 (5) | |
| H4 | 0.4130 | −0.1429 | 0.1905 | 0.040* | |
| C5 | 0.4040 (2) | 0.0005 (2) | 0.28557 (16) | 0.0342 (5) | |
| H5 | 0.2991 | 0.0225 | 0.2534 | 0.041* | |
| C6 | 0.4870 (2) | 0.06791 (19) | 0.36949 (15) | 0.0291 (5) | |
| H6 | 0.4397 | 0.1357 | 0.3945 | 0.035* | |
| C7 | 0.7333 (2) | 0.10069 (16) | 0.50595 (15) | 0.0245 (4) | |
| C8 | 0.7925 (2) | 0.23515 (17) | 0.62486 (15) | 0.0266 (4) | |
| C9 | 0.9529 (2) | 0.35400 (18) | 0.78938 (17) | 0.0337 (5) | |
| H9A | 1.0358 | 0.3499 | 0.7498 | 0.040* | |
| H9B | 0.9684 | 0.4302 | 0.8304 | 0.040* | |
| C10 | 0.9730 (2) | 0.24772 (19) | 0.86414 (16) | 0.0311 (5) | |
| C11 | 1.1623 (2) | 0.1290 (2) | 0.97896 (17) | 0.0392 (6) | |
| H11A | 1.1105 | 0.0528 | 0.9492 | 0.047* | |
| H11B | 1.1252 | 0.1498 | 1.0422 | 0.047* | |
| C12 | 1.3366 (2) | 0.1135 (2) | 1.00597 (17) | 0.0421 (6) | |
| H12A | 1.3655 | 0.0466 | 1.0558 | 0.051* | |
| H12B | 1.3864 | 0.1887 | 1.0373 | 0.051* | |
| H12C | 1.3722 | 0.0952 | 0.9425 | 0.051* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0300 (3) | 0.0316 (3) | 0.0369 (3) | 0.0048 (2) | 0.0031 (2) | −0.0069 (2) |
| O1 | 0.0232 (7) | 0.0275 (7) | 0.0273 (7) | 0.0048 (6) | 0.0037 (5) | −0.0008 (6) |
| O2 | 0.0280 (7) | 0.0554 (10) | 0.0392 (9) | −0.0054 (7) | 0.0056 (7) | −0.0009 (8) |
| O3 | 0.0235 (7) | 0.0397 (8) | 0.0407 (9) | 0.0003 (6) | 0.0026 (6) | 0.0013 (7) |
| N1 | 0.0292 (8) | 0.0333 (10) | 0.0278 (9) | 0.0061 (7) | 0.0031 (7) | −0.0055 (8) |
| N2 | 0.0279 (9) | 0.0354 (10) | 0.0308 (10) | 0.0070 (8) | 0.0038 (7) | −0.0050 (8) |
| C1 | 0.0265 (9) | 0.0261 (10) | 0.0219 (10) | −0.0015 (8) | 0.0074 (8) | 0.0045 (8) |
| C2 | 0.0275 (10) | 0.0286 (10) | 0.0288 (11) | 0.0000 (9) | 0.0066 (8) | 0.0020 (9) |
| C3 | 0.0403 (12) | 0.0296 (11) | 0.0327 (12) | −0.0022 (10) | 0.0103 (9) | −0.0023 (9) |
| C4 | 0.0349 (11) | 0.0373 (12) | 0.0278 (11) | −0.0128 (10) | 0.0061 (9) | −0.0010 (9) |
| C5 | 0.0250 (10) | 0.0473 (13) | 0.0286 (11) | −0.0036 (10) | 0.0031 (9) | 0.0057 (10) |
| C6 | 0.0265 (10) | 0.0354 (11) | 0.0264 (11) | 0.0028 (9) | 0.0085 (8) | 0.0044 (9) |
| C7 | 0.0241 (9) | 0.0235 (10) | 0.0278 (10) | 0.0056 (8) | 0.0101 (8) | 0.0034 (8) |
| C8 | 0.0243 (9) | 0.0283 (10) | 0.0267 (10) | 0.0011 (9) | 0.0050 (8) | 0.0005 (8) |
| C9 | 0.0269 (10) | 0.0336 (11) | 0.0382 (12) | −0.0033 (9) | 0.0027 (9) | −0.0088 (9) |
| C10 | 0.0241 (10) | 0.0381 (12) | 0.0300 (11) | −0.0027 (9) | 0.0040 (8) | −0.0111 (9) |
| C11 | 0.0353 (11) | 0.0437 (14) | 0.0387 (13) | 0.0012 (10) | 0.0089 (10) | 0.0031 (10) |
| C12 | 0.0356 (12) | 0.0534 (15) | 0.0360 (13) | 0.0066 (11) | 0.0056 (10) | 0.0033 (11) |
Geometric parameters (Å, °)
| S1—C8 | 1.729 (2) | C3—H3 | 0.9500 |
| S1—C9 | 1.802 (2) | C4—C5 | 1.377 (3) |
| O1—C8 | 1.366 (2) | C4—H4 | 0.9500 |
| O1—C7 | 1.369 (2) | C5—C6 | 1.387 (3) |
| O2—C10 | 1.202 (2) | C5—H5 | 0.9500 |
| O3—C10 | 1.336 (2) | C6—H6 | 0.9500 |
| O3—C11 | 1.454 (3) | C9—C10 | 1.513 (3) |
| N1—C7 | 1.294 (2) | C9—H9A | 0.9900 |
| N1—N2 | 1.412 (2) | C9—H9B | 0.9900 |
| N2—C8 | 1.291 (2) | C11—C12 | 1.497 (3) |
| C1—C6 | 1.392 (2) | C11—H11A | 0.9900 |
| C1—C2 | 1.398 (3) | C11—H11B | 0.9900 |
| C1—C7 | 1.457 (3) | C12—H12A | 0.9800 |
| C2—C3 | 1.379 (3) | C12—H12B | 0.9800 |
| C2—H2 | 0.9500 | C12—H12C | 0.9800 |
| C3—C4 | 1.390 (3) | ||
| C8—S1—C9 | 96.66 (9) | O1—C7—C1 | 120.13 (15) |
| C8—O1—C7 | 102.24 (13) | N2—C8—O1 | 113.20 (17) |
| C10—O3—C11 | 115.56 (16) | N2—C8—S1 | 128.61 (15) |
| C7—N1—N2 | 106.58 (15) | O1—C8—S1 | 118.18 (13) |
| C8—N2—N1 | 105.66 (15) | C10—C9—S1 | 114.43 (14) |
| C6—C1—C2 | 119.91 (17) | C10—C9—H9A | 108.7 |
| C6—C1—C7 | 121.99 (18) | S1—C9—H9A | 108.7 |
| C2—C1—C7 | 118.10 (16) | C10—C9—H9B | 108.7 |
| C3—C2—C1 | 119.90 (18) | S1—C9—H9B | 108.7 |
| C3—C2—H2 | 120.0 | H9A—C9—H9B | 107.6 |
| C1—C2—H2 | 120.0 | O2—C10—O3 | 124.49 (19) |
| C2—C3—C4 | 120.3 (2) | O2—C10—C9 | 125.87 (18) |
| C2—C3—H3 | 119.8 | O3—C10—C9 | 109.62 (17) |
| C4—C3—H3 | 119.8 | O3—C11—C12 | 107.26 (18) |
| C5—C4—C3 | 119.56 (18) | O3—C11—H11A | 110.3 |
| C5—C4—H4 | 120.2 | C12—C11—H11A | 110.3 |
| C3—C4—H4 | 120.2 | O3—C11—H11B | 110.3 |
| C4—C5—C6 | 121.14 (18) | C12—C11—H11B | 110.3 |
| C4—C5—H5 | 119.4 | H11A—C11—H11B | 108.5 |
| C6—C5—H5 | 119.4 | C11—C12—H12A | 109.5 |
| C5—C6—C1 | 119.2 (2) | C11—C12—H12B | 109.5 |
| C5—C6—H6 | 120.4 | H12A—C12—H12B | 109.5 |
| C1—C6—H6 | 120.4 | C11—C12—H12C | 109.5 |
| N1—C7—O1 | 112.32 (16) | H12A—C12—H12C | 109.5 |
| N1—C7—C1 | 127.55 (18) | H12B—C12—H12C | 109.5 |
| C7—N1—N2—C8 | 0.1 (2) | C6—C1—C7—O1 | −3.2 (3) |
| C6—C1—C2—C3 | 0.6 (3) | C2—C1—C7—O1 | 177.68 (16) |
| C7—C1—C2—C3 | 179.73 (18) | N1—N2—C8—O1 | −0.3 (2) |
| C1—C2—C3—C4 | −0.9 (3) | N1—N2—C8—S1 | 178.66 (15) |
| C2—C3—C4—C5 | 0.5 (3) | C7—O1—C8—N2 | 0.4 (2) |
| C3—C4—C5—C6 | 0.1 (3) | C7—O1—C8—S1 | −178.68 (14) |
| C4—C5—C6—C1 | −0.3 (3) | C9—S1—C8—N2 | 0.1 (2) |
| C2—C1—C6—C5 | 0.0 (3) | C9—S1—C8—O1 | 179.01 (15) |
| C7—C1—C6—C5 | −179.09 (18) | C8—S1—C9—C10 | −69.82 (17) |
| N2—N1—C7—O1 | 0.2 (2) | C11—O3—C10—O2 | −0.3 (3) |
| N2—N1—C7—C1 | −179.84 (18) | C11—O3—C10—C9 | 177.96 (16) |
| C8—O1—C7—N1 | −0.4 (2) | S1—C9—C10—O2 | −22.7 (3) |
| C8—O1—C7—C1 | 179.66 (16) | S1—C9—C10—O3 | 159.06 (14) |
| C6—C1—C7—N1 | 176.80 (19) | C10—O3—C11—C12 | 175.61 (18) |
| C2—C1—C7—N1 | −2.3 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C4—H4···O2i | 0.95 | 2.51 | 3.268 (3) | 137 |
| C9—H9B···N1ii | 0.99 | 2.38 | 3.293 (3) | 153 |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+2, y+1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FB2092).
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/S1600536808007125/fb2092sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808007125/fb2092Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

