supplementary materials


Acta Cryst. (2007). E63, o3721    [ doi:10.1107/S1600536807036148 ]

2-Chloro-5-{[5-(4-pyridyl)-1,3,4-oxadiazol-2-yl]sulfanylmethyl}pyridine

W.-D. Wang, Q.-Y. Ren, J.-J. Wei and H.-W. He

Abstract top

In the title compound, C13H9ClN4OS, the mean plane of the oxadiazole ring makes a dihedral angle of 6.34 (13)° with the mean plane of the pyridine ring. The dihedral angle between the chloropyridine ring and the oxadiazole ring is 74.43 (12)°, and the dihedral angle between the chloropyridine ring and the pyridine ring is 69.78 (11)°. The crystal packing is stabilized by inter- and intramolecular C-H...N hydrogen bonds.

Comment top

1,3,4,-oxadiazole derivatives are important compounds with versatile industrial and medical applications (Reddy & Reddy, 1987; Hui et al., 2000; Lin et al., 2002). We report here the molecular structure of (I). In the title compound, all bond lengths and angles are within normal ranges (Allen et al., 1987) and the molecules are stabilized by intra and intermolecular hydrogen bonds (Table 1). The crystal packing also shows two weak intramolecular ππ stacking interactions.

Related literature top

For the biological and pharmaceutical activity of oxadiazols, see Reddy & Reddy (1987); Hui et al. (2000). Many derivatives of oxadiazols have been prepared by Lin et al. (2002). For related literature, see: Allen et al. (1987).

Experimental top

5-Pyridin-4-yl-1,3,4-oxadiazole-2-thiol (0.72 g, 4 mmol) was added to a solution of 1.2% sodium hydroxide at room temperature while stirring. The mixture of 2-Chloro-5-chloromethyl-pyridine (0.72 g, 4.4 mmol) in methanol (4 ml) was added dropwise while the 5-Pyridin-4-yl-1,3,4-oxadiazole-2-thiol was dissolved. The mixture was then stirred at room temperature for 6 h. The white solid was filtered and recrystallized from dimethylformamide-water mixture to give the title compound (yield 54%). Colourless crystals of (I) suitable for X-ray structure analysis were grown from the mixture of dichloromethane and n-hexane (v/v, 1:8).

Refinement top

All H atoms were placed in calculated positions, with C—H distances in the range 0.93–0.97 Å, and included in the final cycles of refinement using a riding-model approximation, with Uiso(H) = 1.2–1.5Ueq(carrier atom).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXTL (Bruker, 1997).

Figures top
[Figure 1] Fig. 1. The structure of (I). showing 50% probability displacement ellipsoids and the atom-numbering scheme.
[Figure 2] Fig. 2. Crystal Packing diagram of (I). Hydrogen bonds are shown as dashed lines.
2-Chloro-5-{[5-(4-pyridyl)-1,3,4-oxadiazol-2-yl]sulfanylmethyl}pyridine top
Crystal data top
C13H9ClN4OSZ = 2
Mr = 304.75F000 = 312
Triclinic, P1Dx = 1.544 Mg m3
Hall symbol: -p 1Mo Kα radiation
λ = 0.71073 Å
a = 6.2729 (5) ÅCell parameters from 2330 reflections
b = 8.1448 (6) Åθ = 2.7–28.2º
c = 14.0994 (11) ŵ = 0.45 mm1
α = 85.520 (1)ºT = 297 (2) K
β = 77.793 (1)ºBlock, colourless
γ = 68.637 (1)º0.30 × 0.20 × 0.20 mm
V = 655.70 (9) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
2544 independent reflections
Radiation source: fine-focus sealed tube2108 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.047
T = 297(2) Kθmax = 26.0º
φ and ω scansθmin = 1.5º
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 7→7
Tmin = 0.877, Tmax = 0.915k = 6→10
4655 measured reflectionsl = 16→17
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.042  w = 1/[σ2(Fo2) + (0.0696P)2 + 0.0355P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.131(Δ/σ)max < 0.001
S = 1.13Δρmax = 0.27 e Å3
2544 reflectionsΔρmin = 0.25 e Å3
182 parametersExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.069 (8)
Secondary atom site location: difference Fourier map
Crystal data top
C13H9ClN4OSγ = 68.637 (1)º
Mr = 304.75V = 655.70 (9) Å3
Triclinic, P1Z = 2
a = 6.2729 (5) ÅMo Kα
b = 8.1448 (6) ŵ = 0.45 mm1
c = 14.0994 (11) ÅT = 297 (2) K
α = 85.520 (1)º0.30 × 0.20 × 0.20 mm
β = 77.793 (1)º
Data collection top
Bruker SMART CCD area-detector
diffractometer
2544 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
2108 reflections with I > 2σ(I)
Tmin = 0.877, Tmax = 0.915Rint = 0.047
4655 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.042182 parameters
wR(F2) = 0.131H-atom parameters constrained
S = 1.13Δρmax = 0.27 e Å3
2544 reflectionsΔρmin = 0.25 e Å3
Special details top

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 > 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) top
xyzUiso*/Ueq
C10.6614 (4)0.2322 (3)0.49086 (15)0.0395 (5)
C20.8922 (4)0.2144 (3)0.47658 (17)0.0436 (5)
H21.00020.15380.42340.052*
C30.9574 (4)0.2900 (3)0.54425 (17)0.0435 (5)
H31.11200.28090.53760.052*
C40.7901 (4)0.3801 (3)0.62265 (15)0.0381 (5)
C50.5648 (4)0.3872 (3)0.62834 (15)0.0413 (5)
H50.45220.44720.68060.050*
C60.8574 (4)0.4667 (3)0.69576 (17)0.0462 (6)
H6A0.72380.56850.72250.055*
H6B0.98040.50860.66300.055*
C70.6924 (4)0.3411 (3)0.86759 (16)0.0403 (5)
C80.4622 (4)0.2839 (3)0.98761 (15)0.0396 (5)
C90.3821 (4)0.1990 (3)1.07587 (15)0.0390 (5)
C100.5377 (4)0.0739 (3)1.12639 (17)0.0432 (5)
H100.69810.03881.10390.052*
C110.4464 (4)0.0041 (3)1.21055 (17)0.0498 (6)
H110.55060.07941.24380.060*
C120.0730 (5)0.1666 (4)1.19713 (19)0.0543 (7)
H120.08660.19781.22080.065*
C130.1458 (4)0.2445 (3)1.11242 (18)0.0484 (6)
H130.03740.32651.08030.058*
Cl10.57259 (11)0.14110 (9)0.40489 (4)0.0542 (2)
N10.4965 (3)0.3144 (3)0.56436 (13)0.0423 (5)
N20.4872 (3)0.4496 (3)0.86157 (13)0.0464 (5)
N30.3340 (3)0.4109 (3)0.94122 (14)0.0448 (5)
N40.2198 (4)0.0483 (3)1.24723 (15)0.0528 (5)
O10.6933 (3)0.23080 (19)0.94565 (10)0.0410 (4)
S10.95815 (10)0.32163 (9)0.79527 (4)0.0493 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0466 (13)0.0414 (12)0.0346 (11)0.0197 (10)0.0112 (9)0.0048 (9)
C20.0417 (12)0.0459 (13)0.0398 (12)0.0155 (10)0.0014 (9)0.0006 (10)
C30.0320 (11)0.0519 (14)0.0465 (13)0.0169 (10)0.0052 (9)0.0042 (10)
C40.0408 (12)0.0415 (12)0.0377 (11)0.0209 (10)0.0115 (9)0.0084 (9)
C50.0371 (12)0.0518 (14)0.0350 (11)0.0178 (10)0.0037 (9)0.0008 (10)
C60.0481 (14)0.0538 (15)0.0465 (13)0.0282 (12)0.0147 (10)0.0070 (11)
C70.0468 (13)0.0399 (12)0.0362 (11)0.0138 (10)0.0145 (9)0.0022 (9)
C80.0436 (12)0.0373 (12)0.0374 (12)0.0111 (10)0.0108 (9)0.0068 (9)
C90.0432 (12)0.0385 (12)0.0364 (11)0.0131 (9)0.0104 (9)0.0068 (9)
C100.0390 (12)0.0475 (13)0.0416 (12)0.0116 (10)0.0096 (9)0.0047 (10)
C110.0596 (15)0.0462 (14)0.0418 (13)0.0143 (12)0.0149 (11)0.0011 (10)
C120.0505 (15)0.0587 (16)0.0504 (15)0.0190 (12)0.0013 (11)0.0070 (12)
C130.0478 (14)0.0460 (14)0.0498 (14)0.0114 (11)0.0144 (11)0.0034 (11)
Cl10.0654 (4)0.0628 (4)0.0448 (4)0.0320 (3)0.0145 (3)0.0048 (3)
N10.0397 (10)0.0537 (12)0.0382 (10)0.0224 (9)0.0078 (8)0.0007 (9)
N20.0459 (11)0.0469 (11)0.0412 (11)0.0091 (9)0.0120 (9)0.0015 (9)
N30.0388 (10)0.0503 (12)0.0392 (10)0.0081 (9)0.0082 (8)0.0013 (9)
N40.0583 (13)0.0546 (13)0.0471 (12)0.0232 (11)0.0069 (10)0.0040 (10)
O10.0416 (9)0.0421 (9)0.0377 (8)0.0112 (7)0.0114 (6)0.0007 (7)
S10.0399 (4)0.0629 (4)0.0474 (4)0.0184 (3)0.0153 (3)0.0045 (3)
Geometric parameters (Å, °) top
C1—N11.320 (3)C7—S11.720 (2)
C1—C21.374 (3)C8—N31.286 (3)
C1—Cl11.748 (2)C8—O11.364 (3)
C2—C31.377 (3)C8—C91.461 (3)
C2—H20.9300C9—C131.381 (3)
C3—C41.392 (3)C9—C101.398 (3)
C3—H30.9300C10—C111.380 (3)
C4—C51.378 (3)C10—H100.9300
C4—C61.501 (3)C11—N41.328 (3)
C5—N11.335 (3)C11—H110.9300
C5—H50.9300C12—N41.341 (3)
C6—S11.826 (2)C12—C131.378 (4)
C6—H6A0.9700C12—H120.9300
C6—H6B0.9700C13—H130.9300
C7—N21.285 (3)N2—N31.412 (3)
C7—O11.365 (3)
N1—C1—C2125.6 (2)N3—C8—O1112.8 (2)
N1—C1—Cl1116.04 (17)N3—C8—C9126.5 (2)
C2—C1—Cl1118.31 (18)O1—C8—C9120.72 (17)
C1—C2—C3117.3 (2)C13—C9—C10118.2 (2)
C1—C2—H2121.3C13—C9—C8119.7 (2)
C3—C2—H2121.3C10—C9—C8122.1 (2)
C2—C3—C4119.5 (2)C11—C10—C9118.1 (2)
C2—C3—H3120.3C11—C10—H10120.9
C4—C3—H3120.3C9—C10—H10120.9
C5—C4—C3117.2 (2)N4—C11—C10124.3 (2)
C5—C4—C6122.8 (2)N4—C11—H11117.8
C3—C4—C6120.1 (2)C10—C11—H11117.8
N1—C5—C4124.8 (2)N4—C12—C13123.5 (2)
N1—C5—H5117.6N4—C12—H12118.2
C4—C5—H5117.6C13—C12—H12118.2
C4—C6—S1113.78 (16)C12—C13—C9119.0 (2)
C4—C6—H6A108.8C12—C13—H13120.5
S1—C6—H6A108.8C9—C13—H13120.5
C4—C6—H6B108.8C1—N1—C5115.59 (19)
S1—C6—H6B108.8C7—N2—N3105.74 (18)
H6A—C6—H6B107.7C8—N3—N2106.27 (17)
N2—C7—O1113.2 (2)C11—N4—C12116.8 (2)
N2—C7—S1129.65 (19)C8—O1—C7102.04 (16)
O1—C7—S1117.16 (15)C7—S1—C699.33 (11)
N1—C1—C2—C30.6 (3)C8—C9—C13—C12178.3 (2)
Cl1—C1—C2—C3178.82 (16)C2—C1—N1—C51.0 (3)
C1—C2—C3—C40.2 (3)Cl1—C1—N1—C5178.40 (16)
C2—C3—C4—C50.5 (3)C4—C5—N1—C10.7 (3)
C2—C3—C4—C6178.6 (2)O1—C7—N2—N30.4 (3)
C3—C4—C5—N10.1 (3)S1—C7—N2—N3178.04 (18)
C6—C4—C5—N1179.0 (2)O1—C8—N3—N20.4 (2)
C5—C4—C6—S192.6 (2)C9—C8—N3—N2179.6 (2)
C3—C4—C6—S188.4 (2)C7—N2—N3—C80.5 (2)
N3—C8—C9—C135.5 (4)C10—C11—N4—C121.1 (4)
O1—C8—C9—C13174.5 (2)C13—C12—N4—C111.2 (4)
N3—C8—C9—C10173.4 (2)N3—C8—O1—C70.2 (2)
O1—C8—C9—C106.6 (3)C9—C8—O1—C7179.87 (19)
C13—C9—C10—C110.7 (3)N2—C7—O1—C80.2 (2)
C8—C9—C10—C11178.3 (2)S1—C7—O1—C8178.12 (15)
C9—C10—C11—N40.2 (4)N2—C7—S1—C611.0 (2)
N4—C12—C13—C90.4 (4)O1—C7—S1—C6171.46 (17)
C10—C9—C13—C120.6 (4)C4—C6—S1—C782.18 (19)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C2—H2···N4i0.932.613.515 (3)164
C13—H13···N3ii0.932.583.462 (3)158
C5—H5···N20.932.613.273 (3)129
C6—H6A···N20.972.552.961 (3)106
Symmetry codes: (i) x+1, y, z−1; (ii) −x, −y+1, −z+2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C2—H2···N4i0.932.613.515 (3)164
C13—H13···N3ii0.932.583.462 (3)158
C5—H5···N20.932.613.273 (3)129
C6—H6A···N20.972.552.961 (3)106
Symmetry codes: (i) x+1, y, z−1; (ii) −x, −y+1, −z+2.
Acknowledgements top

The authors gratefully acknowledge financial support of this work by the National Basic Research Programme of China (grant No. 2003CB114400) and the National Natural Science Foundation of China (grant No. 20372023).

references
References top

Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.

Bruker (1997). SHELXTL. Version 5.10. Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2000). SMART (Version 5.059), SAINT (Version 6.01) and SADABS (Version 6.10). Bruker AXS Inc., Madison, Wisconsin, USA.

Hui, X. P., Chu, C. H., Zhang, Z. Y., Wang, Q. & Zhang, Q. (2000). Indian J. Chem. Sect. B, 41, 2176–2179.

Lin, N.-H., Dong, L., Bunnelle, W. H., Anderson, D. J. & Meyer, M. D. (2002). Bioorg. Med. Chem. Lett. 12, 3321–3324.

Reddy, P. S. N. & Reddy, P. P. (1987). Indian J. Chem. Sect. B, 26, 890–891.

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Spek, A. L. (2003). J. Appl. Cryst. 36, 7–13.