Abstract
The title molecule, C18H12N4S3, consists of three essentially planar fragments, viz. two methyl-substituted benzonitrile rings and a substituted thiadiazole ring. The dihedral angles between the substituted benzonitrile rings and the central thiadiazole ring are 28.29 (10) and 78.83 (6)°, and the dihedral angle between the two benzonitrile rings is 72.89 (7)°.
Related literature
For related literature, see: Tarafder et al., (2000 ▶); El-Shekeil et al. (1988 ▶); Jinxia et al. (2003 ▶).
Experimental
Crystal data
C18H12N4S3
M r = 380.50
Monoclinic,
a = 7.6974 (15) Å
b = 8.4375 (17) Å
c = 27.272 (6) Å
β = 92.53 (3)°
V = 1769.5 (6) Å3
Z = 4
Mo Kα radiation
μ = 0.43 mm−1
T = 293 (2) K
0.45 × 0.40 × 0.30 mm
Data collection
Rigaku Mercury2 diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.814, T max = 0.903
15327 measured reflections
4028 independent reflections
2754 reflections with I > 2σ(I)
R int = 0.043
Refinement
R[F 2 > 2σ(F 2)] = 0.053
wR(F 2) = 0.115
S = 1.05
4028 reflections
226 parameters
H-atom parameters constrained
Δρmax = 0.20 e Å−3
Δρmin = −0.25 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/S1600536808022848/fl2207sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808022848/fl2207Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Acknowledgments
This work was supported by a Start-up Grant from Southeast University to HZ.
supplementary crystallographic information
Comment
1,3,4-thiadiazole-2,5-dithiol and its derivatives are interesting compounds that have attracted the attention of researchers because of their wide range of applications in many fields, such as the determination of trace elements, the synthesis of novel heterocyclic compounds with antimicrobial activity(El-Shekeil et al. 1988), advanced materials, and battery cathodes (Jinxia et al.2003, Tarafder et al., (2000)). In this paper, we report the structure of one such derviative, the title compound (I).
In (I, Fig. 1) all bond lengths and angles are normal. There are three planar fragments in the molecule, viz. the central S1—S2—S3—C1—C2—N1—N2 plane with C1 farthest out at (0.0077 (19) Å) and the two benzonitrile systems C11—C18 and N4 with C11 farthest out at 0.0280 (19) Å) and C3—C19 and N3 with N3 farthest out at 0.0738 (21) Å. The dihedral angles between the central substituted ring and benzonitrile systems are 28.29 (10)° and 78.83 (6)° and 72.89 (7)° between the two benzonitrile moieties. There is no evidence of typical hydrogenn bonding or intermolecular π–π interactions. Only van-der-waals interactions are observed in the crystal is packing (Fig.2).
Experimental
A dry 50 ml flask was charged with 1,3,4-thiadiazole-2,5-dithiol (10 mmol), 4-(bromomethyl)benzonitrile (20 mmol), K2CO3(10 mmol), and methanol (30 mL). The mixture was stirred with refluxing for 4 h and then was poured into water (40 ml), the precipitate was washed with water for 2–3 times and purified by recrystallization from methanol to give the crystals of the target material.
Refinement
All the C—H hydrogen atoms were calculated geometrically and were allowed to ride on the C atoms to which they are bonded, with acyclic C—H distances ranging as 0.97 Å, phenyl C—H distances ranging as 0.93 Å, and with Uiso(H) = 1.2Ueq(C).
Figures
Fig. 1.
A view of the compound with the atomic numbering scheme. Displacement ellipsoids were drawn at the 30% probability level.
Fig. 2.
Packing diagram of the title compound, showing the structure along the b axis.
Crystal data
| C18H12N4S3 | F(000) = 784 |
| Mr = 380.50 | Dx = 1.428 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 12716 reflections |
| a = 7.6974 (15) Å | θ = 3.3–27.3° |
| b = 8.4375 (17) Å | µ = 0.43 mm−1 |
| c = 27.272 (6) Å | T = 293 K |
| β = 92.53 (3)° | Prism, colorless |
| V = 1769.5 (6) Å3 | 0.45 × 0.40 × 0.30 mm |
| Z = 4 |
Data collection
| Rigaku Mercury2 diffractometer | 4028 independent reflections |
| Radiation source: fine-focus sealed tube | 2754 reflections with I > 2σ(I) |
| graphite | Rint = 0.043 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 3.0° |
| CCD_Profile_fitting scans | h = −9→9 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −10→10 |
| Tmin = 0.814, Tmax = 0.903 | l = −35→35 |
| 15327 measured reflections |
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)] = 0.053 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.115 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0435P)2 + 0.4638P] where P = (Fo2 + 2Fc2)/3 |
| 4028 reflections | (Δ/σ)max < 0.001 |
| 226 parameters | Δρmax = 0.20 e Å−3 |
| 0 restraints | Δρmin = −0.25 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 | ||
| C1 | 0.6555 (3) | 0.3789 (3) | 0.34124 (8) | 0.0469 (5) | |
| C2 | 0.9214 (3) | 0.3764 (3) | 0.38800 (8) | 0.0476 (6) | |
| C3 | 0.4395 (3) | 0.2503 (3) | 0.27094 (10) | 0.0619 (7) | |
| H3A | 0.5357 | 0.2535 | 0.2491 | 0.074* | |
| H3B | 0.4455 | 0.1514 | 0.2891 | 0.074* | |
| C4 | 0.2700 (3) | 0.2614 (3) | 0.24188 (9) | 0.0494 (6) | |
| C5 | 0.1254 (3) | 0.1815 (3) | 0.25715 (10) | 0.0681 (8) | |
| H5 | 0.1344 | 0.1193 | 0.2853 | 0.082* | |
| C6 | −0.0313 (3) | 0.1926 (3) | 0.23136 (10) | 0.0675 (8) | |
| H6 | −0.1277 | 0.1379 | 0.2419 | 0.081* | |
| C7 | −0.0448 (3) | 0.2853 (3) | 0.18983 (8) | 0.0463 (5) | |
| C8 | 0.0971 (3) | 0.3662 (3) | 0.17434 (8) | 0.0504 (6) | |
| H8 | 0.0873 | 0.4293 | 0.1464 | 0.060* | |
| C9 | 0.2533 (3) | 0.3540 (3) | 0.20014 (9) | 0.0521 (6) | |
| H9 | 0.3494 | 0.4087 | 0.1894 | 0.062* | |
| C10 | −0.2123 (3) | 0.3038 (3) | 0.16434 (9) | 0.0576 (7) | |
| C11 | 1.2030 (3) | 0.2210 (3) | 0.42467 (10) | 0.0602 (7) | |
| H11A | 1.1265 | 0.1432 | 0.4386 | 0.072* | |
| H11B | 1.2195 | 0.1920 | 0.3908 | 0.072* | |
| C12 | 1.3756 (3) | 0.2188 (3) | 0.45268 (8) | 0.0489 (6) | |
| C13 | 1.4027 (3) | 0.2929 (3) | 0.49739 (9) | 0.0571 (6) | |
| H13 | 1.3126 | 0.3500 | 0.5106 | 0.068* | |
| C14 | 1.5604 (3) | 0.2838 (3) | 0.52286 (9) | 0.0568 (6) | |
| H14 | 1.5767 | 0.3346 | 0.5530 | 0.068* | |
| C15 | 1.6945 (3) | 0.1987 (3) | 0.50351 (9) | 0.0486 (6) | |
| C16 | 1.6682 (3) | 0.1221 (3) | 0.45909 (9) | 0.0563 (6) | |
| H16 | 1.7575 | 0.0631 | 0.4462 | 0.068* | |
| C17 | 1.5102 (3) | 0.1328 (3) | 0.43390 (9) | 0.0553 (6) | |
| H17 | 1.4936 | 0.0815 | 0.4039 | 0.066* | |
| C18 | 1.8610 (3) | 0.1876 (3) | 0.52986 (9) | 0.0558 (6) | |
| N1 | 0.7442 (3) | 0.2519 (3) | 0.33425 (8) | 0.0576 (5) | |
| N2 | 0.9002 (3) | 0.2507 (2) | 0.36166 (8) | 0.0573 (5) | |
| N3 | −0.3451 (3) | 0.3216 (4) | 0.14549 (9) | 0.0848 (8) | |
| N4 | 1.9930 (3) | 0.1766 (3) | 0.54989 (9) | 0.0740 (7) | |
| S1 | 0.75230 (9) | 0.51067 (8) | 0.38233 (2) | 0.0594 (2) | |
| S2 | 0.45247 (8) | 0.41683 (8) | 0.31298 (2) | 0.0595 (2) | |
| S3 | 1.10283 (9) | 0.41341 (8) | 0.42665 (3) | 0.0642 (2) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0514 (13) | 0.0435 (13) | 0.0451 (13) | −0.0003 (11) | −0.0051 (10) | −0.0021 (10) |
| C2 | 0.0521 (14) | 0.0403 (13) | 0.0499 (13) | −0.0007 (11) | −0.0046 (10) | 0.0007 (10) |
| C3 | 0.0557 (15) | 0.0595 (16) | 0.0689 (17) | 0.0079 (13) | −0.0167 (12) | −0.0152 (13) |
| C4 | 0.0475 (13) | 0.0459 (14) | 0.0540 (14) | 0.0037 (11) | −0.0076 (11) | −0.0056 (11) |
| C5 | 0.0654 (17) | 0.0724 (19) | 0.0653 (17) | −0.0093 (15) | −0.0122 (14) | 0.0269 (14) |
| C6 | 0.0509 (15) | 0.081 (2) | 0.0694 (18) | −0.0132 (14) | −0.0042 (13) | 0.0272 (15) |
| C7 | 0.0423 (13) | 0.0497 (14) | 0.0463 (13) | 0.0028 (11) | −0.0039 (10) | −0.0007 (10) |
| C8 | 0.0535 (14) | 0.0511 (14) | 0.0464 (13) | −0.0022 (12) | −0.0002 (11) | 0.0072 (11) |
| C9 | 0.0470 (14) | 0.0515 (15) | 0.0577 (15) | −0.0082 (12) | 0.0031 (11) | −0.0010 (12) |
| C10 | 0.0511 (16) | 0.0691 (18) | 0.0523 (15) | 0.0021 (14) | 0.0005 (12) | 0.0068 (13) |
| C11 | 0.0546 (15) | 0.0506 (15) | 0.0741 (17) | −0.0006 (12) | −0.0122 (13) | −0.0093 (13) |
| C12 | 0.0502 (14) | 0.0396 (13) | 0.0561 (15) | −0.0038 (11) | −0.0052 (11) | 0.0033 (11) |
| C13 | 0.0517 (14) | 0.0607 (16) | 0.0584 (15) | 0.0103 (13) | −0.0014 (12) | −0.0096 (13) |
| C14 | 0.0565 (15) | 0.0585 (16) | 0.0547 (15) | 0.0084 (13) | −0.0059 (12) | −0.0061 (12) |
| C15 | 0.0464 (13) | 0.0427 (13) | 0.0564 (15) | −0.0002 (11) | −0.0037 (11) | 0.0103 (11) |
| C16 | 0.0526 (15) | 0.0525 (15) | 0.0640 (16) | 0.0085 (12) | 0.0038 (12) | 0.0001 (13) |
| C17 | 0.0603 (16) | 0.0527 (15) | 0.0526 (15) | 0.0027 (13) | −0.0019 (12) | −0.0080 (12) |
| C18 | 0.0553 (16) | 0.0512 (15) | 0.0607 (16) | 0.0061 (13) | 0.0001 (12) | 0.0081 (12) |
| N1 | 0.0526 (12) | 0.0538 (13) | 0.0648 (13) | 0.0076 (10) | −0.0160 (10) | −0.0139 (10) |
| N2 | 0.0525 (12) | 0.0532 (13) | 0.0647 (13) | 0.0061 (10) | −0.0147 (10) | −0.0131 (10) |
| N3 | 0.0503 (14) | 0.126 (2) | 0.0771 (17) | 0.0071 (15) | −0.0094 (12) | 0.0204 (16) |
| N4 | 0.0572 (14) | 0.0870 (18) | 0.0765 (16) | 0.0146 (13) | −0.0119 (12) | 0.0068 (13) |
| S1 | 0.0657 (4) | 0.0441 (4) | 0.0664 (4) | 0.0074 (3) | −0.0187 (3) | −0.0101 (3) |
| S2 | 0.0572 (4) | 0.0556 (4) | 0.0640 (4) | 0.0118 (3) | −0.0159 (3) | −0.0095 (3) |
| S3 | 0.0646 (4) | 0.0468 (4) | 0.0786 (5) | 0.0012 (3) | −0.0278 (3) | −0.0094 (3) |
Geometric parameters (Å, °)
| C1—N1 | 1.289 (3) | C9—H9 | 0.9300 |
| C1—S1 | 1.725 (2) | C10—N3 | 1.134 (3) |
| C1—S2 | 1.742 (2) | C11—C12 | 1.503 (3) |
| C2—N2 | 1.287 (3) | C11—S3 | 1.799 (3) |
| C2—S1 | 1.727 (2) | C11—H11A | 0.9700 |
| C2—S3 | 1.740 (2) | C11—H11B | 0.9700 |
| C3—C4 | 1.499 (3) | C12—C13 | 1.378 (3) |
| C3—S2 | 1.814 (2) | C12—C17 | 1.382 (3) |
| C3—H3A | 0.9700 | C13—C14 | 1.374 (3) |
| C3—H3B | 0.9700 | C13—H13 | 0.9300 |
| C4—C5 | 1.381 (3) | C14—C15 | 1.381 (3) |
| C4—C9 | 1.382 (3) | C14—H14 | 0.9300 |
| C5—C6 | 1.372 (3) | C15—C16 | 1.380 (3) |
| C5—H5 | 0.9300 | C15—C18 | 1.445 (3) |
| C6—C7 | 1.376 (3) | C16—C17 | 1.373 (3) |
| C6—H6 | 0.9300 | C16—H16 | 0.9300 |
| C7—C8 | 1.371 (3) | C17—H17 | 0.9300 |
| C7—C10 | 1.446 (3) | C18—N4 | 1.136 (3) |
| C8—C9 | 1.370 (3) | N1—N2 | 1.386 (3) |
| C8—H8 | 0.9300 | ||
| N1—C1—S1 | 114.56 (17) | C12—C11—S3 | 111.49 (17) |
| N1—C1—S2 | 123.94 (18) | C12—C11—H11A | 109.3 |
| S1—C1—S2 | 121.49 (14) | S3—C11—H11A | 109.3 |
| N2—C2—S1 | 114.47 (17) | C12—C11—H11B | 109.3 |
| N2—C2—S3 | 124.36 (18) | S3—C11—H11B | 109.3 |
| S1—C2—S3 | 121.18 (14) | H11A—C11—H11B | 108.0 |
| C4—C3—S2 | 107.93 (16) | C13—C12—C17 | 118.7 (2) |
| C4—C3—H3A | 110.1 | C13—C12—C11 | 122.7 (2) |
| S2—C3—H3A | 110.1 | C17—C12—C11 | 118.6 (2) |
| C4—C3—H3B | 110.1 | C14—C13—C12 | 121.2 (2) |
| S2—C3—H3B | 110.1 | C14—C13—H13 | 119.4 |
| H3A—C3—H3B | 108.4 | C12—C13—H13 | 119.4 |
| C5—C4—C9 | 118.5 (2) | C13—C14—C15 | 119.6 (2) |
| C5—C4—C3 | 120.3 (2) | C13—C14—H14 | 120.2 |
| C9—C4—C3 | 121.2 (2) | C15—C14—H14 | 120.2 |
| C6—C5—C4 | 120.9 (2) | C16—C15—C14 | 119.7 (2) |
| C6—C5—H5 | 119.6 | C16—C15—C18 | 119.9 (2) |
| C4—C5—H5 | 119.6 | C14—C15—C18 | 120.4 (2) |
| C5—C6—C7 | 119.6 (2) | C17—C16—C15 | 120.0 (2) |
| C5—C6—H6 | 120.2 | C17—C16—H16 | 120.0 |
| C7—C6—H6 | 120.2 | C15—C16—H16 | 120.0 |
| C8—C7—C6 | 120.3 (2) | C16—C17—C12 | 120.7 (2) |
| C8—C7—C10 | 120.2 (2) | C16—C17—H17 | 119.6 |
| C6—C7—C10 | 119.4 (2) | C12—C17—H17 | 119.6 |
| C9—C8—C7 | 119.8 (2) | N4—C18—C15 | 178.6 (3) |
| C9—C8—H8 | 120.1 | C1—N1—N2 | 112.22 (19) |
| C7—C8—H8 | 120.1 | C2—N2—N1 | 112.35 (19) |
| C8—C9—C4 | 120.9 (2) | C1—S1—C2 | 86.40 (12) |
| C8—C9—H9 | 119.5 | C1—S2—C3 | 99.23 (11) |
| C4—C9—H9 | 119.5 | C2—S3—C11 | 98.82 (11) |
| N3—C10—C7 | 177.8 (3) |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FL2207).
References
- El-Shekeil, A., Babaqi, A., Hassan, M. A. & Sheba, S. (1988). Heterocycles, 27, 2577–2580.
- Jinxia, L., Zhan, H. & Zhou, Y. (2003). Electrochem. Commun.5, 555–560.
- Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Tarafder, M. T. H., Azahari, K., Crouse, K. A., Yamin, B. M., Sundara Raj, S. S., Ibrahim, A. R. & Fun, H.-K. (2000). Z. Kristallogr. New Cryst. Struct.215, 487–488.
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/S1600536808022848/fl2207sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808022848/fl2207Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


