organic compounds
2,5-Bis[(3-chlorobenzyl)sulfanyl]-1,3,4-thiadiazole
aCollege of Biology and Environmental Engineering, Zhejiang Shuren University, Hangzhou 310015, People's Republic of China
*Correspondence e-mail: nabosun@gmail.com
The complete molecule of the title compound, C16H12Cl2N2S3, is generated by crystallographic twofold symmetry, with the S atom of the thiadiazole ring lying on the rotation axis. The dihedral angle between the mean planes of the 1,3,4-thiadiazole and benzene rings is 87.19 (7)°. In the crystal, molecules are linked by C—H⋯N interactions and short S⋯S contacts [3.3389 (9) Å] occur.
Related literature
For details of the synthesis, see: Liu et al. (2012); Tan et al. (2012). For a related structure, see: Liu & Liu (2011. For the biological activity of related compounds, see: Liu et al. (2011a,b).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku/MSC, 2005); cell CrystalClear; data reduction: CrystalClear (Rigaku/MSC, 2005); 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.
Supporting information
10.1107/S1600536812019150/hb6758sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812019150/hb6758Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812019150/hb6758Isup3.cml
To a stirred solution of 1,3,4-thiadiazole-2,5-dithiol (5.1 mmol) and potassium carbonate (5.6 mmol) in DMF (15 ml), 1-chloro-3-(chloromethyl)benzene (5.6 mmol) was added dropwise. The resulting mixture was stirred at room temperature overnight. The mixture was poured into water, the precipitate formed was filtered off and recrystallized from acetone to give title compound in good yields. Compound was dissolved in hot alcohol and the resulting solution was allowed to stand in air at room temperature to colourless blocks of the title compound.
All the H atoms were positioned geometrically (C—H = 0.93–0.97 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).
Data collection: CrystalClear (Rigaku/MSC, 2005); cell
CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); 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 (Sheldrick, 2008).Fig. 1. The molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level. |
C16H12Cl2N2S3 | F(000) = 816 |
Mr = 399.36 | Dx = 1.556 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
a = 17.200 (3) Å | Cell parameters from 2634 reflections |
b = 5.6604 (11) Å | θ = 3.3–27.9° |
c = 17.524 (4) Å | µ = 0.75 mm−1 |
β = 92.56 (3)° | T = 113 K |
V = 1704.4 (6) Å3 | Block, colorless |
Z = 4 | 0.12 × 0.10 × 0.06 mm |
Rigaku Saturn CCD diffractometer | 1491 independent reflections |
Radiation source: rotating anode | 1382 reflections with I > 2σ(I) |
Confocal monochromator | Rint = 0.028 |
ω scans | θmax = 25.0°, θmin = 3.3° |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) | h = −20→20 |
Tmin = 0.916, Tmax = 0.957 | k = −6→6 |
5343 measured reflections | l = −14→20 |
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)] = 0.024 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.063 | H-atom parameters constrained |
S = 1.17 | w = 1/[σ2(Fo2) + (0.0254P)2 + 1.1171P] where P = (Fo2 + 2Fc2)/3 |
1491 reflections | (Δ/σ)max = 0.001 |
105 parameters | Δρmax = 0.25 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
C16H12Cl2N2S3 | V = 1704.4 (6) Å3 |
Mr = 399.36 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 17.200 (3) Å | µ = 0.75 mm−1 |
b = 5.6604 (11) Å | T = 113 K |
c = 17.524 (4) Å | 0.12 × 0.10 × 0.06 mm |
β = 92.56 (3)° |
Rigaku Saturn CCD diffractometer | 1491 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) | 1382 reflections with I > 2σ(I) |
Tmin = 0.916, Tmax = 0.957 | Rint = 0.028 |
5343 measured reflections |
R[F2 > 2σ(F2)] = 0.024 | 0 restraints |
wR(F2) = 0.063 | H-atom parameters constrained |
S = 1.17 | Δρmax = 0.25 e Å−3 |
1491 reflections | Δρmin = −0.22 e Å−3 |
105 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.03445 (2) | −0.05340 (7) | 0.41412 (2) | 0.01769 (13) | |
S2 | 0.0000 | 0.13382 (10) | 0.2500 | 0.01979 (16) | |
Cl1 | 0.36343 (2) | −0.14225 (8) | 0.42335 (3) | 0.03039 (14) | |
N1 | 0.01164 (7) | −0.3031 (2) | 0.28829 (7) | 0.0161 (3) | |
C1 | 0.22023 (9) | 0.0583 (3) | 0.41728 (9) | 0.0198 (3) | |
H1 | 0.2061 | −0.0599 | 0.4508 | 0.024* | |
C2 | 0.29495 (9) | 0.0682 (3) | 0.39189 (9) | 0.0206 (4) | |
C3 | 0.31795 (9) | 0.2422 (3) | 0.34242 (9) | 0.0255 (4) | |
H3 | 0.3687 | 0.2464 | 0.3263 | 0.031* | |
C4 | 0.26429 (10) | 0.4097 (3) | 0.31736 (10) | 0.0284 (4) | |
H4 | 0.2789 | 0.5278 | 0.2840 | 0.034* | |
C5 | 0.18844 (10) | 0.4023 (3) | 0.34188 (9) | 0.0232 (4) | |
H5 | 0.1525 | 0.5150 | 0.3245 | 0.028* | |
C6 | 0.16605 (9) | 0.2277 (3) | 0.39205 (8) | 0.0171 (3) | |
C7 | 0.08449 (9) | 0.2289 (3) | 0.42062 (9) | 0.0190 (3) | |
H7A | 0.0540 | 0.3448 | 0.3916 | 0.023* | |
H7B | 0.0869 | 0.2793 | 0.4736 | 0.023* | |
C8 | 0.01873 (8) | −0.0905 (3) | 0.31589 (8) | 0.0136 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0171 (2) | 0.0229 (2) | 0.0129 (2) | −0.00199 (16) | −0.00114 (15) | 0.00075 (15) |
S2 | 0.0314 (3) | 0.0127 (3) | 0.0149 (3) | 0.000 | −0.0042 (2) | 0.000 |
Cl1 | 0.0197 (2) | 0.0303 (3) | 0.0404 (3) | 0.00735 (18) | −0.00680 (18) | 0.00062 (19) |
N1 | 0.0158 (6) | 0.0171 (7) | 0.0153 (6) | −0.0004 (6) | 0.0002 (5) | 0.0007 (5) |
C1 | 0.0191 (8) | 0.0213 (8) | 0.0187 (8) | −0.0008 (7) | −0.0024 (6) | −0.0009 (7) |
C2 | 0.0169 (8) | 0.0213 (8) | 0.0230 (8) | 0.0029 (7) | −0.0063 (6) | −0.0050 (7) |
C3 | 0.0143 (8) | 0.0314 (10) | 0.0308 (9) | −0.0037 (7) | 0.0006 (7) | −0.0027 (8) |
C4 | 0.0230 (10) | 0.0274 (10) | 0.0348 (10) | −0.0044 (8) | 0.0018 (7) | 0.0074 (8) |
C5 | 0.0198 (9) | 0.0204 (9) | 0.0289 (9) | 0.0020 (7) | −0.0031 (7) | 0.0004 (7) |
C6 | 0.0153 (8) | 0.0201 (8) | 0.0156 (7) | −0.0020 (7) | −0.0030 (6) | −0.0070 (6) |
C7 | 0.0166 (8) | 0.0214 (8) | 0.0190 (8) | −0.0002 (7) | −0.0009 (6) | −0.0061 (7) |
C8 | 0.0096 (7) | 0.0164 (8) | 0.0149 (8) | 0.0001 (6) | 0.0006 (6) | 0.0018 (6) |
S1—C8 | 1.7432 (15) | C2—C3 | 1.382 (2) |
S1—C7 | 1.8161 (17) | C3—C4 | 1.381 (2) |
S2—C8i | 1.7367 (15) | C3—H3 | 0.9300 |
S2—C8 | 1.7368 (15) | C4—C5 | 1.392 (2) |
Cl1—C2 | 1.7471 (17) | C4—H4 | 0.9300 |
N1—C8 | 1.301 (2) | C5—C6 | 1.389 (2) |
N1—N1i | 1.383 (2) | C5—H5 | 0.9300 |
C1—C2 | 1.380 (2) | C6—C7 | 1.511 (2) |
C1—C6 | 1.395 (2) | C7—H7A | 0.9700 |
C1—H1 | 0.9300 | C7—H7B | 0.9700 |
C8—S1—C7 | 102.72 (7) | C6—C5—C4 | 120.47 (16) |
C8i—S2—C8 | 86.03 (10) | C6—C5—H5 | 119.8 |
C8—N1—N1i | 112.28 (8) | C4—C5—H5 | 119.8 |
C2—C1—C6 | 119.25 (15) | C5—C6—C1 | 119.31 (15) |
C2—C1—H1 | 120.4 | C5—C6—C7 | 119.64 (15) |
C6—C1—H1 | 120.4 | C1—C6—C7 | 121.02 (14) |
C1—C2—C3 | 121.89 (15) | C6—C7—S1 | 114.82 (11) |
C1—C2—Cl1 | 119.68 (13) | C6—C7—H7A | 108.6 |
C3—C2—Cl1 | 118.43 (13) | S1—C7—H7A | 108.6 |
C4—C3—C2 | 118.87 (15) | C6—C7—H7B | 108.6 |
C4—C3—H3 | 120.6 | S1—C7—H7B | 108.6 |
C2—C3—H3 | 120.6 | H7A—C7—H7B | 107.5 |
C3—C4—C5 | 120.22 (16) | N1—C8—S2 | 114.69 (11) |
C3—C4—H4 | 119.9 | N1—C8—S1 | 119.12 (11) |
C5—C4—H4 | 119.9 | S2—C8—S1 | 125.76 (9) |
C6—C1—C2—C3 | 0.4 (2) | C5—C6—C7—S1 | 131.52 (14) |
C6—C1—C2—Cl1 | 179.77 (12) | C1—C6—C7—S1 | −50.67 (18) |
C1—C2—C3—C4 | −0.5 (3) | C8—S1—C7—C6 | −69.17 (13) |
Cl1—C2—C3—C4 | −179.85 (13) | N1i—N1—C8—S2 | −1.62 (19) |
C2—C3—C4—C5 | 0.1 (3) | N1i—N1—C8—S1 | 171.24 (12) |
C3—C4—C5—C6 | 0.4 (3) | C8i—S2—C8—N1 | 0.62 (7) |
C4—C5—C6—C1 | −0.5 (2) | C8i—S2—C8—S1 | −171.70 (14) |
C4—C5—C6—C7 | 177.37 (15) | C7—S1—C8—N1 | 154.09 (12) |
C2—C1—C6—C5 | 0.1 (2) | C7—S1—C8—S2 | −33.91 (11) |
C2—C1—C6—C7 | −177.73 (14) |
Symmetry code: (i) −x, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···N1ii | 0.93 | 2.59 | 3.514 (2) | 172 |
Symmetry code: (ii) x+1/2, y+1/2, z. |
Experimental details
Crystal data | |
Chemical formula | C16H12Cl2N2S3 |
Mr | 399.36 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 113 |
a, b, c (Å) | 17.200 (3), 5.6604 (11), 17.524 (4) |
β (°) | 92.56 (3) |
V (Å3) | 1704.4 (6) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.75 |
Crystal size (mm) | 0.12 × 0.10 × 0.06 |
Data collection | |
Diffractometer | Rigaku Saturn CCD diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku/MSC, 2005) |
Tmin, Tmax | 0.916, 0.957 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5343, 1491, 1382 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.024, 0.063, 1.17 |
No. of reflections | 1491 |
No. of parameters | 105 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.25, −0.22 |
Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···N1i | 0.93 | 2.59 | 3.514 (2) | 172 |
Symmetry code: (i) x+1/2, y+1/2, z. |
Acknowledgements
The project was supported by the Program of the Education Department of Zhejiang Province, China (Y200803060).
References
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