Abstract
The title compound, C8H6INS, is essentially planar, the largest deviation from the mean plane being for the I atom [0.075 (3) Å]. The crystal structure is mainly stabilized by intermolecular C—I⋯N halogen bonds, forming zigzag supramolecular chains in [10]. Relatively short off-set π–π contacts [centroid–centroid distance = 3.758 (2) Å] between the thiazole rings of inversion-related molecules link neighbouring chains and provide the secondary interactions for building the crystal structure.
Related literature
For the application of benzothiazoles as biologically active compounds, see: Leong et al. (2004 ▶); Yildiz-Oren et al. (2004 ▶); Lockhart et al. (2005 ▶); Sheng et al. (2007 ▶). For the synthesis of the title compound, see: Racané et al. (2006 ▶, 2011 ▶). For related 1,3-benzothiazole structures, see: Matković-Čalogović et al. (2003 ▶); Pavlović et al. (2009 ▶); Đaković et al. (2009 ▶); Čičak et al. (2010 ▶). For graph-set theory, see: Etter (1990 ▶); Bernstein et al. (1995 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶).
Experimental
Crystal data
C8H6INS
M r = 275.11
Monoclinic,
a = 8.3255 (3) Å
b = 7.6967 (3) Å
c = 13.8083 (5) Å
β = 90.686 (4)°
V = 884.76 (6) Å3
Z = 4
Mo Kα radiation
μ = 3.79 mm−1
T = 296 K
0.47 × 0.38 × 0.14 mm
Data collection
Oxford Diffraction Xcalibur diffractometer with a Saphire-3 CCD detector
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.253, T max = 0.658
13190 measured reflections
1928 independent reflections
1729 reflections with I > 2σ(I)
R int = 0.027
Refinement
R[F 2 > 2σ(F 2)] = 0.024
wR(F 2) = 0.064
S = 1.06
1928 reflections
101 parameters
H-atom parameters constrained
Δρmax = 0.84 e Å−3
Δρmin = −0.72 e Å−3
Data collection: CrysAlis PRO (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811004570/fj2389sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004570/fj2389Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Halogen-bond geometry (Å, °).
C4—I1 | I1⋯N1i | C4⋯N1i | C4—I1⋯N1i | |
---|---|---|---|---|
C4—I1⋯N1i | 2.103 (3) | 3.158 (2) | 5.257 (4) | 175.99 (9) |
Symmetry code: (i) .
Acknowledgments
This research was supported by the Ministry of Science, Education and Sports of the Republic of Croatia, Zagreb (grant Nos. 119–1193079–1332 and 119–1191342–1339).
supplementary crystallographic information
Comment
This work was a part of our preparative, structural, mechanistic and computational investigation of a series of substituted benzothiazoles (bta), which attract considerable interest due to their biological activities.
The molecule is almost ideally planar (r.m.s. deviation = 0.009 Å), with the largest deviation from the plane being that of atom I1 [0.075 (3) Å] (Fig.1). The geometry of the benzothiazole rings is consistent with other 1,3-benzothiazoles listed in the CSD base (Allen et al., 2002). The two S—C bonds of the thiazole ring [S1—C1 and S1—C2] differ with respect to each other, but both are within two bortherline cases, single S—C [1.82 Å] and double S=C [1.56 Å], while the endocyclic C—N bond is dominantly double in character. The differences in C—C bonds within benzene ring are common for such fused rings.
In the crystal structure halogen bonds are the principal specific interactions responsible for the crystal packing. There is only one short and directional C—I···N contact [C—I = 2.103 (3) Å] (see Table 1) that link the molecules into antiparallel zigzag C(7) chains (Etter, 1990; Bernstein et al., 1995) in [1 0 - 1] direction (Figs. 2 and 3).
Relatively short off-set π–π contacts [Cg···Cg = 3.758 (2) Å] between the thiazole rings, belonging to the molecules that are related by an inversion centre, link the neighboring supramolecular chains and provide the secondary interactions for building the crystal structure.
The structure of the title compound is one more example showing that halogen bonding is also as effective and reliable tool for assembling molecules into supramolecular architectures.
Experimental
Colourless single crystals of the title compound were obtained by slow evaporation of a dichloromethane solution.
Refinement
All H atoms were placed in geometrically idealized positions and constrained to ride on their parent C atom at distances of 0.93 or 0.96 Å for aromatic or methyl H atoms, respectively, and with Uiso(H) = 1.2Ueq(C) (for aromatic H) or Uiso(H) = 1.5Ueq(C) (for methyl group).
Figures
Fig. 1.
Molecular structure of the title compound with the atom labeling scheme. Displacement ellipsoids for non-H atoms are drawn at the 50% probability level.
Fig. 2.
Crystal packing of the title compound viewed down the b axis showing halogen bonds as dashed lines.
Fig. 3.
Spacefill representaton of a zigzag halogen bonding chain running in [1 0 - 1].
Crystal data
C8H6INS | F(000) = 520 |
Mr = 275.11 | Dx = 2.065 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 10010 reflections |
a = 8.3255 (3) Å | θ = 4.4–32.6° |
b = 7.6967 (3) Å | µ = 3.79 mm−1 |
c = 13.8083 (5) Å | T = 296 K |
β = 90.686 (4)° | Plate, colourless |
V = 884.76 (6) Å3 | 0.47 × 0.38 × 0.14 mm |
Z = 4 |
Data collection
Oxford Diffraction Xcalibur diffractometer with a Saphire-3 CCD detector | 1928 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 1729 reflections with I > 2σ(I) |
graphite | Rint = 0.027 |
Detector resolution: 16.3426 pixels mm-1 | θmax = 27.0°, θmin = 4.6° |
CCD scans | h = −10→10 |
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | k = −9→9 |
Tmin = 0.253, Tmax = 0.658 | l = −17→17 |
13190 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)] = 0.024 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.064 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0397P)2 + 0.4162P] where P = (Fo2 + 2Fc2)/3 |
1928 reflections | (Δ/σ)max = 0.001 |
101 parameters | Δρmax = 0.84 e Å−3 |
0 restraints | Δρmin = −0.72 e Å−3 |
Special details
Experimental. Solvent used: CH2Cl2 Crystal mount: glued on a glass fibre Mosaicity (°): 1.1 (1) Frames collected: 892 Seconds exposure per frame: 5 Degree rotation per frame: 1.0 Crystal-Detector distance (mm): 50.0. |
Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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 | ||
I1 | 0.96733 (2) | 0.14994 (3) | 0.30624 (1) | 0.0485 (1) | |
S1 | 0.66879 (11) | 0.75187 (9) | 0.49021 (6) | 0.0518 (3) | |
N1 | 0.6453 (3) | 0.5615 (3) | 0.64355 (18) | 0.0447 (8) | |
C1 | 0.6117 (4) | 0.7135 (4) | 0.6097 (2) | 0.0457 (9) | |
C2 | 0.7440 (3) | 0.5425 (3) | 0.4842 (2) | 0.0392 (8) | |
C3 | 0.8155 (3) | 0.4585 (4) | 0.40718 (19) | 0.0430 (8) | |
C4 | 0.8633 (3) | 0.2887 (4) | 0.42068 (19) | 0.0399 (8) | |
C5 | 0.8427 (4) | 0.2058 (4) | 0.5097 (2) | 0.0452 (9) | |
C6 | 0.7728 (4) | 0.2900 (4) | 0.5857 (2) | 0.0467 (9) | |
C7 | 0.7211 (3) | 0.4614 (3) | 0.5734 (2) | 0.0386 (7) | |
C8 | 0.5343 (5) | 0.8546 (4) | 0.6669 (3) | 0.0600 (11) | |
H3 | 0.83070 | 0.51470 | 0.34840 | 0.0520* | |
H5 | 0.87710 | 0.09160 | 0.51740 | 0.0540* | |
H6 | 0.75980 | 0.23380 | 0.64480 | 0.0560* | |
H8A | 0.46780 | 0.80420 | 0.71580 | 0.0900* | |
H8B | 0.46950 | 0.92540 | 0.62460 | 0.0900* | |
H8C | 0.61580 | 0.92510 | 0.69710 | 0.0900* |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.0488 (1) | 0.0567 (2) | 0.0402 (1) | 0.0012 (1) | 0.0048 (1) | −0.0055 (1) |
S1 | 0.0658 (5) | 0.0376 (4) | 0.0518 (4) | 0.0063 (3) | −0.0035 (3) | 0.0058 (3) |
N1 | 0.0487 (13) | 0.0419 (13) | 0.0437 (13) | −0.0022 (10) | 0.0082 (10) | −0.0014 (10) |
C1 | 0.0416 (14) | 0.0411 (14) | 0.0543 (17) | −0.0019 (12) | −0.0027 (12) | −0.0054 (12) |
C2 | 0.0424 (14) | 0.0345 (12) | 0.0407 (13) | −0.0029 (11) | −0.0035 (11) | 0.0049 (11) |
C3 | 0.0482 (15) | 0.0457 (14) | 0.0351 (13) | −0.0040 (12) | −0.0001 (11) | 0.0075 (12) |
C4 | 0.0393 (14) | 0.0457 (14) | 0.0347 (13) | −0.0025 (11) | 0.0025 (11) | −0.0027 (11) |
C5 | 0.0536 (16) | 0.0347 (13) | 0.0474 (16) | 0.0044 (12) | 0.0043 (13) | 0.0030 (11) |
C6 | 0.0593 (18) | 0.0394 (13) | 0.0415 (15) | −0.0005 (13) | 0.0114 (13) | 0.0073 (12) |
C7 | 0.0396 (13) | 0.0364 (12) | 0.0399 (13) | −0.0035 (11) | 0.0037 (10) | 0.0013 (10) |
C8 | 0.062 (2) | 0.0511 (19) | 0.067 (2) | 0.0089 (15) | −0.0004 (17) | −0.0108 (15) |
Geometric parameters (Å, °)
I1—C4 | 2.103 (3) | C4—C5 | 1.397 (4) |
S1—C1 | 1.748 (3) | C5—C6 | 1.369 (4) |
S1—C2 | 1.731 (2) | C6—C7 | 1.397 (4) |
N1—C1 | 1.289 (4) | C3—H3 | 0.9300 |
N1—C7 | 1.395 (4) | C5—H5 | 0.9300 |
C1—C8 | 1.494 (5) | C6—H6 | 0.9300 |
C2—C3 | 1.385 (4) | C8—H8A | 0.9600 |
C2—C7 | 1.396 (4) | C8—H8B | 0.9600 |
C3—C4 | 1.378 (4) | C8—H8C | 0.9600 |
I1···C1i | 3.826 (3) | H3···H8Avii | 2.5800 |
I1···N1ii | 3.158 (2) | H5···S1viii | 3.1600 |
I1···H5iii | 3.3100 | H5···I1iii | 3.3100 |
S1···H5iv | 3.1600 | H5···H5iii | 2.5400 |
S1···H8Bv | 3.1600 | H8A···H3ix | 2.5800 |
N1···I1vi | 3.158 (2) | H8B···S1v | 3.1600 |
C1···I1i | 3.826 (3) | ||
C1—S1—C2 | 89.46 (14) | N1—C7—C6 | 125.3 (2) |
C1—N1—C7 | 110.3 (2) | C2—C7—C6 | 119.0 (2) |
S1—C1—N1 | 115.8 (2) | C2—C3—H3 | 121.00 |
S1—C1—C8 | 120.0 (2) | C4—C3—H3 | 121.00 |
N1—C1—C8 | 124.1 (3) | C4—C5—H5 | 119.00 |
S1—C2—C3 | 129.1 (2) | C6—C5—H5 | 120.00 |
S1—C2—C7 | 108.70 (19) | C5—C6—H6 | 120.00 |
C3—C2—C7 | 122.2 (2) | C7—C6—H6 | 120.00 |
C2—C3—C4 | 117.7 (2) | C1—C8—H8A | 110.00 |
I1—C4—C3 | 120.06 (19) | C1—C8—H8B | 110.00 |
I1—C4—C5 | 119.0 (2) | C1—C8—H8C | 109.00 |
C3—C4—C5 | 120.9 (3) | H8A—C8—H8B | 109.00 |
C4—C5—C6 | 121.1 (3) | H8A—C8—H8C | 109.00 |
C5—C6—C7 | 119.1 (3) | H8B—C8—H8C | 109.00 |
N1—C7—C2 | 115.7 (2) | ||
C2—S1—C1—N1 | 0.5 (3) | S1—C2—C7—C6 | 180.0 (2) |
C2—S1—C1—C8 | 178.5 (3) | C3—C2—C7—N1 | −179.1 (2) |
C1—S1—C2—C3 | 179.0 (3) | C3—C2—C7—C6 | 0.4 (4) |
C1—S1—C2—C7 | −0.6 (2) | C2—C3—C4—I1 | 178.41 (19) |
C7—N1—C1—S1 | −0.3 (3) | C2—C3—C4—C5 | −1.1 (4) |
C7—N1—C1—C8 | −178.2 (3) | I1—C4—C5—C6 | −178.8 (2) |
C1—N1—C7—C2 | −0.2 (3) | C3—C4—C5—C6 | 0.8 (5) |
C1—N1—C7—C6 | −179.6 (3) | C4—C5—C6—C7 | 0.2 (5) |
S1—C2—C3—C4 | −179.0 (2) | C5—C6—C7—N1 | 178.6 (3) |
C7—C2—C3—C4 | 0.6 (4) | C5—C6—C7—C2 | −0.8 (4) |
S1—C2—C7—N1 | 0.5 (3) |
Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) x+1/2, −y+1/2, z−1/2; (iii) −x+2, −y, −z+1; (iv) x, y+1, z; (v) −x+1, −y+2, −z+1; (vi) x−1/2, −y+1/2, z+1/2; (vii) x+1/2, −y+3/2, z−1/2; (viii) x, y−1, z; (ix) x−1/2, −y+3/2, z+1/2.
Table 1 Halogen-bond geometry (Å, °)
C4—I1 | I1···N1i | C4···N1i | C4—I1···N1i | |
C4—I1···N1i | 2.103 (3) | 3.158 (2) | 5.257 (4) | 175.99 (9) |
Symmetry code: (i) 1/2 + x, 1/2–y, –1/2 + z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2389).
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/S1600536811004570/fj2389sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004570/fj2389Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report