Abstract
The title compound, C7H6BrNS, crystallizes with two molecules in the asymmetric unit. The dihedral angles between the aromatic ring and the thioamide fragment are 23.6 (4) and 20.5 (3)° in the two molecules. In the crystal, there are intermolecular N—H⋯S hydrogen-bonding interactions between the amine group and the S atoms.
Related literature
For the uses of thioamides, see: Akhtar et al. (2006 ▶, 2007 ▶, 2008 ▶); Jagodzinski et al. (2003 ▶). For the biological activity of thioamides, see: Wei et al. (2006 ▶); Klimesova et al. (1999 ▶). For the synthesis of thioamides, see: Kaboudin et al. (2006 ▶); Cava et al. (1985 ▶). For related crystal structures, see: Khan et al. (2009 ▶); Jian et al. (2006 ▶); Manaka & Sato (2005 ▶).
Experimental
Crystal data
C7H6BrNS
M r = 216.10
Monoclinic,
a = 19.6325 (11) Å
b = 10.6101 (6) Å
c = 7.8859 (5) Å
β = 100.078 (1)°
V = 1617.31 (16) Å3
Z = 8
Mo Kα radiation
μ = 5.26 mm−1
T = 296 K
0.21 × 0.17 × 0.09 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2008 ▶) T min = 0.384, T max = 0.620
12968 measured reflections
3911 independent reflections
2706 reflections with I > 2σ(I)
R int = 0.025
Refinement
R[F 2 > 2σ(F 2)] = 0.035
wR(F 2) = 0.087
S = 1.03
3911 reflections
181 parameters
H-atom parameters constrained
Δρmax = 0.82 e Å−3
Δρmin = −0.78 e Å−3
Data collection: APEX2 (Bruker, 2008 ▶); cell refinement: SAINT (Bruker, 2008 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809018273/bt2956sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809018273/bt2956Isup2.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 |
|---|---|---|---|---|
| N2—H2A⋯S2i | 0.86 | 2.73 | 3.583 (2) | 172 |
| N2—H2B⋯S1ii | 0.86 | 2.65 | 3.500 (2) | 173 |
| N1—H1A⋯S1iii | 0.86 | 2.78 | 3.605 (3) | 160 |
| N1—H1B⋯S2ii | 0.86 | 2.71 | 3.523 (2) | 158 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
The authours thank the HEC, Pakistan, for a Ph.D. fellowship awarded to MuHK under the indiginous Ph.D. Program. JDM thanks Saint Mary’s University for funding.
supplementary crystallographic information
Comment
Thioamides are biologically active compounds, possessing a wide spectrum of activities (Klimesova et al., 1999; Wei et al., 2006). They have enormous practical and synthetic applicability and their importance and impact as synthetic intermediates is continuously growing (Jagodzinski et al., 2003). Thioamides are generally synthesized using Lawesson's reagent (Cava et al., 1985) or phosphorus penta sulfide (Kaboudin et al., 2006). In this article, we wish to report the crystal structure of 4-bromobenzothioamide, which was synthesized by treating 4-bromobenzonitrile with 70% sodium hydrogen sulfide hydrate and magnesium chloride hexahydrate (Manaka & Sato, 2005) in continuation of our previous work on the synthesis and biological screenings of five membered heterocycles (Akhtar et al., 2006, 2007, 2008).
The hydrogen bonding interactions between the nitrogen and sulfur atoms (3.500 (2)Å to 3.605 (3) Å) are in the range of those seen in p-trifluoromethylbenzothioamide where the corresponding interactions are between 3.3735Å and 3.5133Å (Jian et al., 2006) and in the analogus chloride compound where the N···S distances are 3.3769 (15)Å and 3.4527 (15)Å (Khan et al., 2009).
Experimental
The slurry of 70% sodium hydrogen sulfide hydrate (21.98 mmol) and magnesium chloride hexahydrate (10.99 mmol) was prepared in DMF (40 mL). 4-Bromobenzonitrile (11.0 mmol) was added to the slurry and the mixture stirred at room temperature for 2 h. The resulting mixture was poured into water (100 mL) and the precipitated solid collected by filtration. The product obtained was resuspended in 1 N HCl (50 ml), stirred for another 30 min, filtered and washed with excess water. The recrystallization of the product from chloroform afforded the crystals of 4-bromobenzothioamide suitable for X-ray analysis.
Refinement
The hydrogen atoms were placed in geometrically idealized positions of 0.93Å (aromatic C—H) and 0.86Å (amide N—H) and constrained to ride on the parent atom with Uiso(H) = 1.2 UEq(c) for aromatic and amide protons.
Figures
Fig. 1.
Molecular structure of 4-bromobenzothioamide showing displacement ellipsoids at the 50% probability level (for non-H atoms).
Fig. 2.
Packing diagram of 4-bromobenzothioamide. Displacement ellipsoids are shown at the 50% probability level (for non-H atoms).
Crystal data
| C7H6BrNS | F(000) = 848 |
| Mr = 216.10 | Dx = 1.775 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 3900 reflections |
| a = 19.6325 (11) Å | θ = 2.2–26.9° |
| b = 10.6101 (6) Å | µ = 5.26 mm−1 |
| c = 7.8859 (5) Å | T = 296 K |
| β = 100.078 (1)° | Block, yellow |
| V = 1617.31 (16) Å3 | 0.21 × 0.17 × 0.09 mm |
| Z = 8 |
Data collection
| Bruker APEXII CCD diffractometer | 3911 independent reflections |
| Radiation source: fine-focus sealed tube | 2706 reflections with I > 2σ(I) |
| graphite | Rint = 0.025 |
| φ and ω scans | θmax = 28.3°, θmin = 2.1° |
| Absorption correction: multi-scan (SADABS; Bruker, 2008) | h = −25→25 |
| Tmin = 0.384, Tmax = 0.620 | k = −13→14 |
| 12968 measured reflections | l = −10→10 |
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)] = 0.035 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.087 | H-atom parameters constrained |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0372P)2 + 0.7786P] where P = (Fo2 + 2Fc2)/3 |
| 3911 reflections | (Δ/σ)max = 0.001 |
| 181 parameters | Δρmax = 0.82 e Å−3 |
| 0 restraints | Δρmin = −0.77 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 | ||
| Br2 | 0.315314 (16) | 0.36346 (4) | 0.36641 (5) | 0.07035 (13) | |
| Br1 | 0.538072 (18) | 0.69050 (5) | 1.27120 (5) | 0.08477 (16) | |
| S2 | −0.04123 (4) | 0.26135 (7) | 0.39188 (10) | 0.05003 (18) | |
| S1 | 0.21328 (4) | 0.52885 (7) | 0.75427 (10) | 0.05230 (19) | |
| N2 | −0.03383 (11) | 0.4881 (2) | 0.2688 (3) | 0.0473 (6) | |
| H2A | −0.0119 | 0.5515 | 0.2367 | 0.057* | |
| H2B | −0.0780 | 0.4916 | 0.2623 | 0.057* | |
| C1 | 0.23831 (13) | 0.6495 (2) | 0.8875 (3) | 0.0412 (6) | |
| C9 | 0.07643 (12) | 0.3842 (2) | 0.3369 (3) | 0.0342 (5) | |
| C12 | 0.21855 (13) | 0.3743 (3) | 0.3549 (3) | 0.0429 (6) | |
| C10 | 0.10919 (14) | 0.4633 (2) | 0.2364 (4) | 0.0459 (6) | |
| H10A | 0.0831 | 0.5200 | 0.1618 | 0.055* | |
| C14 | 0.11668 (14) | 0.3004 (3) | 0.4448 (3) | 0.0474 (7) | |
| H14A | 0.0956 | 0.2466 | 0.5131 | 0.057* | |
| C5 | 0.44606 (15) | 0.6804 (3) | 1.1491 (4) | 0.0558 (8) | |
| C8 | 0.00020 (13) | 0.3859 (2) | 0.3280 (3) | 0.0370 (5) | |
| C13 | 0.18748 (14) | 0.2945 (3) | 0.4535 (4) | 0.0515 (7) | |
| H13A | 0.2137 | 0.2366 | 0.5260 | 0.062* | |
| C11 | 0.18020 (15) | 0.4589 (3) | 0.2457 (4) | 0.0498 (7) | |
| H11A | 0.2018 | 0.5127 | 0.1785 | 0.060* | |
| N1 | 0.19425 (12) | 0.7375 (2) | 0.9174 (3) | 0.0554 (6) | |
| H1A | 0.2082 | 0.7985 | 0.9867 | 0.067* | |
| H1B | 0.1517 | 0.7338 | 0.8675 | 0.067* | |
| C2 | 0.31088 (13) | 0.6623 (2) | 0.9781 (3) | 0.0408 (6) | |
| C6 | 0.40650 (16) | 0.7873 (3) | 1.1197 (4) | 0.0622 (8) | |
| H6A | 0.4250 | 0.8654 | 1.1563 | 0.075* | |
| C3 | 0.35274 (15) | 0.5562 (3) | 1.0060 (4) | 0.0549 (7) | |
| H3A | 0.3351 | 0.4783 | 0.9659 | 0.066* | |
| C7 | 0.33903 (15) | 0.7780 (3) | 1.0352 (4) | 0.0540 (7) | |
| H7A | 0.3119 | 0.8502 | 1.0162 | 0.065* | |
| C4 | 0.42000 (16) | 0.5644 (3) | 1.0919 (4) | 0.0639 (9) | |
| H4A | 0.4475 | 0.4926 | 1.1110 | 0.077* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br2 | 0.03962 (17) | 0.0895 (3) | 0.0834 (3) | 0.00005 (15) | 0.01476 (15) | 0.00159 (19) |
| Br1 | 0.04511 (19) | 0.1196 (4) | 0.0842 (3) | −0.00878 (19) | −0.00386 (16) | −0.0108 (2) |
| S2 | 0.0434 (4) | 0.0390 (4) | 0.0685 (5) | −0.0063 (3) | 0.0120 (3) | 0.0056 (3) |
| S1 | 0.0465 (4) | 0.0459 (4) | 0.0626 (5) | −0.0022 (3) | 0.0043 (3) | −0.0081 (3) |
| N2 | 0.0398 (12) | 0.0358 (12) | 0.0667 (15) | 0.0016 (9) | 0.0101 (11) | 0.0030 (11) |
| C1 | 0.0427 (14) | 0.0402 (14) | 0.0415 (14) | 0.0002 (11) | 0.0096 (11) | 0.0055 (11) |
| C9 | 0.0400 (13) | 0.0271 (12) | 0.0358 (13) | −0.0022 (10) | 0.0076 (10) | −0.0035 (10) |
| C12 | 0.0405 (14) | 0.0435 (15) | 0.0448 (15) | −0.0022 (12) | 0.0078 (11) | −0.0071 (12) |
| C10 | 0.0485 (15) | 0.0347 (14) | 0.0566 (17) | 0.0078 (12) | 0.0150 (12) | 0.0086 (12) |
| C14 | 0.0444 (15) | 0.0515 (17) | 0.0459 (15) | −0.0021 (12) | 0.0067 (12) | 0.0152 (13) |
| C5 | 0.0392 (15) | 0.078 (2) | 0.0497 (17) | −0.0057 (15) | 0.0057 (12) | −0.0030 (15) |
| C8 | 0.0428 (13) | 0.0305 (13) | 0.0375 (13) | −0.0018 (10) | 0.0065 (10) | −0.0057 (10) |
| C13 | 0.0420 (15) | 0.0607 (18) | 0.0499 (16) | 0.0040 (13) | 0.0023 (12) | 0.0138 (14) |
| C11 | 0.0552 (17) | 0.0372 (15) | 0.0628 (18) | −0.0003 (13) | 0.0261 (14) | 0.0071 (13) |
| N1 | 0.0442 (13) | 0.0528 (15) | 0.0659 (16) | 0.0090 (11) | 0.0004 (11) | −0.0115 (12) |
| C2 | 0.0395 (13) | 0.0418 (15) | 0.0420 (14) | 0.0003 (11) | 0.0099 (11) | 0.0036 (11) |
| C6 | 0.0509 (18) | 0.063 (2) | 0.072 (2) | −0.0100 (15) | 0.0088 (15) | −0.0202 (17) |
| C3 | 0.0483 (16) | 0.0439 (16) | 0.069 (2) | −0.0015 (13) | 0.0022 (14) | 0.0035 (14) |
| C7 | 0.0518 (17) | 0.0471 (17) | 0.0633 (19) | −0.0007 (13) | 0.0108 (14) | −0.0083 (14) |
| C4 | 0.0477 (17) | 0.058 (2) | 0.082 (2) | 0.0054 (15) | 0.0008 (15) | 0.0080 (17) |
Geometric parameters (Å, °)
| Br2—C12 | 1.890 (3) | C14—C13 | 1.381 (4) |
| Br1—C5 | 1.896 (3) | C14—H14A | 0.9300 |
| S2—C8 | 1.675 (3) | C5—C6 | 1.371 (5) |
| S1—C1 | 1.674 (3) | C5—C4 | 1.379 (5) |
| N2—C8 | 1.316 (3) | C13—H13A | 0.9300 |
| N2—H2A | 0.8600 | C11—H11A | 0.9300 |
| N2—H2B | 0.8600 | N1—H1A | 0.8600 |
| C1—N1 | 1.322 (3) | N1—H1B | 0.8600 |
| C1—C2 | 1.484 (4) | C2—C3 | 1.388 (4) |
| C9—C14 | 1.380 (3) | C2—C7 | 1.389 (4) |
| C9—C10 | 1.388 (3) | C6—C7 | 1.378 (4) |
| C9—C8 | 1.486 (3) | C6—H6A | 0.9300 |
| C12—C13 | 1.364 (4) | C3—C4 | 1.377 (4) |
| C12—C11 | 1.373 (4) | C3—H3A | 0.9300 |
| C10—C11 | 1.384 (4) | C7—H7A | 0.9300 |
| C10—H10A | 0.9300 | C4—H4A | 0.9300 |
| C8—N2—H2A | 120.0 | C12—C13—C14 | 119.3 (3) |
| C8—N2—H2B | 120.0 | C12—C13—H13A | 120.3 |
| H2A—N2—H2B | 120.0 | C14—C13—H13A | 120.3 |
| N1—C1—C2 | 116.9 (2) | C12—C11—C10 | 119.5 (3) |
| N1—C1—S1 | 121.5 (2) | C12—C11—H11A | 120.3 |
| C2—C1—S1 | 121.58 (19) | C10—C11—H11A | 120.3 |
| C14—C9—C10 | 118.0 (2) | C1—N1—H1A | 120.0 |
| C14—C9—C8 | 120.0 (2) | C1—N1—H1B | 120.0 |
| C10—C9—C8 | 122.0 (2) | H1A—N1—H1B | 120.0 |
| C13—C12—C11 | 120.8 (3) | C3—C2—C7 | 118.3 (3) |
| C13—C12—Br2 | 118.7 (2) | C3—C2—C1 | 119.6 (2) |
| C11—C12—Br2 | 120.4 (2) | C7—C2—C1 | 122.1 (2) |
| C11—C10—C9 | 120.8 (2) | C5—C6—C7 | 119.3 (3) |
| C11—C10—H10A | 119.6 | C5—C6—H6A | 120.3 |
| C9—C10—H10A | 119.6 | C7—C6—H6A | 120.3 |
| C9—C14—C13 | 121.5 (2) | C4—C3—C2 | 121.1 (3) |
| C9—C14—H14A | 119.2 | C4—C3—H3A | 119.4 |
| C13—C14—H14A | 119.2 | C2—C3—H3A | 119.4 |
| C6—C5—C4 | 121.1 (3) | C6—C7—C2 | 121.0 (3) |
| C6—C5—Br1 | 120.0 (2) | C6—C7—H7A | 119.5 |
| C4—C5—Br1 | 118.9 (2) | C2—C7—H7A | 119.5 |
| N2—C8—C9 | 118.1 (2) | C3—C4—C5 | 119.1 (3) |
| N2—C8—S2 | 120.9 (2) | C3—C4—H4A | 120.5 |
| C9—C8—S2 | 120.96 (18) | C5—C4—H4A | 120.5 |
| C3—C1—C2—S1 | 23.6 (3) | C14—C8—C9—S2 | 20.5 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2A···S2i | 0.86 | 2.73 | 3.583 (2) | 172 |
| N2—H2B···S1ii | 0.86 | 2.65 | 3.500 (2) | 173 |
| N1—H1A···S1iii | 0.86 | 2.78 | 3.605 (3) | 160 |
| N1—H1B···S2ii | 0.86 | 2.71 | 3.523 (2) | 158 |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) −x, −y+1, −z+1; (iii) x, −y+3/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2956).
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 I, global. DOI: 10.1107/S1600536809018273/bt2956sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809018273/bt2956Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


