supplementary materials


bt2956 scheme

Acta Cryst. (2009). E65, o1333    [ doi:10.1107/S1600536809018273 ]

4-Bromothiobenzamide

M.-H. Khan, S. Hameed, T. Akhtar and J. D. Masuda

Abstract top

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.

Comment top

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).

Related literature top

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 top

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 top

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.

Computing details top

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); 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).

Figures top
[Figure 1] Fig. 1. Molecular structure of 4-bromobenzothioamide showing displacement ellipsoids at the 50% probability level (for non-H atoms).
[Figure 2] Fig. 2. Packing diagram of 4-bromobenzothioamide. Displacement ellipsoids are shown at the 50% probability level (for non-H atoms).
4-Bromothiobenzamide top
Crystal data top
C7H6BrNSF000 = 848
Mr = 216.10Dx = 1.775 Mg m3
Monoclinic, P21/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3900 reflections
a = 19.6325 (11) Åθ = 2.2–26.9º
b = 10.6101 (6) ŵ = 5.26 mm1
c = 7.8859 (5) ÅT = 296 K
β = 100.0780 (10)ºBlock, yellow
V = 1617.31 (16) Å30.21 × 0.17 × 0.09 mm
Z = 8
Data collection top
Bruker APEXII CCD
diffractometer
3911 independent reflections
Radiation source: fine-focus sealed tube2706 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.025
T = 296 Kθmax = 28.3º
φ and ω scansθmin = 2.1º
Absorption correction: multi-scan
(SADABS; Bruker, 2008)
h = 25→25
Tmin = 0.384, Tmax = 0.620k = 13→14
12968 measured reflectionsl = 10→10
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.035H-atom parameters constrained
wR(F2) = 0.087  w = 1/[σ2(Fo2) + (0.0372P)2 + 0.7786P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
3911 reflectionsΔρmax = 0.82 e Å3
181 parametersΔρmin = 0.77 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C7H6BrNSV = 1617.31 (16) Å3
Mr = 216.10Z = 8
Monoclinic, P21/cMo Kα
a = 19.6325 (11) ŵ = 5.26 mm1
b = 10.6101 (6) ÅT = 296 K
c = 7.8859 (5) Å0.21 × 0.17 × 0.09 mm
β = 100.0780 (10)º
Data collection top
Bruker APEXII CCD
diffractometer
3911 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2008)
2706 reflections with I > 2σ(I)
Tmin = 0.384, Tmax = 0.620Rint = 0.025
12968 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.035181 parameters
wR(F2) = 0.087H-atom parameters constrained
S = 1.03Δρmax = 0.82 e Å3
3911 reflectionsΔρmin = 0.77 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 > 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) top
xyzUiso*/Ueq
Br20.315314 (16)0.36346 (4)0.36641 (5)0.07035 (13)
Br10.538072 (18)0.69050 (5)1.27120 (5)0.08477 (16)
S20.04123 (4)0.26135 (7)0.39188 (10)0.05003 (18)
S10.21328 (4)0.52885 (7)0.75427 (10)0.05230 (19)
N20.03383 (11)0.4881 (2)0.2688 (3)0.0473 (6)
H2A0.01190.55150.23670.057*
H2B0.07800.49160.26230.057*
C10.23831 (13)0.6495 (2)0.8875 (3)0.0412 (6)
C90.07643 (12)0.3842 (2)0.3369 (3)0.0342 (5)
C120.21855 (13)0.3743 (3)0.3549 (3)0.0429 (6)
C100.10919 (14)0.4633 (2)0.2364 (4)0.0459 (6)
H10A0.08310.52000.16180.055*
C140.11668 (14)0.3004 (3)0.4448 (3)0.0474 (7)
H14A0.09560.24660.51310.057*
C50.44606 (15)0.6804 (3)1.1491 (4)0.0558 (8)
C80.00020 (13)0.3859 (2)0.3280 (3)0.0370 (5)
C130.18748 (14)0.2945 (3)0.4535 (4)0.0515 (7)
H13A0.21370.23660.52600.062*
C110.18020 (15)0.4589 (3)0.2457 (4)0.0498 (7)
H11A0.20180.51270.17850.060*
N10.19425 (12)0.7375 (2)0.9174 (3)0.0554 (6)
H1A0.20820.79850.98670.067*
H1B0.15170.73380.86750.067*
C20.31088 (13)0.6623 (2)0.9781 (3)0.0408 (6)
C60.40650 (16)0.7873 (3)1.1197 (4)0.0622 (8)
H6A0.42500.86541.15630.075*
C30.35274 (15)0.5562 (3)1.0060 (4)0.0549 (7)
H3A0.33510.47830.96590.066*
C70.33903 (15)0.7780 (3)1.0352 (4)0.0540 (7)
H7A0.31190.85021.01620.065*
C40.42000 (16)0.5644 (3)1.0919 (4)0.0639 (9)
H4A0.44750.49261.11100.077*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br20.03962 (17)0.0895 (3)0.0834 (3)0.00005 (15)0.01476 (15)0.00159 (19)
Br10.04511 (19)0.1196 (4)0.0842 (3)0.00878 (19)0.00386 (16)0.0108 (2)
S20.0434 (4)0.0390 (4)0.0685 (5)0.0063 (3)0.0120 (3)0.0056 (3)
S10.0465 (4)0.0459 (4)0.0626 (5)0.0022 (3)0.0043 (3)0.0081 (3)
N20.0398 (12)0.0358 (12)0.0667 (15)0.0016 (9)0.0101 (11)0.0030 (11)
C10.0427 (14)0.0402 (14)0.0415 (14)0.0002 (11)0.0096 (11)0.0055 (11)
C90.0400 (13)0.0271 (12)0.0358 (13)0.0022 (10)0.0076 (10)0.0035 (10)
C120.0405 (14)0.0435 (15)0.0448 (15)0.0022 (12)0.0078 (11)0.0071 (12)
C100.0485 (15)0.0347 (14)0.0566 (17)0.0078 (12)0.0150 (12)0.0086 (12)
C140.0444 (15)0.0515 (17)0.0459 (15)0.0021 (12)0.0067 (12)0.0152 (13)
C50.0392 (15)0.078 (2)0.0497 (17)0.0057 (15)0.0057 (12)0.0030 (15)
C80.0428 (13)0.0305 (13)0.0375 (13)0.0018 (10)0.0065 (10)0.0057 (10)
C130.0420 (15)0.0607 (18)0.0499 (16)0.0040 (13)0.0023 (12)0.0138 (14)
C110.0552 (17)0.0372 (15)0.0628 (18)0.0003 (13)0.0261 (14)0.0071 (13)
N10.0442 (13)0.0528 (15)0.0659 (16)0.0090 (11)0.0004 (11)0.0115 (12)
C20.0395 (13)0.0418 (15)0.0420 (14)0.0003 (11)0.0099 (11)0.0036 (11)
C60.0509 (18)0.063 (2)0.072 (2)0.0100 (15)0.0088 (15)0.0202 (17)
C30.0483 (16)0.0439 (16)0.069 (2)0.0015 (13)0.0022 (14)0.0035 (14)
C70.0518 (17)0.0471 (17)0.0633 (19)0.0007 (13)0.0108 (14)0.0083 (14)
C40.0477 (17)0.058 (2)0.082 (2)0.0054 (15)0.0008 (15)0.0080 (17)
Geometric parameters (Å, °) top
Br2—C121.890 (3)C14—C131.381 (4)
Br1—C51.896 (3)C14—H14A0.9300
S2—C81.675 (3)C5—C61.371 (5)
S1—C11.674 (3)C5—C41.379 (5)
N2—C81.316 (3)C13—H13A0.9300
N2—H2A0.8600C11—H11A0.9300
N2—H2B0.8600N1—H1A0.8600
C1—N11.322 (3)N1—H1B0.8600
C1—C21.484 (4)C2—C31.388 (4)
C9—C141.380 (3)C2—C71.389 (4)
C9—C101.388 (3)C6—C71.378 (4)
C9—C81.486 (3)C6—H6A0.9300
C12—C131.364 (4)C3—C41.377 (4)
C12—C111.373 (4)C3—H3A0.9300
C10—C111.384 (4)C7—H7A0.9300
C10—H10A0.9300C4—H4A0.9300
C8—N2—H2A120.0C12—C13—C14119.3 (3)
C8—N2—H2B120.0C12—C13—H13A120.3
H2A—N2—H2B120.0C14—C13—H13A120.3
N1—C1—C2116.9 (2)C12—C11—C10119.5 (3)
N1—C1—S1121.5 (2)C12—C11—H11A120.3
C2—C1—S1121.58 (19)C10—C11—H11A120.3
C14—C9—C10118.0 (2)C1—N1—H1A120.0
C14—C9—C8120.0 (2)C1—N1—H1B120.0
C10—C9—C8122.0 (2)H1A—N1—H1B120.0
C13—C12—C11120.8 (3)C3—C2—C7118.3 (3)
C13—C12—Br2118.7 (2)C3—C2—C1119.6 (2)
C11—C12—Br2120.4 (2)C7—C2—C1122.1 (2)
C11—C10—C9120.8 (2)C5—C6—C7119.3 (3)
C11—C10—H10A119.6C5—C6—H6A120.3
C9—C10—H10A119.6C7—C6—H6A120.3
C9—C14—C13121.5 (2)C4—C3—C2121.1 (3)
C9—C14—H14A119.2C4—C3—H3A119.4
C13—C14—H14A119.2C2—C3—H3A119.4
C6—C5—C4121.1 (3)C6—C7—C2121.0 (3)
C6—C5—Br1120.0 (2)C6—C7—H7A119.5
C4—C5—Br1118.9 (2)C2—C7—H7A119.5
N2—C8—C9118.1 (2)C3—C4—C5119.1 (3)
N2—C8—S2120.9 (2)C3—C4—H4A120.5
C9—C8—S2120.96 (18)C5—C4—H4A120.5
C3—C1—C2—S123.6 (3)C14—C8—C9—S220.5 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···S2i0.862.733.583 (2)172
N2—H2B···S1ii0.862.653.500 (2)173
N1—H1A···S1iii0.862.783.605 (3)160
N1—H1B···S2ii0.862.713.523 (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.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N2—H2A···S2i0.862.733.583 (2)172
N2—H2B···S1ii0.862.653.500 (2)173
N1—H1A···S1iii0.862.783.605 (3)160
N1—H1B···S2ii0.862.713.523 (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.
Acknowledgements top

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.

references
References top

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