organic compounds
N-(2-Bromophenyl)thiourea
aSchool of Chemical Sciences and Food Technology, Universiti Kebangsaan Malaysia, UKM 43600 Bangi Selangor, Malaysia
*Correspondence e-mail: bohari@ukm.my
In the title compound, C7H7BrN2S, the thiourea unit is almost perpendicular to the bromobenzene fragment, making a dihedral angle of 80.82 (16)°. The is stabilized by N—H⋯S intermolecular hydrogen bonds, which form linear chains along the ab diagonal.
Related literature
For bond-length data, see: Allen et al. (1987). For related structures, see: Steiner (1998); Shen & Xu (2004); Wang et al. (1991). For the antiviral activity of phenylthioureas, see: D'Cruz & Uckun (2005); Frank & Smith (1955); Mao et al. (2000); Sudbeck et al. (1998).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2000); cell SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-32 for Windows (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXTL (Sheldrick, 2008), PARST (Nardelli, 1995) and PLATON.
Supporting information
10.1107/S1600536810008305/dn2543sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810008305/dn2543Isup2.hkl
The compound was prepared by the method described by Frank & Smith (1955) with a slight modification. Ammonium thiocyante (0.38 g, 0.005 mol) in 15 ml acetone was added into 20 ml acetone solution of containing benzoylchloride (0.70 g, 0.005 mole). The solution was filtered and the filtrate was kept into a 100 ml two neck round bottom flask. o-Bromoaniline (0.86 g, 0.005 mole) was added into the flask and the mixture was refluxed for 2 hours. The final solution was poured into a baker containing some ice cubes. The precipitate formed was filtered. The precipitate was then added into a beaker containing 50 ml aqueous solution of sodium hydroxide (7 g). The solution was heated to boiling for 10 minutes. After a week on standing at room temperature some colourless crystals were obtained and found suitable for X-ray investigation. The yield was 81% and melting point; 428.1-429.3 K.
H atoms on the C atoms were positioned geometrically with C—H= 0.93 for aromatic group and constrained to ride on their parent atoms with Uiso(H)= 1.2 x Ueq(C parent atom). The hydrogen atoms attached to the nitrogen atoms were located from the Fourier map and initially refined with Uiso(H)= 1.2 x Ueq(N) . In the last stage of
they were treated as riding on their parent N atoms.Data collection: SMART (Bruker, 2000); cell
SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-32 for Windows (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXTL (Sheldrick, 2008), PARST (Nardelli, 1995) and PLATON (Spek, 2009).C7H7BrN2S | F(000) = 912 |
Mr = 231.12 | Dx = 1.695 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 1400 reflections |
a = 15.181 (3) Å | θ = 2.6–27.0° |
b = 7.7952 (16) Å | µ = 4.71 mm−1 |
c = 15.312 (3) Å | T = 298 K |
β = 90.803 (4)° | Block, colourless |
V = 1811.8 (6) Å3 | 0.44 × 0.27 × 0.11 mm |
Z = 8 |
Bruker SMART APEX CCD area-detector diffractometer | 1972 independent reflections |
Radiation source: fine-focus sealed tube | 1327 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.028 |
Detector resolution: 83.66 pixels mm-1 | θmax = 27.0°, θmin = 2.6° |
ω scan | h = −19→19 |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | k = −5→9 |
Tmin = 0.231, Tmax = 0.625 | l = −19→19 |
5817 measured reflections |
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)] = 0.046 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.129 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0664P)2 + 1.1624P] where P = (Fo2 + 2Fc2)/3 |
1972 reflections | (Δ/σ)max < 0.001 |
100 parameters | Δρmax = 0.61 e Å−3 |
0 restraints | Δρmin = −0.65 e Å−3 |
C7H7BrN2S | V = 1811.8 (6) Å3 |
Mr = 231.12 | Z = 8 |
Monoclinic, C2/c | Mo Kα radiation |
a = 15.181 (3) Å | µ = 4.71 mm−1 |
b = 7.7952 (16) Å | T = 298 K |
c = 15.312 (3) Å | 0.44 × 0.27 × 0.11 mm |
β = 90.803 (4)° |
Bruker SMART APEX CCD area-detector diffractometer | 1972 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | 1327 reflections with I > 2σ(I) |
Tmin = 0.231, Tmax = 0.625 | Rint = 0.028 |
5817 measured reflections |
R[F2 > 2σ(F2)] = 0.046 | 0 restraints |
wR(F2) = 0.129 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.61 e Å−3 |
1972 reflections | Δρmin = −0.65 e Å−3 |
100 parameters |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 | ||
Br1 | 0.10527 (4) | 1.16677 (8) | 0.59724 (3) | 0.0909 (3) | |
S1 | 0.13874 (6) | 0.57559 (13) | 0.47185 (6) | 0.0488 (3) | |
N1 | 0.16731 (19) | 0.7869 (4) | 0.60361 (19) | 0.0498 (8) | |
H1A | 0.2173 | 0.7961 | 0.5790 | 0.060* | |
N2 | 0.0356 (2) | 0.6495 (5) | 0.6038 (2) | 0.0660 (11) | |
H2A | −0.0030 | 0.5879 | 0.5780 | 0.079* | |
H2B | 0.0218 | 0.7159 | 0.6460 | 0.079* | |
C1 | 0.1703 (3) | 0.7627 (6) | 0.7636 (3) | 0.0565 (10) | |
H1 | 0.1868 | 0.6482 | 0.7587 | 0.068* | |
C2 | 0.1620 (3) | 0.8362 (6) | 0.8439 (3) | 0.0648 (12) | |
H2 | 0.1754 | 0.7731 | 0.8939 | 0.078* | |
C3 | 0.1338 (3) | 1.0031 (7) | 0.8512 (3) | 0.0661 (12) | |
H3 | 0.1267 | 1.0510 | 0.9063 | 0.079* | |
C4 | 0.1163 (3) | 1.0993 (6) | 0.7788 (3) | 0.0645 (11) | |
H4 | 0.0972 | 1.2122 | 0.7845 | 0.077* | |
C5 | 0.1267 (2) | 1.0289 (5) | 0.6969 (2) | 0.0511 (9) | |
C6 | 0.1536 (2) | 0.8622 (5) | 0.6873 (2) | 0.0447 (9) | |
C7 | 0.1116 (2) | 0.6777 (4) | 0.5653 (2) | 0.0422 (8) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.1262 (6) | 0.0874 (4) | 0.0595 (3) | 0.0326 (3) | 0.0145 (3) | 0.0182 (3) |
S1 | 0.0499 (5) | 0.0498 (5) | 0.0472 (5) | −0.0151 (4) | 0.0139 (4) | −0.0146 (4) |
N1 | 0.0425 (17) | 0.0608 (19) | 0.0465 (17) | −0.0151 (15) | 0.0159 (14) | −0.0186 (15) |
N2 | 0.0445 (18) | 0.087 (3) | 0.067 (2) | −0.0264 (18) | 0.0218 (16) | −0.036 (2) |
C1 | 0.052 (2) | 0.057 (2) | 0.060 (2) | 0.004 (2) | 0.0012 (19) | −0.008 (2) |
C2 | 0.072 (3) | 0.077 (3) | 0.045 (2) | −0.010 (2) | 0.005 (2) | 0.007 (2) |
C3 | 0.080 (3) | 0.076 (3) | 0.042 (2) | −0.014 (3) | 0.011 (2) | −0.013 (2) |
C4 | 0.084 (3) | 0.056 (2) | 0.054 (2) | 0.001 (2) | 0.016 (2) | −0.014 (2) |
C5 | 0.056 (2) | 0.055 (2) | 0.0418 (19) | −0.0019 (19) | 0.0074 (17) | −0.0036 (17) |
C6 | 0.0402 (19) | 0.054 (2) | 0.0403 (19) | −0.0100 (17) | 0.0091 (15) | −0.0098 (16) |
C7 | 0.0391 (19) | 0.044 (2) | 0.0440 (18) | −0.0072 (15) | 0.0077 (15) | −0.0072 (15) |
Br1—C5 | 1.891 (4) | C1—C6 | 1.421 (6) |
S1—C7 | 1.693 (4) | C1—H1 | 0.9300 |
N1—C7 | 1.331 (4) | C2—C3 | 1.375 (7) |
N1—C6 | 1.428 (4) | C2—H2 | 0.9300 |
N1—H1A | 0.8551 | C3—C4 | 1.361 (6) |
N2—C7 | 1.320 (4) | C3—H3 | 0.9300 |
N2—H2A | 0.8506 | C4—C5 | 1.380 (5) |
N2—H2B | 0.8562 | C4—H4 | 0.9300 |
C1—C2 | 1.364 (6) | C5—C6 | 1.371 (5) |
C7—N1—C6 | 124.0 (3) | C2—C3—H3 | 119.6 |
C7—N1—H1A | 115.0 | C3—C4—C5 | 119.8 (4) |
C6—N1—H1A | 120.1 | C3—C4—H4 | 120.1 |
C7—N2—H2A | 119.1 | C5—C4—H4 | 120.1 |
C7—N2—H2B | 117.4 | C6—C5—C4 | 120.8 (4) |
H2A—N2—H2B | 121.2 | C6—C5—Br1 | 120.0 (3) |
C2—C1—C6 | 119.6 (4) | C4—C5—Br1 | 119.1 (3) |
C2—C1—H1 | 120.2 | C5—C6—C1 | 118.6 (3) |
C6—C1—H1 | 120.2 | C5—C6—N1 | 122.2 (4) |
C1—C2—C3 | 120.2 (4) | C1—C6—N1 | 119.1 (3) |
C1—C2—H2 | 119.9 | N2—C7—N1 | 117.6 (3) |
C3—C2—H2 | 119.9 | N2—C7—S1 | 121.6 (3) |
C4—C3—C2 | 120.9 (4) | N1—C7—S1 | 120.8 (3) |
C4—C3—H3 | 119.6 | ||
C6—C1—C2—C3 | 2.9 (6) | Br1—C5—C6—N1 | 0.6 (5) |
C1—C2—C3—C4 | −1.9 (7) | C2—C1—C6—C5 | −2.1 (6) |
C2—C3—C4—C5 | 0.0 (7) | C2—C1—C6—N1 | 176.5 (4) |
C3—C4—C5—C6 | 0.8 (6) | C7—N1—C6—C5 | −103.7 (4) |
C3—C4—C5—Br1 | −178.2 (3) | C7—N1—C6—C1 | 77.7 (5) |
C4—C5—C6—C1 | 0.2 (6) | C6—N1—C7—N2 | 6.2 (6) |
Br1—C5—C6—C1 | 179.2 (3) | C6—N1—C7—S1 | −172.3 (3) |
C4—C5—C6—N1 | −178.3 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···S1i | 0.86 | 2.54 | 3.354 (3) | 161 |
N2—H2A···S1ii | 0.85 | 2.53 | 3.368 (3) | 168 |
Symmetry codes: (i) −x+1/2, −y+3/2, −z+1; (ii) −x, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C7H7BrN2S |
Mr | 231.12 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 298 |
a, b, c (Å) | 15.181 (3), 7.7952 (16), 15.312 (3) |
β (°) | 90.803 (4) |
V (Å3) | 1811.8 (6) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 4.71 |
Crystal size (mm) | 0.44 × 0.27 × 0.11 |
Data collection | |
Diffractometer | Bruker SMART APEX CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2000) |
Tmin, Tmax | 0.231, 0.625 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5817, 1972, 1327 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.046, 0.129, 1.06 |
No. of reflections | 1972 |
No. of parameters | 100 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.61, −0.65 |
Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-32 for Windows (Farrugia, 1997) and PLATON (Spek, 2009), SHELXTL (Sheldrick, 2008), PARST (Nardelli, 1995) and PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···S1i | 0.86 | 2.54 | 3.354 (3) | 160.5 |
N2—H2A···S1ii | 0.85 | 2.53 | 3.368 (3) | 167.6 |
Symmetry codes: (i) −x+1/2, −y+3/2, −z+1; (ii) −x, −y+1, −z+1. |
Acknowledgements
The authors thank the Ministry of Higher Education of Malaysia and Universiti Kebangsaan Malaysia for the research grant UKM-GUP-NBT-68–27/110. A scholarship from the Libyan Government to SFH is greatly appreciated.
References
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The number of publications including patents on the application of thiourea compounds in the field of pharmaceutical is increasing at a considerable rate. The antivarial activities of a series of phenylthioureas as none-nucleoside inhibitors HIV-1 reverse transcriptase (NNRTIs) with efficacy against multi-drug resistant viruses (Sudbeck et al., 1998; Mao et al., 2000; D'Cruz & Uckun, 2005) are some of the interesting examples. Several N-thiourea compounds of the type H2NC(S)NHR are now commercially available.
The title compound (I) is analagous to phenylthiourea (II, Shen et al., 2004), o-fluorophenylthiourea (III, Steiner, 1998) and p-bromophenylthiourea(IV, Wang et al., 1991). The thiourea moiety, S1/N1/N2/C7, and the 2-bromoaniline fragment, Br1/N1/(C1—C6) are each planar with maximum deviation of 0.024 (5)Å for C2 atom from the least square plane. The two planes are perpendicular to each other with dihedral angle of 80.82 (16)° compare to 68.57° in (IV). The thiourea moiety maintains its cis-trans geometry. The bond lengths and angles are in normal ranges (Allen et al., 1987) and comparable to those in (II), (III) and (IV). In contrast to its fluoro- analog ,the molecule is stablized only by pairs of N1—H1A···S1 and N2—H2A···S1 (symmetry codes as in Table 1) intermolecular hydrogen bonds to form linear chains along the diagnal of the ab face (Fig.2).