organic compounds
4-Bromo-2-chloroaniline
aThe Key Laboratory for Chemical Biology of Fujian Province, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen, Fujian 361005, People's Republic of China
*Correspondence e-mail: yejl@xmu.edu.cn
The title compound, C6H5BrClN, is almost planar (r.m.s. deviation = 0.018 Å). In the crystal, molecules are linked by intermolecular N—H⋯N and weak N—H⋯Br hydrogen bonds, generating sheets.
Related literature
For background to halogentaed aromatic compounds, see: Katritzky et al. (1994). For related structures, see: Cox (2001); Parkin et al. (2005); Ng (2005); Ferguson et al. (1998). For the synthesis, see: Ault & Kraig (1966).
Experimental
Crystal data
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Data collection: SMART (Bruker, 2001); cell SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536809054944/hb5285sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809054944/hb5285Isup2.hkl
The tiltle compound was prepared according to a previously reported method (Ault & Kraig, 1966). Colourless needles of (I) were obtained by slow evaporation of a petroleum ether solution.
The hydrogen atoms were positioned geometrically, with C—H = 0.93, 0.98, 0.97 and 0.96 Å for phenyl, methine, methylene and methyl H atoms, respectively, and were included in the
in the riding model approximation. The displacement parameters of methyl H atoms were set to 1.5Ueq(C), while those of other H atoms were set to 1.2Ueq(C). In the absence of significant effects, Friedel pairs were merged.Data collection: SMART (Bruker, 2001); cell
SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).C6H5BrClN | F(000) = 424 |
Mr = 206.47 | Dx = 1.965 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 1199 reflections |
a = 10.965 (4) Å | θ = 2.3–29.8° |
b = 15.814 (6) Å | µ = 6.17 mm−1 |
c = 4.0232 (15) Å | T = 298 K |
V = 697.7 (4) Å3 | Needle, colourless |
Z = 4 | 0.7 × 0.19 × 0.15 mm |
Bruker SMART CCD diffractometer | 1710 independent reflections |
Radiation source: fine-focus sealed tube | 1333 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.044 |
ϕ and ω scan | θmax = 29.8°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −14→14 |
Tmin = 0.254, Tmax = 0.396 | k = −20→21 |
5799 measured reflections | l = −5→5 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.033 | w = 1/[σ2(Fo2) + (0.0374P)2] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.081 | (Δ/σ)max = 0.008 |
S = 0.99 | Δρmax = 0.33 e Å−3 |
1710 reflections | Δρmin = −0.48 e Å−3 |
83 parameters | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.246 (8) |
Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983), 511 Friedel pairs |
Secondary atom site location: difference Fourier map | Absolute structure parameter: 0.035 (15) |
C6H5BrClN | V = 697.7 (4) Å3 |
Mr = 206.47 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 10.965 (4) Å | µ = 6.17 mm−1 |
b = 15.814 (6) Å | T = 298 K |
c = 4.0232 (15) Å | 0.7 × 0.19 × 0.15 mm |
Bruker SMART CCD diffractometer | 1710 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | 1333 reflections with I > 2σ(I) |
Tmin = 0.254, Tmax = 0.396 | Rint = 0.044 |
5799 measured reflections |
R[F2 > 2σ(F2)] = 0.033 | H-atom parameters constrained |
wR(F2) = 0.081 | Δρmax = 0.33 e Å−3 |
S = 0.99 | Δρmin = −0.48 e Å−3 |
1710 reflections | Absolute structure: Flack (1983), 511 Friedel pairs |
83 parameters | Absolute structure parameter: 0.035 (15) |
0 restraints |
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 > 2sigma(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 | 0.28337 (3) | 0.74386 (2) | 0.51936 (10) | 0.0646 (2) | |
Cl1 | 0.42519 (8) | 0.41363 (5) | 0.4648 (3) | 0.0588 (3) | |
C1 | 0.3957 (3) | 0.65802 (18) | 0.6258 (8) | 0.0432 (7) | |
C2 | 0.4999 (3) | 0.6770 (2) | 0.7973 (9) | 0.0494 (8) | |
H2A | 0.5151 | 0.7322 | 0.8656 | 0.059* | |
C3 | 0.5812 (3) | 0.6145 (2) | 0.8673 (9) | 0.0456 (8) | |
H3A | 0.6518 | 0.6276 | 0.9846 | 0.055* | |
C4 | 0.5613 (3) | 0.5320 (2) | 0.7681 (8) | 0.0428 (8) | |
C5 | 0.4548 (3) | 0.51544 (19) | 0.5957 (8) | 0.0395 (7) | |
C6 | 0.3728 (2) | 0.57746 (17) | 0.5249 (7) | 0.0431 (7) | |
H6A | 0.3018 | 0.5649 | 0.4087 | 0.052* | |
N1 | 0.6464 (2) | 0.47087 (18) | 0.8346 (8) | 0.0565 (8) | |
H1A | 0.7124 | 0.4838 | 0.9383 | 0.068* | |
H1B | 0.6338 | 0.4196 | 0.7726 | 0.068* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0770 (3) | 0.0451 (2) | 0.0717 (3) | 0.01789 (15) | −0.0064 (2) | 0.0025 (2) |
Cl1 | 0.0638 (5) | 0.0349 (4) | 0.0776 (6) | −0.0034 (3) | −0.0023 (5) | −0.0047 (5) |
C1 | 0.0509 (17) | 0.0347 (16) | 0.0438 (16) | 0.0061 (14) | 0.0043 (14) | 0.0027 (13) |
C2 | 0.0582 (18) | 0.0357 (18) | 0.054 (2) | −0.0081 (15) | 0.0075 (16) | −0.0027 (15) |
C3 | 0.0368 (15) | 0.0481 (19) | 0.0520 (18) | −0.0064 (14) | −0.0002 (14) | −0.0008 (15) |
C4 | 0.0399 (16) | 0.0430 (18) | 0.0455 (18) | 0.0005 (14) | 0.0086 (14) | 0.0040 (13) |
C5 | 0.0416 (15) | 0.0344 (15) | 0.0424 (16) | −0.0028 (12) | 0.0053 (13) | 0.0012 (12) |
C6 | 0.0424 (14) | 0.0406 (15) | 0.0461 (16) | −0.0022 (12) | −0.0007 (16) | 0.0016 (16) |
N1 | 0.0434 (15) | 0.0500 (17) | 0.076 (2) | 0.0101 (13) | −0.0015 (15) | 0.0006 (15) |
Br1—C1 | 1.883 (3) | C3—H3A | 0.9300 |
Cl1—C5 | 1.725 (3) | C4—N1 | 1.369 (4) |
C1—C6 | 1.361 (4) | C4—C5 | 1.383 (4) |
C1—C2 | 1.368 (5) | C5—C6 | 1.361 (4) |
C2—C3 | 1.361 (5) | C6—H6A | 0.9300 |
C2—H2A | 0.9300 | N1—H1A | 0.8600 |
C3—C4 | 1.382 (4) | N1—H1B | 0.8600 |
C6—C1—C2 | 120.7 (3) | C3—C4—C5 | 117.1 (3) |
C6—C1—Br1 | 119.1 (2) | C6—C5—C4 | 121.8 (3) |
C2—C1—Br1 | 120.2 (2) | C6—C5—Cl1 | 119.0 (2) |
C3—C2—C1 | 119.4 (3) | C4—C5—Cl1 | 119.2 (2) |
C3—C2—H2A | 120.3 | C1—C6—C5 | 119.4 (3) |
C1—C2—H2A | 120.3 | C1—C6—H6A | 120.3 |
C2—C3—C4 | 121.6 (3) | C5—C6—H6A | 120.3 |
C2—C3—H3A | 119.2 | C4—N1—H1A | 120.0 |
C4—C3—H3A | 119.2 | C4—N1—H1B | 120.0 |
N1—C4—C3 | 120.2 (3) | H1A—N1—H1B | 120.0 |
N1—C4—C5 | 122.7 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1B···Br1i | 0.86 | 3.04 | 3.719 (3) | 137 |
N1—H1A···N1ii | 0.86 | 2.34 | 3.172 (4) | 164 |
Symmetry codes: (i) −x+1, y−1/2, −z+3/2; (ii) −x+3/2, −y+1, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C6H5BrClN |
Mr | 206.47 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 298 |
a, b, c (Å) | 10.965 (4), 15.814 (6), 4.0232 (15) |
V (Å3) | 697.7 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 6.17 |
Crystal size (mm) | 0.7 × 0.19 × 0.15 |
Data collection | |
Diffractometer | Bruker SMART CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2001) |
Tmin, Tmax | 0.254, 0.396 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5799, 1710, 1333 |
Rint | 0.044 |
(sin θ/λ)max (Å−1) | 0.698 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.033, 0.081, 0.99 |
No. of reflections | 1710 |
No. of parameters | 83 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.33, −0.48 |
Absolute structure | Flack (1983), 511 Friedel pairs |
Absolute structure parameter | 0.035 (15) |
Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXTL (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1B···Br1i | 0.86 | 3.04 | 3.719 (3) | 137 |
N1—H1A···N1ii | 0.86 | 2.34 | 3.172 (4) | 164 |
Symmetry codes: (i) −x+1, y−1/2, −z+3/2; (ii) −x+3/2, −y+1, z+1/2. |
Acknowledgements
The authors thank the Natural Science Foundation of China (No. 20602028) and the NFFTBS (No. J0630429) for financial support.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Halogenated aromatic compounds is an important class of intermediates for the synthesis of bio-active substances such as antibacterial, antioxidizing, antiviral agents (e.g. Katritzky et al., 1994). Despite their simple structures, the X-ray structures of halogenated aniline compounds periodically were reported, such as 2,5-dichloroaniline (Cox, 2001), 2-iodoaniline (Parkin et al., 2005) and 5-chloro-2-nitroaniline (Ng, 2005). We now report the title compound, (I).
The packing of molecules in the crystal structure is stabilized and linked into a two-dimensional texture by intermolecular N—H···N and N—H···Br hydrogen bonds. The N···N distance is 3.172 (4) Å in hydrogen bond N—H···N, which are similar to that observed in 2,4-dibromo-6- chloroaniline (Ferguson et al., 1998), 3.150 (11) Å and 2-iodoaniline (Parkin et al., 2005), 3.161 (14) Å.