Abstract
In the title compound, C8H6BrNO3, there are two molecules, A and B, in the asymmetric unit. The nitro and ethanone groups lie close to the plane of the benzene ring and the bromine atom is twisted slightly: the dihedral angles between the mean planes of the nitro and ethanone groups and the benzene ring are 4.6 (4) (A) and 2.8 (3) (B), and 0.8 (8) (A) and 5.5 (8)° (B), respectively. An extensive array of weak C—H⋯O hydrogen bonds, π–π ring stacking [centroid–centroid distances = 3.710 (5) and 3.677 (5) Å] and short non-hydrogen Br⋯O and O⋯Br intermolecular interactions [3.16 (6)and 3.06 (8) Å] contribute to the crystal stability, forming a supermolecular three-dimensional network structure along 110. These interactions give rise to a variety of cyclic graph-set motifs and form interconnected sheets in the three-dimensional structure.
Related literature
For the use of α-haloketones in the synthesis of pharmaceuticals, see: Erian et al. (2003 ▶). For related structures, see: Gupta & Prasad (1971 ▶); Sim (1986 ▶); Sutherland & Hoy (1968 ▶, 1969 ▶); Sutherland et al. (1974 ▶); Yathirajan et al. (2007 ▶); Young et al. (1968 ▶). For cyclic graph-set motifs, see: Etter (1990 ▶). For reference bond-length data, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C8H6BrNO3
M r = 244.05
Triclinic,
a = 8.8259 (7) Å
b = 8.8651 (8) Å
c = 11.6775 (8) Å
α = 74.691 (7)°
β = 75.174 (7)°
γ = 78.681 (7)°
V = 843.76 (12) Å3
Z = 4
Cu Kα radiation
μ = 6.45 mm−1
T = 123 K
0.75 × 0.62 × 0.19 mm
Data collection
Oxford Diffraction Xcalibur Ruby Gemini diffractometer
Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2007 ▶) T min = 0.066, T max = 0.389
4708 measured reflections
3215 independent reflections
3023 reflections with I > 2σ(I)
R int = 0.053
Refinement
R[F 2 > 2σ(F 2)] = 0.090
wR(F 2) = 0.248
S = 1.12
3215 reflections
235 parameters
H-atom parameters constrained
Δρmax = 2.39 e Å−3
Δρmin = −1.83 e Å−3
Data collection: CrysAlis PRO (Oxford Diffraction, 2007 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis RED (Oxford Diffraction, 2007 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶)); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810049585/sj5067sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049585/sj5067Isup2.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 |
|---|---|---|---|---|
| C4A—H4AA⋯O1Bi | 0.95 | 2.49 | 3.314 (10) | 145 |
| C5A—H5AA⋯Br2ii | 0.95 | 3.04 | 3.849 (8) | 144 |
| C5A—H5AA⋯O2Bi | 0.95 | 2.55 | 3.409 (11) | 150 |
| C6A—H6AA⋯O3Bii | 0.95 | 2.38 | 3.320 (10) | 171 |
| C4B—H4BA⋯O1Aiii | 0.95 | 2.56 | 3.420 (9) | 150 |
| C6B—H6BA⋯O3A | 0.95 | 2.35 | 3.278 (10) | 165 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
ASP thanks the University of Mysore (UOM) for research facilities and HSY thanks UOM for sabbatical leave. RJB acknowledges the NSF MRI program (grant No. CHE-0619278) for funds to purchase an X-ray diffractometer.
supplementary crystallographic information
Comment
α-Haloketones have been attracting increasing attention in view of their high reactivity as building blocks for the preparation of compounds of various classes due to their selective transformations with different reagents. The α-haloketones can be particularly promising synthons in combinatorial synthesis of functionalized carbo- and heterocyclic compounds used in the design of novel highly effective pharmaceuticals with a broad spectrum of bioresponses (Erian et al., 2003). Crystal structures of some acetyl biphenyl derivatives viz., 4-acetyl-2'-fluorobiphenyl (Young et al., 1968), 4-acetyl-2'-chlorobiphenyl (Sutherland & Hoy, 1968), 4-acetyl-3'-bromobiphenyl (Sutherland & Hoy, 1969), 4-acetyl-2'-nitrobiphenyl (Sutherland et al., 1974), α-bromoacetophenone (Gupta & Prasad, 1971), 2-Bromo-4'-phenylacetophenone (Sim, 1986 ) and methyl 4-(bromomethyl)benzoate (Yathirajan et al.2007) have been reported. In view of the importance of the α-haloketones, the title compound, (I), has been prepared and its crystal structure is reported.
In the title compound, C8H6BrNO3, two molecules crystallize in the asymmetric unit (Fig. 2). The nitro and ethanone groups are planar with the benzene ring and the bromine atom is twisted slightly (Torsion angles C1A/C7A/C8A/Br1 = -177.5 (5)° and C1B/C7B/C8B/Br2 = 168.6 (5)°. Bond distances and angles are in normal ranges (Allen et al., 1987). An extensive array of weak C—H···O and C—H···Br hydrogen bonds (Table 1), π–π ring stacking (Table 2) and short non-hydrogen, Br···O and O···Br, intermolecular interactions (Table 3) contribute to crystal stability forming a supermolecular 3-dimensional network structure along 110 (Fig. 3). These interactions give rise to a variety of cyclic graph-set motifs (R31(3), R22(7), R22(8), R33(12), R33(18)), Fig. 3, (Etter, 1990) and form interconnected sheets in the three-dimensional structure.
Experimental
To a stirred solution of 1-(3-nitrophenyl)ethanone (1 g, 6.05 mmol) in chloroform (10 ml), bromine (0.97 g, 6.05 mmol) was added at 0–5°C (Fig. 1). The reaction mixture was stirred at room temperature for 2 h, poured into ice cold water and layers were separated. The organic layer was washed with water (1 x 10 ml), 10% aq.sodium bicarbonate solution (1 x 10 ml) and brine (1 x 10 ml), dried over Na2SO4 and concentrated under reduced pressure. The crude product was purified by column chromatography in silca gel (230–400 mesh) using 0–10% petroleum ether and ethyl acetate as the elutant. Single crystals were grown from THF by the slow evaporation method with a yield of 96% (m.p.365–367 K).
Refinement
All of the H atoms were placed in their calculated positions and refined using the riding model with Atom—H lengths of 0.95Å (CH) or 0.99Å (CH2). Isotropic displacement parameters for these atoms were set to 1.19–1.22 (CH) or 1.18–1.20 (CH2) times Ueq of the parent atom.
Figures
Fig. 1.
Molecular structure of the title compound showing the atom labeling scheme and 50% probability displacement ellipsoids. Dashed lines indicate weak C—H···O intermolecular hydrogen bonds between two molecules in the asymmetric unit.
Fig. 2.
Packing diagram of the title compound viewed down the a axis. Dashed lines indicate weak C—H···O and C—H···Br hydrogen bonds and short non-hydrogen, Br···O and O···Br, intermolecular interactions creating a 3-D supramolecular structure along 110.
Fig. 3.
A planar sheet of C8H6BrNO3 molecules connected by weak C—H···O and C—H···Br hydrogen bonds and short non-hydrogen, Br···O and O···Br intermolecular interactions. These patterns are shown by cyclic graph-set motif analysis (R31(3), R22(7), R22(8), R33(12), R33(18)) in an extended 2-dimensional array.
Crystal data
| C8H6BrNO3 | Z = 4 |
| Mr = 244.05 | F(000) = 480 |
| Triclinic, P1 | Dx = 1.921 Mg m−3 |
| Hall symbol: -P 1 | Cu Kα radiation, λ = 1.54178 Å |
| a = 8.8259 (7) Å | Cell parameters from 4487 reflections |
| b = 8.8651 (8) Å | θ = 5.2–74.4° |
| c = 11.6775 (8) Å | µ = 6.45 mm−1 |
| α = 74.691 (7)° | T = 123 K |
| β = 75.174 (7)° | Plate, colorless |
| γ = 78.681 (7)° | 0.75 × 0.62 × 0.19 mm |
| V = 843.76 (12) Å3 |
Data collection
| Oxford Diffraction Xcalibur Ruby Gemini diffractometer | 3215 independent reflections |
| Radiation source: Enhance (Cu) X-ray Source | 3023 reflections with I > 2σ(I) |
| graphite | Rint = 0.053 |
| Detector resolution: 10.5081 pixels mm-1 | θmax = 74.5°, θmin = 5.2° |
| ω scans | h = −10→10 |
| Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2007) | k = −10→11 |
| Tmin = 0.066, Tmax = 0.389 | l = −10→14 |
| 4708 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)] = 0.090 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.248 | H-atom parameters constrained |
| S = 1.12 | w = 1/[σ2(Fo2) + (0.1498P)2 + 8.1184P] where P = (Fo2 + 2Fc2)/3 |
| 3215 reflections | (Δ/σ)max < 0.001 |
| 235 parameters | Δρmax = 2.39 e Å−3 |
| 0 restraints | Δρmin = −1.83 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 | ||
| Br1 | 0.22668 (10) | 0.51160 (10) | 0.93394 (7) | 0.0303 (3) | |
| Br2 | 0.72920 (10) | −0.00313 (10) | 0.49047 (7) | 0.0301 (3) | |
| O1A | 0.4973 (7) | 0.2908 (7) | 0.3052 (5) | 0.0323 (13) | |
| O2A | 0.3515 (9) | 0.4156 (10) | 0.1781 (6) | 0.0471 (17) | |
| O3A | 0.3683 (8) | 0.3750 (8) | 0.7146 (5) | 0.0341 (14) | |
| O1B | 0.9660 (7) | −0.2309 (7) | 1.1190 (6) | 0.0343 (13) | |
| O2B | 0.8390 (10) | −0.0778 (11) | 1.2376 (7) | 0.056 (2) | |
| O3B | 0.8567 (9) | −0.1476 (9) | 0.7169 (6) | 0.0470 (18) | |
| N1A | 0.3867 (8) | 0.3869 (8) | 0.2772 (6) | 0.0279 (14) | |
| N1B | 0.8677 (8) | −0.1185 (9) | 1.1406 (6) | 0.0300 (15) | |
| C1A | 0.2294 (9) | 0.5263 (9) | 0.5648 (7) | 0.0213 (14) | |
| C2A | 0.3214 (9) | 0.4390 (9) | 0.4807 (7) | 0.0230 (15) | |
| H2AA | 0.4027 | 0.3562 | 0.5020 | 0.028* | |
| C3A | 0.2895 (9) | 0.4778 (9) | 0.3663 (7) | 0.0234 (15) | |
| C4A | 0.1708 (9) | 0.5973 (9) | 0.3319 (7) | 0.0260 (16) | |
| H4AA | 0.1522 | 0.6209 | 0.2520 | 0.031* | |
| C5A | 0.0816 (10) | 0.6799 (9) | 0.4154 (8) | 0.0268 (16) | |
| H5AA | −0.0004 | 0.7614 | 0.3936 | 0.032* | |
| C6A | 0.1098 (9) | 0.6459 (9) | 0.5319 (7) | 0.0250 (15) | |
| H6AA | 0.0474 | 0.7044 | 0.5892 | 0.030* | |
| C7A | 0.2640 (9) | 0.4810 (9) | 0.6892 (7) | 0.0231 (15) | |
| C8A | 0.1639 (10) | 0.5758 (9) | 0.7794 (7) | 0.0262 (15) | |
| H8AA | 0.0515 | 0.5626 | 0.7923 | 0.031* | |
| H8AB | 0.1733 | 0.6891 | 0.7451 | 0.031* | |
| C1B | 0.7227 (9) | 0.0124 (9) | 0.8533 (7) | 0.0210 (14) | |
| C2B | 0.8084 (9) | −0.0752 (9) | 0.9417 (7) | 0.0221 (14) | |
| H2BA | 0.8829 | −0.1653 | 0.9282 | 0.027* | |
| C3B | 0.7801 (9) | −0.0256 (9) | 1.0474 (7) | 0.0239 (15) | |
| C4B | 0.6745 (9) | 0.1066 (9) | 1.0720 (7) | 0.0258 (16) | |
| H4BA | 0.6607 | 0.1374 | 1.1464 | 0.031* | |
| C5B | 0.5909 (10) | 0.1913 (9) | 0.9858 (8) | 0.0272 (16) | |
| H5BA | 0.5175 | 0.2816 | 1.0005 | 0.033* | |
| C6B | 0.6136 (9) | 0.1452 (8) | 0.8766 (7) | 0.0224 (15) | |
| H6BA | 0.5548 | 0.2039 | 0.8176 | 0.027* | |
| C7B | 0.7549 (9) | −0.0401 (9) | 0.7370 (7) | 0.0252 (15) | |
| C8B | 0.6500 (9) | 0.0468 (10) | 0.6461 (7) | 0.0249 (15) | |
| H8BA | 0.6431 | 0.1621 | 0.6367 | 0.030* | |
| H8BB | 0.5418 | 0.0182 | 0.6791 | 0.030* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1 | 0.0385 (5) | 0.0349 (5) | 0.0186 (5) | −0.0091 (4) | −0.0038 (3) | −0.0072 (3) |
| Br2 | 0.0404 (6) | 0.0338 (5) | 0.0163 (5) | −0.0076 (4) | −0.0030 (3) | −0.0075 (3) |
| O1A | 0.041 (3) | 0.029 (3) | 0.022 (3) | 0.000 (3) | 0.000 (2) | −0.008 (2) |
| O2A | 0.055 (4) | 0.064 (5) | 0.027 (3) | 0.004 (3) | −0.015 (3) | −0.022 (3) |
| O3A | 0.040 (3) | 0.037 (3) | 0.022 (3) | 0.007 (3) | −0.010 (2) | −0.007 (2) |
| O1B | 0.041 (3) | 0.032 (3) | 0.030 (3) | 0.002 (3) | −0.015 (3) | −0.006 (2) |
| O2B | 0.073 (5) | 0.071 (5) | 0.024 (3) | 0.021 (4) | −0.019 (3) | −0.025 (3) |
| O3B | 0.063 (4) | 0.055 (4) | 0.020 (3) | 0.018 (4) | −0.014 (3) | −0.019 (3) |
| N1A | 0.032 (3) | 0.031 (3) | 0.019 (3) | −0.010 (3) | 0.005 (3) | −0.008 (3) |
| N1B | 0.034 (4) | 0.038 (4) | 0.018 (3) | −0.008 (3) | −0.006 (3) | −0.003 (3) |
| C1A | 0.023 (3) | 0.024 (3) | 0.018 (4) | −0.009 (3) | −0.002 (3) | −0.004 (3) |
| C2A | 0.025 (4) | 0.023 (4) | 0.018 (4) | −0.007 (3) | 0.002 (3) | −0.003 (3) |
| C3A | 0.025 (4) | 0.026 (4) | 0.018 (4) | −0.011 (3) | 0.002 (3) | −0.005 (3) |
| C4A | 0.031 (4) | 0.024 (4) | 0.020 (4) | −0.012 (3) | −0.004 (3) | 0.003 (3) |
| C5A | 0.031 (4) | 0.021 (4) | 0.027 (4) | −0.006 (3) | −0.010 (3) | 0.002 (3) |
| C6A | 0.027 (4) | 0.025 (4) | 0.023 (4) | −0.008 (3) | −0.004 (3) | −0.003 (3) |
| C7A | 0.028 (4) | 0.019 (3) | 0.021 (4) | −0.007 (3) | −0.005 (3) | −0.002 (3) |
| C8A | 0.035 (4) | 0.026 (4) | 0.018 (4) | 0.001 (3) | −0.008 (3) | −0.006 (3) |
| C1B | 0.025 (3) | 0.021 (3) | 0.016 (3) | −0.004 (3) | −0.002 (3) | −0.004 (3) |
| C2B | 0.023 (3) | 0.024 (4) | 0.017 (3) | −0.006 (3) | 0.000 (3) | −0.003 (3) |
| C3B | 0.025 (4) | 0.027 (4) | 0.017 (4) | −0.006 (3) | −0.002 (3) | −0.001 (3) |
| C4B | 0.033 (4) | 0.028 (4) | 0.015 (3) | −0.012 (3) | 0.005 (3) | −0.007 (3) |
| C5B | 0.028 (4) | 0.025 (4) | 0.025 (4) | −0.006 (3) | 0.004 (3) | −0.008 (3) |
| C6B | 0.027 (4) | 0.018 (3) | 0.018 (3) | −0.003 (3) | −0.001 (3) | 0.001 (3) |
| C7B | 0.025 (4) | 0.026 (4) | 0.022 (4) | −0.001 (3) | 0.001 (3) | −0.008 (3) |
| C8B | 0.031 (4) | 0.033 (4) | 0.014 (3) | −0.006 (3) | −0.005 (3) | −0.009 (3) |
Geometric parameters (Å, °)
| Br1—C8A | 1.932 (8) | C5A—H5AA | 0.9500 |
| Br2—C8B | 1.908 (7) | C6A—H6AA | 0.9500 |
| O1A—N1A | 1.215 (9) | C7A—C8A | 1.515 (11) |
| O2A—N1A | 1.224 (10) | C8A—H8AA | 0.9900 |
| O3A—C7A | 1.213 (10) | C8A—H8AB | 0.9900 |
| O1B—N1B | 1.221 (10) | C1B—C6B | 1.406 (10) |
| O2B—N1B | 1.229 (10) | C1B—C2B | 1.410 (11) |
| O3B—C7B | 1.202 (10) | C1B—C7B | 1.492 (11) |
| N1A—C3A | 1.477 (10) | C2B—C3B | 1.366 (11) |
| N1B—C3B | 1.472 (10) | C2B—H2BA | 0.9500 |
| C1A—C6A | 1.392 (11) | C3B—C4B | 1.392 (11) |
| C1A—C2A | 1.403 (11) | C4B—C5B | 1.373 (12) |
| C1A—C7A | 1.496 (11) | C4B—H4BA | 0.9500 |
| C2A—C3A | 1.377 (11) | C5B—C6B | 1.394 (12) |
| C2A—H2AA | 0.9500 | C5B—H5BA | 0.9500 |
| C3A—C4A | 1.392 (12) | C6B—H6BA | 0.9500 |
| C4A—C5A | 1.365 (12) | C7B—C8B | 1.539 (11) |
| C4A—H4AA | 0.9500 | C8B—H8BA | 0.9900 |
| C5A—C6A | 1.390 (12) | C8B—H8BB | 0.9900 |
| O1A—N1A—O2A | 124.0 (7) | C7A—C8A—H8AB | 109.2 |
| O1A—N1A—C3A | 118.7 (7) | Br1—C8A—H8AB | 109.2 |
| O2A—N1A—C3A | 117.3 (7) | H8AA—C8A—H8AB | 107.9 |
| O1B—N1B—O2B | 122.5 (7) | C6B—C1B—C2B | 119.5 (7) |
| O1B—N1B—C3B | 119.5 (7) | C6B—C1B—C7B | 122.9 (7) |
| O2B—N1B—C3B | 118.0 (7) | C2B—C1B—C7B | 117.6 (7) |
| C6A—C1A—C2A | 120.2 (7) | C3B—C2B—C1B | 117.4 (7) |
| C6A—C1A—C7A | 123.0 (7) | C3B—C2B—H2BA | 121.3 |
| C2A—C1A—C7A | 116.8 (7) | C1B—C2B—H2BA | 121.3 |
| C3A—C2A—C1A | 117.5 (7) | C2B—C3B—C4B | 124.2 (8) |
| C3A—C2A—H2AA | 121.3 | C2B—C3B—N1B | 117.5 (7) |
| C1A—C2A—H2AA | 121.3 | C4B—C3B—N1B | 118.3 (7) |
| C2A—C3A—C4A | 123.0 (7) | C5B—C4B—C3B | 118.2 (7) |
| C2A—C3A—N1A | 117.7 (7) | C5B—C4B—H4BA | 120.9 |
| C4A—C3A—N1A | 119.3 (7) | C3B—C4B—H4BA | 120.9 |
| C5A—C4A—C3A | 118.6 (8) | C4B—C5B—C6B | 120.2 (7) |
| C5A—C4A—H4AA | 120.7 | C4B—C5B—H5BA | 119.9 |
| C3A—C4A—H4AA | 120.7 | C6B—C5B—H5BA | 119.9 |
| C4A—C5A—C6A | 120.6 (8) | C5B—C6B—C1B | 120.5 (7) |
| C4A—C5A—H5AA | 119.7 | C5B—C6B—H6BA | 119.7 |
| C6A—C5A—H5AA | 119.7 | C1B—C6B—H6BA | 119.7 |
| C5A—C6A—C1A | 120.1 (8) | O3B—C7B—C1B | 121.0 (7) |
| C5A—C6A—H6AA | 120.0 | O3B—C7B—C8B | 121.9 (7) |
| C1A—C6A—H6AA | 120.0 | C1B—C7B—C8B | 117.1 (6) |
| O3A—C7A—C1A | 121.0 (7) | C7B—C8B—Br2 | 112.4 (5) |
| O3A—C7A—C8A | 122.6 (7) | C7B—C8B—H8BA | 109.1 |
| C1A—C7A—C8A | 116.4 (7) | Br2—C8B—H8BA | 109.1 |
| C7A—C8A—Br1 | 112.2 (5) | C7B—C8B—H8BB | 109.1 |
| C7A—C8A—H8AA | 109.2 | Br2—C8B—H8BB | 109.1 |
| Br1—C8A—H8AA | 109.2 | H8BA—C8B—H8BB | 107.8 |
| C6A—C1A—C2A—C3A | 0.7 (11) | C6B—C1B—C2B—C3B | 0.1 (11) |
| C7A—C1A—C2A—C3A | 179.1 (6) | C7B—C1B—C2B—C3B | 179.2 (7) |
| C1A—C2A—C3A—C4A | −0.5 (11) | C1B—C2B—C3B—C4B | −1.1 (11) |
| C1A—C2A—C3A—N1A | 179.7 (6) | C1B—C2B—C3B—N1B | 179.1 (6) |
| O1A—N1A—C3A—C2A | −5.5 (10) | O1B—N1B—C3B—C2B | 3.0 (11) |
| O2A—N1A—C3A—C2A | 175.7 (7) | O2B—N1B—C3B—C2B | −177.6 (8) |
| O1A—N1A—C3A—C4A | 174.7 (7) | O1B—N1B—C3B—C4B | −176.8 (7) |
| O2A—N1A—C3A—C4A | −4.1 (11) | O2B—N1B—C3B—C4B | 2.6 (11) |
| C2A—C3A—C4A—C5A | −0.1 (11) | C2B—C3B—C4B—C5B | 1.3 (12) |
| N1A—C3A—C4A—C5A | 179.8 (7) | N1B—C3B—C4B—C5B | −178.9 (7) |
| C3A—C4A—C5A—C6A | 0.5 (11) | C3B—C4B—C5B—C6B | −0.5 (11) |
| C4A—C5A—C6A—C1A | −0.3 (12) | C4B—C5B—C6B—C1B | −0.4 (12) |
| C2A—C1A—C6A—C5A | −0.3 (11) | C2B—C1B—C6B—C5B | 0.6 (11) |
| C7A—C1A—C6A—C5A | −178.6 (7) | C7B—C1B—C6B—C5B | −178.4 (7) |
| C6A—C1A—C7A—O3A | 179.3 (7) | C6B—C1B—C7B—O3B | 174.9 (8) |
| C2A—C1A—C7A—O3A | 0.9 (11) | C2B—C1B—C7B—O3B | −4.2 (12) |
| C6A—C1A—C7A—C8A | −1.5 (11) | C6B—C1B—C7B—C8B | −6.5 (11) |
| C2A—C1A—C7A—C8A | −179.9 (7) | C2B—C1B—C7B—C8B | 174.5 (6) |
| O3A—C7A—C8A—Br1 | 1.7 (10) | O3B—C7B—C8B—Br2 | −12.8 (10) |
| C1A—C7A—C8A—Br1 | −177.5 (5) | C1B—C7B—C8B—Br2 | 168.6 (5) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C4A—H4AA···O1Bi | 0.95 | 2.49 | 3.314 (10) | 145. |
| C5A—H5AA···Br2ii | 0.95 | 3.04 | 3.849 (8) | 144. |
| C5A—H5AA···O2Bi | 0.95 | 2.55 | 3.409 (11) | 150. |
| C6A—H6AA···O3Bii | 0.95 | 2.38 | 3.320 (10) | 171. |
| C4B—H4BA···O1Aiii | 0.95 | 2.56 | 3.420 (9) | 150. |
| C6B—H6BA···O3A | 0.95 | 2.35 | 3.278 (10) | 165. |
Symmetry codes: (i) x−1, y+1, z−1; (ii) x−1, y+1, z; (iii) x, y, z+1.
Table 2 Cg···Cg π stacking interactions (Å)
Cg1 and Cg2 are the centroids of rings C1A–C6A and Cg1B–Cg6B
| CgI···CgJ | Cg···Cg | CgI Perp | CgJ Perp | Slippage |
| Cg1···Cg1i | 3.710 (5) | -3.357 (3) | -3.357 (3) | 1.58 (2) |
| Cg2···Cg2ii | 3.677 (5) | -3.418 (3) | -3.418 (3) | 1.35 (5) |
Symmetry codes: (i) -x, 1-y, 1-z; (ii) 1-x, -y, 2-z.
Table 3 Short non-hydrogen intermolecular interactions (Å).
| Atom I···Atom J | d(I–J) | Del |
| Br1i···O2Aii | 3.16 (6) | -0.20 |
| O2Ai···Br1iii | 3.16 (6) | -0.20 |
| Br2i···O2Biii | 3.06 (8) | -0.30 |
| O2Bi···Br2ii | 3.06 (8) | -0.30 |
Symmetry codes: (i) x, y, z; (ii) x, y, 1+z; (iii) x, y, -1+z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SJ5067).
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/S1600536810049585/sj5067sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049585/sj5067Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



