Abstract
The asymmetric unit of the title compound, C8H7Br2NO3, comprises two crystallographically independent molecules (A and B). The nitro groups are twisted from the attached benzene rings, making dihedral angles of 39.26 (9) and 35.90 (9)° in molecules A and B, respectively. In each molecule, the dibromomethyl group is orientated in such a way that the two Br atoms are tilted away from the benzene ring. An interesting features of the crystal structure is the two short Br⋯Br interactions which, together with intermolecular C—H⋯O hydrogen bonds, link the molecules into an extended three-dimensional network. The crystal structure is further stabilized by weak C—H⋯π interactions.
Related literature
For general background to and applications of brominated organic compounds, see Augustine et al. (2007 ▶); Derdau et al. (2003 ▶); Khatuya (2001 ▶); Tyeklar et al. (1993 ▶). For related structures, see: Fun, Chantrapromma, Maity et al. (2009 ▶); Fun, Chantrapromma, Sujith et al. (2009 ▶); Yeap et al. (2008 ▶). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986 ▶).
Experimental
Crystal data
C8H7Br2NO3
M r = 324.97
Triclinic,
a = 7.9591 (1) Å
b = 11.1949 (2) Å
c = 12.2509 (2) Å
α = 106.285 (1)°
β = 99.691 (1)°
γ = 102.401 (1)°
V = 992.45 (3) Å3
Z = 4
Mo Kα radiation
μ = 8.15 mm−1
T = 100 K
0.28 × 0.25 × 0.19 mm
Data collection
Bruker SMART APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2005 ▶) T min = 0.210, T max = 0.311 (expected range = 0.147–0.218)
32659 measured reflections
8800 independent reflections
7332 reflections with I > 2σ(I)
R int = 0.027
Refinement
R[F 2 > 2σ(F 2)] = 0.026
wR(F 2) = 0.066
S = 1.01
8800 reflections
261 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.78 e Å−3
Δρmin = −0.47 e Å−3
Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809031833/wn2343sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809031833/wn2343Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected interatomic distances (Å).
| Br1A⋯Br2Bi | 3.5915 (3) |
| Br2A⋯Br1Bii | 3.6279 (2) |
Symmetry codes: (i)
; (ii)
.
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C7A—H7A⋯O2B | 0.95 (2) | 2.47 (2) | 3.134 (2) | 126.8 (17) |
| C8B—H8BA⋯O1Aiii | 0.96 | 2.52 | 3.370 (2) | 148 |
| C8A—H8AA⋯Cg2iv | 0.96 | 2.95 | 3.839 (2) | 155 |
Symmetry codes: (iii)
; (iv)
. Cg2 is the centroid of the C1B–C6B benzene ring.
Acknowledgments
HKF and JHG thank Universiti Sains Malaysia (USM) for the Research Universiti Golden Goose Grant (No. 1001/PFIZIK/811012). JHG thanks USM for the award of a USM Fellowship. AMI is grateful to the Director, NITK, Surathkal, India, for providing research facilities.
supplementary crystallographic information
Comment
Brominated organic compounds are important synthetic intermediates and products in organic chemistry (Augustine et al., 2007). They are found in C-C coupling reactions, as precursors to organometallic species and in nucleophilic substitutions (Tyeklar et al., 1993). They are also used for the synthesis of useful pharmaceutical materials and agrochemicals (Derdau et al., 2003). However the use of molecular bromine as an electrophilic brominating reagent has several drawbacks arising from its toxic and corrosive nature and its high reactivity (Tyeklar et al., 1993). Alternative brominating reagents such as N-bromosuccinimide make for easier handling and result in improved selectivity (Khatuya, 2001).
In the asymmetric unit of the title compound, there are two crystallographically independent molecules, designated A and B (Fig. 1). In each molecule, the nitro group is twisted from the mean plane of the C1-C6 benzene ring, as shown by the dihedral angle formed between the mean plane through C5/N1/O2/O3 and the C1-C6 benzene ring of 39.26 (9)° in molecule A; the comparable angle is 35.90 (9)° for molecule B. Meanwhile, the dibromomethyl group is orientated in such a way that the two Br atoms are tilted away from the benzene ring. The bond lengths and angles are comparable to those found in related structures (Fun, Chantrapromma, Maity et al., 2009; Fun, Chantrapromma, Sujith et al., 2009; Yeap et al., 2008).
In the crystal structure (Fig. 2), the interesting features are the Br1A···Br2B and Br2A···Br1B short interactions (Table 1). Together with intermolecular C7A—H7A···O2B and C8B—H8BA···O1A hydrogen bonds (Table 2), they link the molecules into a three-dimensional extended network. The crystal structure is further stabilized by weak C8A—H8AA···Cg2 interactions (Table 2).
Experimental
Benzoyl peroxide (0.20 g, 10 %) and N-bromosuccinimide (6.38 g, 0.0358 mol) were added in portions to a solution of 4-methyl-2-nitroanisole (2.00 g, 0.0119 mol) in CCl4 (20 ml). The reaction mixture was heated at 85 °C under a nitrogen atmosphere for 12 h. The reaction mass was cooled and filtered. The filtrate was concentrated to produce a crude product. The latter was recrystallized with hexane to afford the title compound as a colourless crystalline solid. The yield was 3.50 g, 92 %. M.p. 370–373 K.
Refinement
The H-atoms bound to C7A and C7B were located from the difference Fourier map and allowed to refine freely. The other H-atoms were placed in calculated positions, with C—H = 0.93 Å, Uiso(H) = 1.2Ueq(C) for aromatic, and C—H = 0.96 Å, Uiso(H) = 1.5Ueq(C) for methyl group; these aromatic and methyl group H atoms were refined as riding on their parent atoms. A rotating group model was used for the methyl group.
Figures
Fig. 1.
The molecular structure of the asymmetric unit of the title compound, showing 50% probability displacement ellipsoids and the atom-numbering scheme. Hydrogen atoms are shown as spheres of arbitrary radius.
Fig. 2.
Three-dimensional extended network, viewed along the a axis. Intermolecular interactions are shown as dashed lines.
Crystal data
| C8H7Br2NO3 | Z = 4 |
| Mr = 324.97 | F(000) = 624 |
| Triclinic, P1 | Dx = 2.175 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.9591 (1) Å | Cell parameters from 9885 reflections |
| b = 11.1949 (2) Å | θ = 2.2–35.1° |
| c = 12.2509 (2) Å | µ = 8.15 mm−1 |
| α = 106.285 (1)° | T = 100 K |
| β = 99.691 (1)° | Block, colourless |
| γ = 102.401 (1)° | 0.28 × 0.25 × 0.19 mm |
| V = 992.45 (3) Å3 |
Data collection
| Bruker SMART APEXII CCD area-detector diffractometer | 8800 independent reflections |
| Radiation source: fine-focus sealed tube | 7332 reflections with I > 2σ(I) |
| graphite | Rint = 0.027 |
| φ and ω scans | θmax = 35.3°, θmin = 2.0° |
| Absorption correction: multi-scan (SADABS; Bruker, 2005) | h = −12→12 |
| Tmin = 0.210, Tmax = 0.311 | k = −17→18 |
| 32659 measured reflections | l = −19→19 |
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)] = 0.026 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.066 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.01 | w = 1/[σ2(Fo2) + (0.0361P)2 + 0.2346P] where P = (Fo2 + 2Fc2)/3 |
| 8800 reflections | (Δ/σ)max = 0.004 |
| 261 parameters | Δρmax = 0.78 e Å−3 |
| 0 restraints | Δρmin = −0.47 e Å−3 |
Special details
| Experimental. The crystal was placed in the cold stream of an Oxford Cyrosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1)K. |
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| Br1A | 0.79537 (2) | 1.230776 (16) | 0.197580 (14) | 0.02458 (4) | |
| Br2A | 0.90786 (2) | 1.101536 (16) | 0.387687 (13) | 0.02180 (4) | |
| O1A | 0.76010 (16) | 0.62902 (12) | −0.10724 (10) | 0.0229 (2) | |
| O2A | 0.30267 (16) | 0.76549 (13) | 0.10327 (11) | 0.0265 (2) | |
| O3A | 0.37293 (16) | 0.96938 (13) | 0.11963 (11) | 0.0257 (2) | |
| N1A | 0.40781 (17) | 0.86506 (14) | 0.10586 (11) | 0.0208 (2) | |
| C1A | 0.8937 (2) | 0.94163 (16) | 0.11837 (13) | 0.0209 (3) | |
| H1AA | 0.9990 | 1.0061 | 0.1578 | 0.025* | |
| C2A | 0.8985 (2) | 0.83283 (16) | 0.03310 (13) | 0.0216 (3) | |
| H2AA | 1.0052 | 0.8260 | 0.0142 | 0.026* | |
| C3A | 0.7427 (2) | 0.73241 (15) | −0.02523 (13) | 0.0195 (3) | |
| C4A | 0.58321 (19) | 0.74374 (15) | 0.00283 (13) | 0.0188 (2) | |
| H4AA | 0.4792 | 0.6770 | −0.0335 | 0.023* | |
| C5A | 0.58299 (19) | 0.85699 (15) | 0.08631 (13) | 0.0185 (2) | |
| C6A | 0.73536 (19) | 0.95856 (15) | 0.14790 (13) | 0.0184 (2) | |
| C7A | 0.7370 (2) | 1.07568 (15) | 0.24351 (13) | 0.0196 (3) | |
| C8A | 0.6054 (2) | 0.52136 (17) | −0.16335 (15) | 0.0256 (3) | |
| H8AA | 0.6344 | 0.4546 | −0.2193 | 0.038* | |
| H8AB | 0.5141 | 0.5491 | −0.2029 | 0.038* | |
| H8AC | 0.5640 | 0.4883 | −0.1055 | 0.038* | |
| Br1B | −0.20637 (2) | 0.726206 (17) | 0.325018 (14) | 0.02462 (4) | |
| Br2B | −0.10244 (2) | 0.523519 (16) | 0.125556 (13) | 0.02342 (4) | |
| O1B | 0.50849 (16) | 0.63292 (12) | 0.60857 (11) | 0.0243 (2) | |
| O2B | 0.49443 (16) | 0.92884 (12) | 0.36858 (11) | 0.0252 (2) | |
| O3B | 0.22098 (17) | 0.93622 (12) | 0.34859 (12) | 0.0261 (2) | |
| N1B | 0.33898 (17) | 0.88484 (13) | 0.36914 (11) | 0.0197 (2) | |
| C1B | 0.1045 (2) | 0.56681 (15) | 0.38962 (13) | 0.0206 (3) | |
| H1BA | −0.0019 | 0.5017 | 0.3575 | 0.025* | |
| C2B | 0.2309 (2) | 0.55536 (16) | 0.47501 (14) | 0.0215 (3) | |
| H2BA | 0.2081 | 0.4840 | 0.5005 | 0.026* | |
| C3B | 0.3935 (2) | 0.65079 (16) | 0.52360 (13) | 0.0200 (3) | |
| C4B | 0.4281 (2) | 0.75603 (15) | 0.48395 (13) | 0.0199 (3) | |
| H4BA | 0.5370 | 0.8186 | 0.5131 | 0.024* | |
| C5B | 0.29538 (19) | 0.76575 (15) | 0.39929 (13) | 0.0180 (2) | |
| C6B | 0.13101 (19) | 0.67357 (15) | 0.34948 (13) | 0.0185 (2) | |
| C7B | −0.0114 (2) | 0.68337 (16) | 0.25833 (13) | 0.0203 (3) | |
| C8B | 0.6731 (2) | 0.73163 (19) | 0.66117 (16) | 0.0289 (3) | |
| H8BA | 0.7436 | 0.7088 | 0.7196 | 0.043* | |
| H8BB | 0.6504 | 0.8126 | 0.6971 | 0.043* | |
| H8BC | 0.7359 | 0.7397 | 0.6021 | 0.043* | |
| H7A | 0.627 (3) | 1.0704 (19) | 0.2645 (17) | 0.013 (4)* | |
| H7B | 0.022 (3) | 0.747 (2) | 0.226 (2) | 0.028 (6)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1A | 0.03013 (8) | 0.01907 (7) | 0.02323 (7) | 0.00585 (6) | 0.00401 (6) | 0.00714 (6) |
| Br2A | 0.01964 (7) | 0.02534 (8) | 0.01851 (6) | 0.00619 (5) | 0.00280 (5) | 0.00539 (5) |
| O1A | 0.0221 (5) | 0.0217 (5) | 0.0231 (5) | 0.0078 (4) | 0.0056 (4) | 0.0033 (4) |
| O2A | 0.0185 (5) | 0.0262 (6) | 0.0315 (6) | 0.0021 (4) | 0.0067 (4) | 0.0068 (5) |
| O3A | 0.0211 (5) | 0.0255 (6) | 0.0293 (6) | 0.0111 (4) | 0.0033 (4) | 0.0052 (5) |
| N1A | 0.0171 (5) | 0.0232 (6) | 0.0198 (5) | 0.0060 (5) | 0.0029 (4) | 0.0043 (5) |
| C1A | 0.0167 (6) | 0.0229 (7) | 0.0215 (6) | 0.0049 (5) | 0.0037 (5) | 0.0060 (5) |
| C2A | 0.0180 (6) | 0.0255 (7) | 0.0210 (6) | 0.0071 (5) | 0.0051 (5) | 0.0062 (5) |
| C3A | 0.0206 (6) | 0.0198 (7) | 0.0185 (6) | 0.0076 (5) | 0.0039 (5) | 0.0061 (5) |
| C4A | 0.0173 (6) | 0.0179 (6) | 0.0196 (6) | 0.0050 (5) | 0.0020 (5) | 0.0051 (5) |
| C5A | 0.0158 (6) | 0.0200 (7) | 0.0199 (6) | 0.0062 (5) | 0.0037 (5) | 0.0063 (5) |
| C6A | 0.0173 (6) | 0.0189 (6) | 0.0186 (6) | 0.0051 (5) | 0.0036 (5) | 0.0060 (5) |
| C7A | 0.0191 (6) | 0.0186 (6) | 0.0189 (6) | 0.0034 (5) | 0.0034 (5) | 0.0046 (5) |
| C8A | 0.0278 (8) | 0.0205 (7) | 0.0260 (7) | 0.0066 (6) | 0.0064 (6) | 0.0042 (6) |
| Br1B | 0.01982 (7) | 0.02733 (8) | 0.02389 (7) | 0.00989 (6) | 0.00277 (5) | 0.00308 (6) |
| Br2B | 0.02590 (7) | 0.02424 (8) | 0.01841 (6) | 0.00830 (6) | 0.00365 (5) | 0.00441 (5) |
| O1B | 0.0208 (5) | 0.0264 (6) | 0.0264 (5) | 0.0062 (4) | 0.0013 (4) | 0.0125 (5) |
| O2B | 0.0205 (5) | 0.0262 (6) | 0.0282 (6) | 0.0014 (4) | 0.0061 (4) | 0.0118 (5) |
| O3B | 0.0262 (6) | 0.0224 (6) | 0.0327 (6) | 0.0100 (5) | 0.0059 (5) | 0.0122 (5) |
| N1B | 0.0209 (6) | 0.0174 (6) | 0.0202 (5) | 0.0043 (5) | 0.0045 (4) | 0.0065 (4) |
| C1B | 0.0197 (6) | 0.0189 (7) | 0.0225 (6) | 0.0038 (5) | 0.0042 (5) | 0.0076 (5) |
| C2B | 0.0211 (6) | 0.0197 (7) | 0.0251 (7) | 0.0055 (5) | 0.0058 (5) | 0.0094 (5) |
| C3B | 0.0187 (6) | 0.0211 (7) | 0.0216 (6) | 0.0073 (5) | 0.0049 (5) | 0.0077 (5) |
| C4B | 0.0181 (6) | 0.0200 (7) | 0.0211 (6) | 0.0050 (5) | 0.0040 (5) | 0.0065 (5) |
| C5B | 0.0191 (6) | 0.0165 (6) | 0.0196 (6) | 0.0055 (5) | 0.0057 (5) | 0.0066 (5) |
| C6B | 0.0170 (6) | 0.0190 (6) | 0.0192 (6) | 0.0051 (5) | 0.0042 (5) | 0.0058 (5) |
| C7B | 0.0193 (6) | 0.0199 (7) | 0.0208 (6) | 0.0048 (5) | 0.0039 (5) | 0.0065 (5) |
| C8B | 0.0228 (7) | 0.0303 (9) | 0.0301 (8) | 0.0047 (6) | −0.0012 (6) | 0.0112 (7) |
Geometric parameters (Å, °)
| Br1A—C7A | 1.9587 (15) | Br1B—C7B | 1.9576 (16) |
| Br2A—C7A | 1.9462 (15) | Br2B—C7B | 1.9460 (16) |
| O1A—C3A | 1.3535 (19) | O1B—C3B | 1.3547 (19) |
| O1A—C8A | 1.433 (2) | O1B—C8B | 1.431 (2) |
| O2A—N1A | 1.2306 (18) | O2B—N1B | 1.2314 (17) |
| O3A—N1A | 1.2305 (19) | O3B—N1B | 1.2288 (18) |
| N1A—C5A | 1.4710 (19) | N1B—C5B | 1.4680 (19) |
| C1A—C2A | 1.377 (2) | C1B—C2B | 1.378 (2) |
| C1A—C6A | 1.405 (2) | C1B—C6B | 1.404 (2) |
| C1A—H1AA | 0.9300 | C1B—H1BA | 0.9300 |
| C2A—C3A | 1.402 (2) | C2B—C3B | 1.401 (2) |
| C2A—H2AA | 0.9300 | C2B—H2BA | 0.9300 |
| C3A—C4A | 1.392 (2) | C3B—C4B | 1.388 (2) |
| C4A—C5A | 1.388 (2) | C4B—C5B | 1.395 (2) |
| C4A—H4AA | 0.9300 | C4B—H4BA | 0.9300 |
| C5A—C6A | 1.397 (2) | C5B—C6B | 1.395 (2) |
| C6A—C7A | 1.489 (2) | C6B—C7B | 1.497 (2) |
| C7A—H7A | 0.948 (19) | C7B—H7B | 0.92 (2) |
| C8A—H8AA | 0.9600 | C8B—H8BA | 0.9600 |
| C8A—H8AB | 0.9600 | C8B—H8BB | 0.9600 |
| C8A—H8AC | 0.9600 | C8B—H8BC | 0.9600 |
| Br1A···Br2Bi | 3.5915 (3) | Br2A···Br1Bii | 3.6279 (2) |
| C3A—O1A—C8A | 117.29 (13) | C3B—O1B—C8B | 116.75 (13) |
| O3A—N1A—O2A | 123.97 (14) | O3B—N1B—O2B | 123.87 (14) |
| O3A—N1A—C5A | 118.23 (13) | O3B—N1B—C5B | 118.83 (12) |
| O2A—N1A—C5A | 117.75 (14) | O2B—N1B—C5B | 117.28 (13) |
| C2A—C1A—C6A | 122.27 (14) | C2B—C1B—C6B | 122.16 (14) |
| C2A—C1A—H1AA | 118.9 | C2B—C1B—H1BA | 118.9 |
| C6A—C1A—H1AA | 118.9 | C6B—C1B—H1BA | 118.9 |
| C1A—C2A—C3A | 120.06 (14) | C1B—C2B—C3B | 120.25 (14) |
| C1A—C2A—H2AA | 120.0 | C1B—C2B—H2BA | 119.9 |
| C3A—C2A—H2AA | 120.0 | C3B—C2B—H2BA | 119.9 |
| O1A—C3A—C4A | 124.35 (14) | O1B—C3B—C4B | 124.10 (14) |
| O1A—C3A—C2A | 115.97 (13) | O1B—C3B—C2B | 116.25 (14) |
| C4A—C3A—C2A | 119.68 (14) | C4B—C3B—C2B | 119.65 (14) |
| C5A—C4A—C3A | 118.44 (14) | C3B—C4B—C5B | 118.43 (14) |
| C5A—C4A—H4AA | 120.8 | C3B—C4B—H4BA | 120.8 |
| C3A—C4A—H4AA | 120.8 | C5B—C4B—H4BA | 120.8 |
| C4A—C5A—C6A | 123.78 (14) | C4B—C5B—C6B | 123.70 (14) |
| C4A—C5A—N1A | 115.23 (13) | C4B—C5B—N1B | 114.52 (13) |
| C6A—C5A—N1A | 120.98 (14) | C6B—C5B—N1B | 121.73 (13) |
| C5A—C6A—C1A | 115.70 (14) | C5B—C6B—C1B | 115.76 (14) |
| C5A—C6A—C7A | 123.71 (13) | C5B—C6B—C7B | 123.88 (14) |
| C1A—C6A—C7A | 120.52 (13) | C1B—C6B—C7B | 120.36 (13) |
| C6A—C7A—Br2A | 111.59 (11) | C6B—C7B—Br2B | 111.47 (11) |
| C6A—C7A—Br1A | 110.77 (10) | C6B—C7B—Br1B | 110.83 (10) |
| Br2A—C7A—Br1A | 108.66 (7) | Br2B—C7B—Br1B | 109.65 (7) |
| C6A—C7A—H7A | 113.2 (12) | C6B—C7B—H7B | 115.7 (15) |
| Br2A—C7A—H7A | 104.8 (12) | Br2B—C7B—H7B | 105.1 (15) |
| Br1A—C7A—H7A | 107.5 (12) | Br1B—C7B—H7B | 103.7 (15) |
| O1A—C8A—H8AA | 109.5 | O1B—C8B—H8BA | 109.5 |
| O1A—C8A—H8AB | 109.5 | O1B—C8B—H8BB | 109.5 |
| H8AA—C8A—H8AB | 109.5 | H8BA—C8B—H8BB | 109.5 |
| O1A—C8A—H8AC | 109.5 | O1B—C8B—H8BC | 109.5 |
| H8AA—C8A—H8AC | 109.5 | H8BA—C8B—H8BC | 109.5 |
| H8AB—C8A—H8AC | 109.5 | H8BB—C8B—H8BC | 109.5 |
| C6A—C1A—C2A—C3A | −1.9 (2) | C6B—C1B—C2B—C3B | −1.1 (2) |
| C8A—O1A—C3A—C4A | −3.9 (2) | C8B—O1B—C3B—C4B | 1.5 (2) |
| C8A—O1A—C3A—C2A | 176.29 (14) | C8B—O1B—C3B—C2B | −178.30 (15) |
| C1A—C2A—C3A—O1A | −179.68 (14) | C1B—C2B—C3B—O1B | 178.77 (15) |
| C1A—C2A—C3A—C4A | 0.5 (2) | C1B—C2B—C3B—C4B | −1.1 (2) |
| O1A—C3A—C4A—C5A | −178.01 (14) | O1B—C3B—C4B—C5B | −177.36 (15) |
| C2A—C3A—C4A—C5A | 1.8 (2) | C2B—C3B—C4B—C5B | 2.4 (2) |
| C3A—C4A—C5A—C6A | −2.9 (2) | C3B—C4B—C5B—C6B | −1.9 (2) |
| C3A—C4A—C5A—N1A | 176.35 (13) | C3B—C4B—C5B—N1B | 175.71 (14) |
| O3A—N1A—C5A—C4A | −139.68 (14) | O3B—N1B—C5B—C4B | −142.98 (15) |
| O2A—N1A—C5A—C4A | 37.79 (19) | O2B—N1B—C5B—C4B | 35.46 (19) |
| O3A—N1A—C5A—C6A | 39.6 (2) | O3B—N1B—C5B—C6B | 34.7 (2) |
| O2A—N1A—C5A—C6A | −142.94 (15) | O2B—N1B—C5B—C6B | −146.90 (14) |
| C4A—C5A—C6A—C1A | 1.6 (2) | C4B—C5B—C6B—C1B | −0.1 (2) |
| N1A—C5A—C6A—C1A | −177.63 (13) | N1B—C5B—C6B—C1B | −177.56 (14) |
| C4A—C5A—C6A—C7A | −175.35 (14) | C4B—C5B—C6B—C7B | −179.76 (15) |
| N1A—C5A—C6A—C7A | 5.5 (2) | N1B—C5B—C6B—C7B | 2.8 (2) |
| C2A—C1A—C6A—C5A | 0.9 (2) | C2B—C1B—C6B—C5B | 1.6 (2) |
| C2A—C1A—C6A—C7A | 177.90 (14) | C2B—C1B—C6B—C7B | −178.73 (15) |
| C5A—C6A—C7A—Br2A | 124.47 (14) | C5B—C6B—C7B—Br2B | 130.42 (13) |
| C1A—C6A—C7A—Br2A | −52.30 (17) | C1B—C6B—C7B—Br2B | −49.18 (17) |
| C5A—C6A—C7A—Br1A | −114.33 (14) | C5B—C6B—C7B—Br1B | −107.15 (14) |
| C1A—C6A—C7A—Br1A | 68.89 (16) | C1B—C6B—C7B—Br1B | 73.24 (17) |
Symmetry codes: (i) x+1, y+1, z; (ii) −x+1, −y+2, −z+1.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C7A—H7A···O2B | 0.95 (2) | 2.47 (2) | 3.134 (2) | 126.8 (17) |
| C8B—H8BA···O1Aiii | 0.96 | 2.52 | 3.370 (2) | 148 |
| C8A—H8AA···Cg2iv | 0.96 | 2.95 | 3.839 (2) | 155 |
Symmetry codes: (iii) x, y, z+1; (iv) −x+1, −y+1, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WN2343).
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/S1600536809031833/wn2343sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809031833/wn2343Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


