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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 4;67(Pt 1):o29–o30. doi: 10.1107/S1600536810049585

2-Bromo-1-(3-nitro­phen­yl)ethanone

Jerry P Jasinski a,*, Ray J Butcher b, A S Praveen c, H S Yathirajan c, B Narayana d
PMCID: PMC3050415  PMID: 21522741

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 ▶).graphic file with name e-67-00o29-scheme1.jpg

Experimental

Crystal data

  • C8H6BrNO3

  • M r = 244.05

  • Triclinic, Inline graphic

  • 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

e-67-00o29-sup1.cif (19.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049585/sj5067Isup2.hkl

e-67-00o29-Isup2.hkl (157.7KB, 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) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

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.

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.

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.

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

e-67-00o29-sup1.cif (19.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049585/sj5067Isup2.hkl

e-67-00o29-Isup2.hkl (157.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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