organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

4-[2,3-Di­bromo-3-(4-bromo­phen­yl)propano­yl]-2-phenyl-1,2,3-oxa­diazol-2-ium-5-olate

aX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia, and bDepartment of Studies in Chemistry, Mangalore University, Mangalagangotri, Mangalore 574 199, India
*Correspondence e-mail: hkfun@usm.my

(Received 5 October 2010; accepted 9 October 2010; online 20 October 2010)

In the title compound, C17H11Br3N2O3, the whole mol­ecule is disordered over two positions with a refined occupancy ratio of 0.770 (5):0.230 (5). In the major component, the 1,2,3-oxadiazo­lidine ring is essentially planar [maximum deviation = 0.017 (6) Å] and makes dihedral angles of 22.5 (3) and 70.2 (3)° with the 4-bromo­phenyl and phenyl rings, respectively. In the minor component, the corresponding values are 18.9 (11) and 84.9 (12)°. In the crystal, inter­molecular C—H⋯Br hydrogen bonds link the mol­ecules into ribbons along [010]. There is a short O⋯N contact [2.83 (3) Å] in the minor component. In the major component, the mol­ecular structure is stabilized by an intra­molecular C—H⋯O hydrogen bond, which forms an S(6) ring motif.

Related literature

For biological activity of sydnones, mesoionic compounds having a 1,2,3-oxadiazole skeleton and bearing an oxygen atom attached to the 5-position, see: Jyothi et al. (2008[Jyothi, C. H., Girisha, K. S., Adithya, A. & Kalluraya, B. (2008). Eur. J. Med. Chem. 43, 2831-2834.]); Rai et al. (2007[Rai, N. S., Kalluraya, B. & Lingappa, B. (2007). Synth. Commun. 37, 2267-2273.]; 2008[Rai, N. S., Kalluraya, B., Lingappa, B., Shenoy, S. & Puranic, V. G. (2008). Eur. J. Med. Chem. 43, 1715-1720.]). For a related structure, see: Goh et al. (2010[Goh, J. H., Fun, H.-K., Nithinchandra, & Kalluraya, B. (2010). Acta Cryst. E66, o1303.]). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986[Cosier, J. & Glazer, A. M. (1986). J. Appl. Cryst. 19, 105-107.]). For bond-length data, see: Allen et al. (1987[Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1-19.]). For hydrogen-bond motifs, see: Bernstein et al. (1995[Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.]).

[Scheme 1]

Experimental

Crystal data
  • C17H11Br3N2O3

  • Mr = 531.01

  • Monoclinic, P 21 /n

  • a = 17.6996 (3) Å

  • b = 5.8322 (1) Å

  • c = 18.2445 (3) Å

  • β = 105.973 (1)°

  • V = 1810.62 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 6.70 mm−1

  • T = 100 K

  • 0.43 × 0.38 × 0.12 mm

Data collection
  • Bruker SMART APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.159, Tmax = 0.505

  • 20140 measured reflections

  • 5243 independent reflections

  • 4218 reflections with I > 2σ(I)

  • Rint = 0.028

Refinement
  • R[F2 > 2σ(F2)] = 0.025

  • wR(F2) = 0.055

  • S = 1.02

  • 5243 reflections

  • 352 parameters

  • 207 restraints

  • H-atom parameters constrained

  • Δρmax = 0.50 e Å−3

  • Δρmin = −0.37 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C10A—H10A⋯O2A 0.98 2.40 3.168 (4) 135
C14A—H14A⋯Br3Ai 0.93 2.91 3.809 (5) 163
Symmetry code: (i) [-x+{\script{3\over 2}}, y-{\script{1\over 2}}, -z+{\script{1\over 2}}].

Data collection: APEX2 (Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009[Spek, A. L. (2009). Acta Cryst. D65, 148-155.]).

Supporting information


Comment top

Sydnones are mesoionic heterocyclic aromatic chemical compounds. The study of sydnones still remains a field of interests because of their electronic structures and also because of the varied types of biological activities displayed by some of them (Rai et al., 2008). Recently sydnone derivatives were found to exhibit promising antimicrobial properties (Jyothi et al., 2008). Since their discovery, sydnones have shown diverse biological activities and it is thought that the meso-ionic nature of the sydnone ring promotes significant interactions with biological systems. Because of wide variety of properties displayed by sydnones we were prompted to synthesize a new chalcone containing a sydnone type ring. Propenones are prepared by the condensation of 4-acetyl-3-arylsydnones with appropriately substituted aromatic aldehydes in an ethanol medium employing sodium hydroxide as catalyst. Bromination of these propenones were carried out using bromine in glacial acetic acid medium to give dibromochalcones (Rai et al., 2007).

In the title compound (Fig. 1), the whole molecule is disordered over two positions with a refined occupancy ratio of 0.770 (5):0.230 (5). This molecule consists of three rings, namely phenyl (C1–C6), 1,2,3-oxadiazolidine (N1/N2/O1/C7/C8) and bromophenyl (C12–C17/Br3) rings. In the major component, the 1,2,3-oxadiazolidine ring is essentially planar (maximum deviation of 0.017 (6) Å at atom N1A) and makes dihedral angles of 22.5 (3) and 70.2 (3)° with 4-bromophenyl and phenyl rings, respectively. In the minor component, the corresponding values are 18.9 (11) and 84.9 (12)° between the 1,2,3-oxadiazolidine ring (maximum deviation of 0.020 (16) Å at atom O1B) and with the 4-bromophenyl and phenyl ring. The bond lengths (Allen et al., 1987) and angles are within normal ranges and are comparable to the closely related structure (Goh et al., 2010). The molecular structure is stabilized by an intramolecular C10A–H10A···O2A hydrogen bond, which forms an S(6) ring motif.

In the crystal packing (Fig. 2 & Fig. 3), intermolecular C14A—H14A···Br3A hydrogen bonds (Table 1), link the molecules into one-dimensional ribbons along the [010] direction. There is a short contact [O2B···N2B = 2.83 (3) Å, symmetry code 1/2 - x, -1/2 + y, 1/2 - z] in the minor component.

Related literature top

For biological activity of sydnones, mesoionic compounds having a 1,2,3-oxadiazole skeleton and bearing an oxygen atom attached to the 5-position, see: Jyothi et al. (2008); Rai et al. (2007; 2008). For a related structure, see: Goh et al. (2010). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986). For bond-length data, see: Allen et al. (1987). For hydrogen-bond motifs, see: Bernstein et al. (1995).

Experimental top

1-(3-Phenylsydnon-4yl)-3-(p-bromophenyl)-propen-1-one (0.01 mol) was dissolved in glacial acetic acid (25–30 ml) by gentle warming. A solution of bromine in glacial acetic acid (30% w/v) was added to it with constant stirring till the yellow colour of the bromine persisted. The reaction mixture was stirred at room temperature for 1–2 h. The separated solid was filtered, washed with methanol and dried. It was then recrystallized from ethanol. Crystals suitable for X-ray analysis were obtained from 1:2 mixtures of DMF and ethanol by slow evaporation.

Refinement top

All the H atoms were positioned geometrically [C–H = 0.93 to 0.98 Å] and were refined using a riding model, with Uiso(H) = 1.2 Ueq (C). The whole molecule is disordered over two positions with a refined ratio of 0.770 (5):0.230 (5). Rigidity, similarity and simulation restraints were applied. The possibility of a supercell in which the whole-molecule disorder would be no longer exit was addressed by examining the h0l, 0kl, hk0 precession layers to ensure there are no rows of weak reflections between the rows that represent the current unit cell. No such supercell reflections were found. This finding is consistent with the fact that if such a supercell exists, the occupanies of the major and minor components would be the same. However the refined occupanies are 0.770 (5): 0.230 (5) disproving the existence of a supercell.

Structure description top

Sydnones are mesoionic heterocyclic aromatic chemical compounds. The study of sydnones still remains a field of interests because of their electronic structures and also because of the varied types of biological activities displayed by some of them (Rai et al., 2008). Recently sydnone derivatives were found to exhibit promising antimicrobial properties (Jyothi et al., 2008). Since their discovery, sydnones have shown diverse biological activities and it is thought that the meso-ionic nature of the sydnone ring promotes significant interactions with biological systems. Because of wide variety of properties displayed by sydnones we were prompted to synthesize a new chalcone containing a sydnone type ring. Propenones are prepared by the condensation of 4-acetyl-3-arylsydnones with appropriately substituted aromatic aldehydes in an ethanol medium employing sodium hydroxide as catalyst. Bromination of these propenones were carried out using bromine in glacial acetic acid medium to give dibromochalcones (Rai et al., 2007).

In the title compound (Fig. 1), the whole molecule is disordered over two positions with a refined occupancy ratio of 0.770 (5):0.230 (5). This molecule consists of three rings, namely phenyl (C1–C6), 1,2,3-oxadiazolidine (N1/N2/O1/C7/C8) and bromophenyl (C12–C17/Br3) rings. In the major component, the 1,2,3-oxadiazolidine ring is essentially planar (maximum deviation of 0.017 (6) Å at atom N1A) and makes dihedral angles of 22.5 (3) and 70.2 (3)° with 4-bromophenyl and phenyl rings, respectively. In the minor component, the corresponding values are 18.9 (11) and 84.9 (12)° between the 1,2,3-oxadiazolidine ring (maximum deviation of 0.020 (16) Å at atom O1B) and with the 4-bromophenyl and phenyl ring. The bond lengths (Allen et al., 1987) and angles are within normal ranges and are comparable to the closely related structure (Goh et al., 2010). The molecular structure is stabilized by an intramolecular C10A–H10A···O2A hydrogen bond, which forms an S(6) ring motif.

In the crystal packing (Fig. 2 & Fig. 3), intermolecular C14A—H14A···Br3A hydrogen bonds (Table 1), link the molecules into one-dimensional ribbons along the [010] direction. There is a short contact [O2B···N2B = 2.83 (3) Å, symmetry code 1/2 - x, -1/2 + y, 1/2 - z] in the minor component.

For biological activity of sydnones, mesoionic compounds having a 1,2,3-oxadiazole skeleton and bearing an oxygen atom attached to the 5-position, see: Jyothi et al. (2008); Rai et al. (2007; 2008). For a related structure, see: Goh et al. (2010). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986). For bond-length data, see: Allen et al. (1987). For hydrogen-bond motifs, see: Bernstein et al. (1995).

Computing details top

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing 30% probability displacement ellipsoids and the atom-numbering scheme. Both major and minor components are shown. Intramolecular interaction is shown in dashed line.
[Figure 2] Fig. 2. The crystal packing of the title compound, viewed along c axis. Only the major disordered component is shown. Hydrogen atoms not involved in intermolecular hydrogen bonding (dashed lines) are omitted for clarity.
4-[2,3-Dibromo-3-(4-bromophenyl)propanoyl]-2-phenyl-1,2,3-oxadiazol-2- ium-5-olate top
Crystal data top
C17H11Br3N2O3F(000) = 1024
Mr = 531.01Dx = 1.948 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 9198 reflections
a = 17.6996 (3) Åθ = 2.4–29.8°
b = 5.8322 (1) ŵ = 6.70 mm1
c = 18.2445 (3) ÅT = 100 K
β = 105.973 (1)°Block, yellow
V = 1810.62 (5) Å30.43 × 0.38 × 0.12 mm
Z = 4
Data collection top
Bruker SMART APEXII CCD area-detector
diffractometer
5243 independent reflections
Radiation source: fine-focus sealed tube4218 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
φ and ω scansθmax = 30.0°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
h = 2424
Tmin = 0.159, Tmax = 0.505k = 87
20140 measured reflectionsl = 2425
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.025Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.055H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0238P)2 + 0.3541P]
where P = (Fo2 + 2Fc2)/3
5243 reflections(Δ/σ)max = 0.002
352 parametersΔρmax = 0.50 e Å3
207 restraintsΔρmin = 0.37 e Å3
Crystal data top
C17H11Br3N2O3V = 1810.62 (5) Å3
Mr = 531.01Z = 4
Monoclinic, P21/nMo Kα radiation
a = 17.6996 (3) ŵ = 6.70 mm1
b = 5.8322 (1) ÅT = 100 K
c = 18.2445 (3) Å0.43 × 0.38 × 0.12 mm
β = 105.973 (1)°
Data collection top
Bruker SMART APEXII CCD area-detector
diffractometer
5243 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
4218 reflections with I > 2σ(I)
Tmin = 0.159, Tmax = 0.505Rint = 0.028
20140 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.025207 restraints
wR(F2) = 0.055H-atom parameters constrained
S = 1.02Δρmax = 0.50 e Å3
5243 reflectionsΔρmin = 0.37 e Å3
352 parameters
Special details top

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 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) top
xyzUiso*/UeqOcc. (<1)
Br1A0.39809 (10)0.0392 (3)0.03443 (10)0.03273 (19)0.770 (5)
Br2A0.46821 (7)0.55027 (18)0.23460 (8)0.0428 (3)0.770 (5)
Br3A0.80250 (8)0.0292 (2)0.16887 (6)0.03402 (19)0.770 (5)
O1A0.1949 (3)0.0068 (9)0.1943 (3)0.0282 (8)0.770 (5)
O2A0.32784 (19)0.0399 (6)0.2397 (2)0.0293 (6)0.770 (5)
O3A0.30678 (12)0.5098 (4)0.06838 (17)0.0339 (6)0.770 (5)
N1A0.1841 (3)0.2416 (10)0.1078 (3)0.0233 (9)0.770 (5)
N2A0.1416 (3)0.1153 (13)0.1392 (4)0.0299 (11)0.770 (5)
C1A0.1437 (4)0.3491 (9)0.0250 (3)0.0435 (13)0.770 (5)
H1AA0.17030.22220.03630.052*0.770 (5)
C2A0.1033 (3)0.4963 (9)0.0814 (3)0.0473 (11)0.770 (5)
H2AA0.10100.46760.13210.057*0.770 (5)
C3A0.0659 (3)0.6880 (8)0.0620 (3)0.0416 (10)0.770 (5)
H3AA0.03960.78890.10000.050*0.770 (5)
C4A0.0676 (4)0.7296 (9)0.0128 (3)0.0381 (10)0.770 (5)
H4AA0.04140.85640.02480.046*0.770 (5)
C5A0.1078 (5)0.5851 (12)0.0702 (4)0.0301 (11)0.770 (5)
H5AA0.11090.61310.12110.036*0.770 (5)
C6A0.1432 (6)0.3969 (14)0.0479 (3)0.0292 (16)0.770 (5)
C7A0.2730 (2)0.0478 (7)0.1932 (3)0.0261 (8)0.770 (5)
C8A0.26327 (18)0.2104 (6)0.1337 (2)0.0231 (7)0.770 (5)
C12A0.54873 (13)0.3090 (5)0.14317 (17)0.0243 (6)0.770 (5)
C13A0.57473 (14)0.1083 (5)0.18318 (18)0.0274 (6)0.770 (5)
H13A0.54150.02870.20570.033*0.770 (5)
C14A0.6501 (2)0.0248 (8)0.1899 (3)0.0292 (8)0.770 (5)
H14A0.66770.10860.21720.035*0.770 (5)
C15A0.6983 (4)0.1445 (18)0.1551 (9)0.033 (2)0.770 (5)
C16A0.6744 (3)0.3462 (14)0.1168 (5)0.0332 (15)0.770 (5)
H16A0.70850.42780.09580.040*0.770 (5)
C17A0.59879 (19)0.4272 (7)0.1096 (2)0.0267 (7)0.770 (5)
H17A0.58170.56090.08230.032*0.770 (5)
C9A0.32136 (14)0.3360 (5)0.10637 (19)0.0266 (6)0.770 (5)
C10A0.40246 (13)0.2259 (5)0.12510 (16)0.0245 (6)0.770 (5)
H10A0.41090.12840.17040.029*0.770 (5)
C11A0.46785 (13)0.4009 (4)0.13558 (15)0.0241 (6)0.770 (5)
H11A0.45420.51400.09430.029*0.770 (5)
Br1B0.3986 (4)0.0778 (11)0.0224 (4)0.0432 (10)0.230 (5)
Br2B0.4661 (2)0.5668 (4)0.2298 (2)0.0207 (6)0.230 (5)
Br3B0.8041 (3)0.0491 (10)0.1649 (3)0.0645 (14)0.230 (5)
O1B0.2081 (8)0.011 (3)0.1999 (11)0.025 (3)*0.230 (5)
O2B0.3419 (6)0.015 (2)0.2543 (7)0.025 (3)*0.230 (5)
O3B0.3133 (5)0.5587 (14)0.0938 (5)0.035 (2)*0.230 (5)
N1B0.1956 (8)0.248 (4)0.1157 (11)0.025 (4)*0.230 (5)
N2B0.1529 (8)0.109 (4)0.1467 (12)0.016 (3)*0.230 (5)
C1B0.1377 (11)0.305 (3)0.0245 (9)0.021 (3)*0.230 (5)
H1BA0.15800.16390.03320.026*0.230 (5)
C2B0.0980 (11)0.437 (2)0.0865 (9)0.035 (4)*0.230 (5)
H2BA0.09600.38980.13570.042*0.230 (5)
C3B0.0620 (10)0.635 (2)0.0751 (9)0.031 (3)*0.230 (5)
H3BA0.03100.71610.11640.037*0.230 (5)
C4B0.0718 (13)0.714 (3)0.0023 (10)0.031 (4)*0.230 (5)
H4BA0.05160.85650.00550.037*0.230 (5)
C5B0.112 (2)0.581 (5)0.0605 (12)0.038 (6)*0.230 (5)
H5BA0.11440.63060.10950.045*0.230 (5)
C6B0.1480 (19)0.378 (5)0.0502 (9)0.022 (5)*0.230 (5)
C7B0.2854 (7)0.064 (3)0.2074 (7)0.015 (3)*0.230 (5)
C8B0.2729 (6)0.237 (2)0.1508 (6)0.019 (3)*0.230 (5)
C12B0.5443 (5)0.2546 (16)0.1212 (5)0.023 (2)*0.230 (5)
C13B0.5719 (6)0.0563 (17)0.1606 (6)0.029 (3)*0.230 (5)
H13B0.53740.03750.17710.035*0.230 (5)
C14B0.6499 (8)0.005 (3)0.1759 (10)0.032 (4)*0.230 (5)
H14B0.66760.14320.20000.038*0.230 (5)
C15B0.7008 (10)0.142 (5)0.155 (3)0.019 (6)*0.230 (5)
C16B0.6757 (10)0.331 (4)0.1083 (16)0.018 (3)*0.230 (5)
H16B0.70960.41480.08750.022*0.230 (5)
C17B0.5971 (7)0.388 (2)0.0948 (8)0.026 (3)*0.230 (5)
H17B0.57860.51990.06700.031*0.230 (5)
C9B0.3306 (5)0.3857 (16)0.1293 (6)0.025 (2)*0.230 (5)
C10B0.4170 (4)0.3055 (17)0.1585 (5)0.029 (2)0.230 (5)
H10B0.42230.15660.18430.035*0.230 (5)
C11B0.4576 (4)0.3139 (16)0.0966 (5)0.032 (2)0.230 (5)
H11B0.45030.46550.07250.038*0.230 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br1A0.0304 (2)0.0336 (3)0.0315 (5)0.0036 (2)0.0040 (3)0.0067 (3)
Br2A0.0259 (3)0.0618 (6)0.0411 (4)0.0048 (3)0.0101 (3)0.0172 (4)
Br3A0.0247 (4)0.0442 (3)0.0324 (3)0.0101 (2)0.0065 (2)0.0044 (2)
O1A0.0256 (15)0.0239 (12)0.0370 (18)0.0000 (14)0.0119 (15)0.0039 (9)
O2A0.0259 (13)0.0293 (13)0.0317 (16)0.0041 (11)0.0061 (11)0.0065 (12)
O3A0.0259 (10)0.0315 (12)0.0420 (15)0.0016 (8)0.0054 (10)0.0170 (11)
N1A0.0199 (14)0.0208 (13)0.0299 (18)0.0014 (13)0.0080 (12)0.0024 (12)
N2A0.0267 (19)0.0269 (15)0.034 (2)0.0022 (17)0.0050 (17)0.0016 (12)
C1A0.047 (2)0.040 (3)0.048 (2)0.004 (2)0.0208 (15)0.0047 (19)
C2A0.054 (2)0.056 (3)0.0329 (18)0.000 (2)0.0135 (15)0.0065 (19)
C3A0.0350 (17)0.035 (2)0.046 (3)0.0005 (16)0.0032 (15)0.0080 (18)
C4A0.0311 (17)0.0349 (19)0.043 (3)0.0083 (11)0.001 (2)0.0001 (18)
C5A0.0250 (17)0.0277 (19)0.034 (2)0.0012 (10)0.0011 (19)0.0035 (15)
C6A0.022 (2)0.028 (3)0.036 (2)0.0023 (12)0.0047 (11)0.0061 (12)
C7A0.0251 (17)0.0225 (14)0.030 (2)0.0001 (12)0.0070 (14)0.0037 (15)
C8A0.0212 (14)0.0225 (14)0.0239 (16)0.0007 (9)0.0035 (12)0.0004 (13)
C12A0.0218 (11)0.0239 (13)0.0265 (14)0.0024 (9)0.0057 (10)0.0035 (11)
C13A0.0254 (12)0.0295 (14)0.0277 (15)0.0032 (10)0.0079 (10)0.0007 (12)
C14A0.0269 (15)0.0287 (17)0.030 (2)0.0057 (11)0.0041 (12)0.0021 (16)
C15A0.021 (2)0.045 (3)0.030 (2)0.0018 (11)0.0034 (11)0.0086 (12)
C16A0.0256 (16)0.045 (3)0.032 (3)0.0077 (12)0.0123 (13)0.005 (2)
C17A0.0276 (14)0.0241 (16)0.0286 (18)0.0012 (10)0.0083 (12)0.0004 (15)
C9A0.0225 (12)0.0277 (14)0.0279 (15)0.0012 (10)0.0042 (10)0.0012 (12)
C10A0.0218 (11)0.0253 (14)0.0247 (14)0.0001 (9)0.0035 (10)0.0024 (10)
C11A0.0217 (11)0.0252 (13)0.0250 (14)0.0001 (9)0.0054 (9)0.0019 (10)
Br1B0.0388 (8)0.057 (2)0.0294 (14)0.0112 (12)0.0026 (8)0.0042 (12)
Br2B0.0323 (12)0.0050 (8)0.0308 (10)0.0039 (6)0.0186 (8)0.0053 (6)
Br3B0.0315 (16)0.096 (3)0.070 (2)0.0027 (15)0.0214 (14)0.0156 (16)
C10B0.022 (4)0.029 (5)0.033 (5)0.002 (3)0.001 (4)0.004 (4)
C11B0.027 (4)0.032 (5)0.032 (5)0.005 (3)0.001 (3)0.001 (4)
Geometric parameters (Å, º) top
Br1A—C10A1.964 (4)Br1B—C11B2.010 (12)
Br2A—C11A2.004 (3)Br2B—C10B2.036 (11)
Br3A—C15A1.913 (5)Br3B—C15B1.867 (13)
O1A—N2A1.374 (5)O1B—N2B1.367 (13)
O1A—C7A1.423 (5)O1B—C7B1.407 (13)
O2A—C7A1.212 (4)O2B—C7B1.214 (12)
O3A—C9A1.215 (3)O3B—C9B1.193 (11)
N1A—N2A1.293 (4)N1B—N2B1.334 (14)
N1A—C8A1.363 (4)N1B—C8B1.344 (12)
N1A—C6A1.450 (5)N1B—C6B1.469 (13)
C1A—C6A1.362 (5)C1B—C2B1.386 (14)
C1A—C2A1.379 (5)C1B—C6B1.392 (13)
C1A—H1AA0.9300C1B—H1BA0.9300
C2A—C3A1.393 (5)C2B—C3B1.365 (14)
C2A—H2AA0.9300C2B—H2BA0.9300
C3A—C4A1.380 (6)C3B—C4B1.370 (14)
C3A—H3AA0.9300C3B—H3BA0.9300
C4A—C5A1.379 (5)C4B—C5B1.403 (15)
C4A—H4AA0.9300C4B—H4BA0.9300
C5A—C6A1.379 (6)C5B—C6B1.382 (14)
C5A—H5AA0.9300C5B—H5BA0.9300
C7A—C8A1.415 (4)C7B—C8B1.419 (12)
C8A—C9A1.458 (3)C8B—C9B1.472 (11)
C12A—C13A1.390 (3)C12B—C13B1.378 (11)
C12A—C17A1.391 (3)C12B—C17B1.400 (12)
C12A—C11A1.499 (3)C12B—C11B1.515 (10)
C13A—C14A1.393 (4)C13B—C14B1.378 (13)
C13A—H13A0.9300C13B—H13B0.9300
C14A—C15A1.385 (6)C14B—C15B1.374 (14)
C14A—H14A0.9300C14B—H14B0.9300
C15A—C16A1.374 (6)C15B—C16B1.389 (14)
C16A—C17A1.391 (5)C16B—C17B1.384 (14)
C16A—H16A0.9300C16B—H16B0.9300
C17A—H17A0.9300C17B—H17B0.9300
C9A—C10A1.523 (3)C9B—C10B1.547 (10)
C10A—C11A1.515 (3)C10B—C11B1.497 (11)
C10A—H10A0.9800C10B—H10B0.9800
C11A—H11A0.9800C11B—H11B0.9800
N2A—O1A—C7A110.4 (4)N2B—O1B—C7B113.3 (12)
N2A—N1A—C8A116.0 (4)N2B—N1B—C8B113.0 (11)
N2A—N1A—C6A117.4 (5)N2B—N1B—C6B113.1 (17)
C8A—N1A—C6A126.6 (5)C8B—N1B—C6B133.9 (18)
N1A—N2A—O1A104.6 (4)N1B—N2B—O1B103.6 (12)
C6A—C1A—C2A117.4 (5)C2B—C1B—C6B122.0 (14)
C6A—C1A—H1AA121.3C2B—C1B—H1BA119.0
C2A—C1A—H1AA121.3C6B—C1B—H1BA119.0
C1A—C2A—C3A119.7 (4)C3B—C2B—C1B119.9 (14)
C1A—C2A—H2AA120.1C3B—C2B—H2BA120.1
C3A—C2A—H2AA120.1C1B—C2B—H2BA120.1
C4A—C3A—C2A120.6 (4)C2B—C3B—C4B119.5 (14)
C4A—C3A—H3AA119.7C2B—C3B—H3BA120.2
C2A—C3A—H3AA119.7C4B—C3B—H3BA120.2
C5A—C4A—C3A120.6 (4)C3B—C4B—C5B120.4 (15)
C5A—C4A—H4AA119.7C3B—C4B—H4BA119.8
C3A—C4A—H4AA119.7C5B—C4B—H4BA119.8
C4A—C5A—C6A116.4 (5)C6B—C5B—C4B120.8 (16)
C4A—C5A—H5AA121.8C6B—C5B—H5BA119.6
C6A—C5A—H5AA121.8C4B—C5B—H5BA119.6
C1A—C6A—C5A125.1 (5)C5B—C6B—C1B117.0 (13)
C1A—C6A—N1A118.2 (5)C5B—C6B—N1B121.1 (16)
C5A—C6A—N1A116.6 (5)C1B—C6B—N1B122.0 (16)
O2A—C7A—C8A136.4 (4)O2B—C7B—O1B122.8 (12)
O2A—C7A—O1A119.3 (4)O2B—C7B—C8B135.8 (12)
C8A—C7A—O1A104.3 (3)O1B—C7B—C8B101.4 (10)
N1A—C8A—C7A104.6 (3)N1B—C8B—C7B108.4 (10)
N1A—C8A—C9A124.7 (3)N1B—C8B—C9B122.3 (10)
C7A—C8A—C9A130.6 (3)C7B—C8B—C9B129.3 (10)
C13A—C12A—C17A119.4 (2)C13B—C12B—C17B118.1 (9)
C13A—C12A—C11A121.3 (2)C13B—C12B—C11B122.1 (8)
C17A—C12A—C11A119.4 (2)C17B—C12B—C11B119.3 (9)
C12A—C13A—C14A120.7 (3)C14B—C13B—C12B121.0 (11)
C12A—C13A—H13A119.6C14B—C13B—H13B119.5
C14A—C13A—H13A119.6C12B—C13B—H13B119.5
C15A—C14A—C13A118.7 (4)C15B—C14B—C13B118.6 (13)
C15A—C14A—H14A120.7C15B—C14B—H14B120.7
C13A—C14A—H14A120.7C13B—C14B—H14B120.7
C16A—C15A—C14A121.5 (5)C14B—C15B—C16B122.9 (15)
C16A—C15A—Br3A121.3 (4)C14B—C15B—Br3B119.4 (12)
C14A—C15A—Br3A117.1 (4)C16B—C15B—Br3B115.5 (12)
C15A—C16A—C17A119.5 (5)C17B—C16B—C15B115.8 (14)
C15A—C16A—H16A120.2C17B—C16B—H16B122.1
C17A—C16A—H16A120.2C15B—C16B—H16B122.1
C12A—C17A—C16A120.2 (4)C16B—C17B—C12B122.7 (13)
C12A—C17A—H17A119.9C16B—C17B—H17B118.7
C16A—C17A—H17A119.9C12B—C17B—H17B118.7
O3A—C9A—C8A123.7 (2)O3B—C9B—C8B123.4 (9)
O3A—C9A—C10A121.3 (2)O3B—C9B—C10B121.6 (9)
C8A—C9A—C10A114.9 (2)C8B—C9B—C10B115.0 (8)
C11A—C10A—C9A112.6 (2)C11B—C10B—C9B111.4 (7)
C11A—C10A—Br1A109.35 (19)C11B—C10B—Br2B104.3 (7)
C9A—C10A—Br1A103.21 (18)C9B—C10B—Br2B101.7 (6)
C11A—C10A—H10A110.5C11B—C10B—H10B112.9
C9A—C10A—H10A110.5C9B—C10B—H10B112.9
Br1A—C10A—H10A110.5Br2B—C10B—H10B112.9
C12A—C11A—C10A116.6 (2)C10B—C11B—C12B115.3 (7)
C12A—C11A—Br2A107.83 (17)C10B—C11B—Br1B102.5 (7)
C10A—C11A—Br2A102.68 (17)C12B—C11B—Br1B109.8 (6)
C12A—C11A—H11A109.8C10B—C11B—H11B109.7
C10A—C11A—H11A109.8C12B—C11B—H11B109.7
Br2A—C11A—H11A109.8Br1B—C11B—H11B109.7
C8A—N1A—N2A—O1A3.2 (9)C8B—N1B—N2B—O1B6 (3)
C6A—N1A—N2A—O1A178.2 (6)C6B—N1B—N2B—O1B174 (2)
C7A—O1A—N2A—N1A1.8 (9)C7B—O1B—N2B—N1B5 (3)
C6A—C1A—C2A—C3A1.7 (10)C6B—C1B—C2B—C3B6 (3)
C1A—C2A—C3A—C4A1.3 (8)C1B—C2B—C3B—C4B6 (3)
C2A—C3A—C4A—C5A1.5 (10)C2B—C3B—C4B—C5B6 (4)
C3A—C4A—C5A—C6A2.0 (13)C3B—C4B—C5B—C6B5 (5)
C2A—C1A—C6A—C5A2.4 (15)C4B—C5B—C6B—C1B4 (6)
C2A—C1A—C6A—N1A178.8 (7)C4B—C5B—C6B—N1B175 (3)
C4A—C5A—C6A—C1A2.5 (17)C2B—C1B—C6B—C5B4 (5)
C4A—C5A—C6A—N1A178.6 (8)C2B—C1B—C6B—N1B175 (2)
N2A—N1A—C6A—C1A109.4 (10)N2B—N1B—C6B—C5B84 (4)
C8A—N1A—C6A—C1A69.1 (12)C8B—N1B—C6B—C5B96 (4)
N2A—N1A—C6A—C5A71.7 (12)N2B—N1B—C6B—C1B96 (4)
C8A—N1A—C6A—C5A109.9 (10)C8B—N1B—C6B—C1B83 (4)
N2A—O1A—C7A—O2A178.0 (6)N2B—O1B—C7B—O2B176 (2)
N2A—O1A—C7A—C8A0.1 (7)N2B—O1B—C7B—C8B2 (2)
N2A—N1A—C8A—C7A3.3 (8)N2B—N1B—C8B—C7B5 (3)
C6A—N1A—C8A—C7A178.3 (6)C6B—N1B—C8B—C7B175 (2)
N2A—N1A—C8A—C9A179.6 (6)N2B—N1B—C8B—C9B176.1 (18)
C6A—N1A—C8A—C9A2.0 (9)C6B—N1B—C8B—C9B4 (4)
O2A—C7A—C8A—N1A175.7 (6)O2B—C7B—C8B—N1B180 (2)
O1A—C7A—C8A—N1A1.8 (5)O1B—C7B—C8B—N1B1 (2)
O2A—C7A—C8A—C9A0.3 (9)O2B—C7B—C8B—C9B1 (3)
O1A—C7A—C8A—C9A177.9 (4)O1B—C7B—C8B—C9B179.6 (15)
C17A—C12A—C13A—C14A0.0 (5)C17B—C12B—C13B—C14B2.2 (16)
C11A—C12A—C13A—C14A179.9 (3)C11B—C12B—C13B—C14B173.7 (11)
C12A—C13A—C14A—C15A0.8 (10)C12B—C13B—C14B—C15B4 (3)
C13A—C14A—C15A—C16A2.3 (18)C13B—C14B—C15B—C16B11 (5)
C13A—C14A—C15A—Br3A177.9 (6)C13B—C14B—C15B—Br3B173 (2)
C14A—C15A—C16A—C17A3 (2)C14B—C15B—C16B—C17B11 (6)
Br3A—C15A—C16A—C17A178.4 (8)Br3B—C15B—C16B—C17B174 (2)
C13A—C12A—C17A—C16A0.7 (7)C15B—C16B—C17B—C12B5 (4)
C11A—C12A—C17A—C16A179.2 (5)C13B—C12B—C17B—C16B2 (2)
C15A—C16A—C17A—C12A2.2 (13)C11B—C12B—C17B—C16B173.4 (18)
N1A—C8A—C9A—O3A14.4 (6)N1B—C8B—C9B—O3B19 (2)
C7A—C8A—C9A—O3A160.9 (4)C7B—C8B—C9B—O3B162.4 (13)
N1A—C8A—C9A—C10A162.3 (4)N1B—C8B—C9B—C10B163.2 (16)
C7A—C8A—C9A—C10A22.4 (6)C7B—C8B—C9B—C10B15.8 (17)
O3A—C9A—C10A—C11A34.0 (4)O3B—C9B—C10B—C11B48.6 (13)
C8A—C9A—C10A—C11A149.2 (3)C8B—C9B—C10B—C11B133.2 (10)
O3A—C9A—C10A—Br1A83.8 (3)O3B—C9B—C10B—Br2B62.0 (10)
C8A—C9A—C10A—Br1A93.0 (3)C8B—C9B—C10B—Br2B116.1 (8)
C13A—C12A—C11A—C10A37.9 (4)C9B—C10B—C11B—C12B175.8 (7)
C17A—C12A—C11A—C10A142.2 (3)Br2B—C10B—C11B—C12B66.9 (8)
C13A—C12A—C11A—Br2A76.9 (3)C9B—C10B—C11B—Br1B64.9 (8)
C17A—C12A—C11A—Br2A103.0 (3)Br2B—C10B—C11B—Br1B173.8 (4)
C9A—C10A—C11A—C12A171.6 (2)C13B—C12B—C11B—C10B51.9 (13)
Br1A—C10A—C11A—C12A57.5 (3)C17B—C12B—C11B—C10B136.7 (10)
C9A—C10A—C11A—Br2A70.8 (2)C13B—C12B—C11B—Br1B63.2 (10)
Br1A—C10A—C11A—Br2A175.09 (13)C17B—C12B—C11B—Br1B108.2 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C10A—H10A···O2A0.982.403.168 (4)135
C14A—H14A···Br3Ai0.932.913.809 (5)163
Symmetry code: (i) x+3/2, y1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC17H11Br3N2O3
Mr531.01
Crystal system, space groupMonoclinic, P21/n
Temperature (K)100
a, b, c (Å)17.6996 (3), 5.8322 (1), 18.2445 (3)
β (°) 105.973 (1)
V3)1810.62 (5)
Z4
Radiation typeMo Kα
µ (mm1)6.70
Crystal size (mm)0.43 × 0.38 × 0.12
Data collection
DiffractometerBruker SMART APEXII CCD area-detector
Absorption correctionMulti-scan
(SADABS; Bruker, 2009)
Tmin, Tmax0.159, 0.505
No. of measured, independent and
observed [I > 2σ(I)] reflections
20140, 5243, 4218
Rint0.028
(sin θ/λ)max1)0.704
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.025, 0.055, 1.02
No. of reflections5243
No. of parameters352
No. of restraints207
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.50, 0.37

Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C10A—H10A···O2A0.982.403.168 (4)135
C14A—H14A···Br3Ai0.932.913.809 (5)163
Symmetry code: (i) x+3/2, y1/2, z+1/2.
 

Footnotes

Thomson Reuters ResearcherID: A-3561-2009.

Acknowledgements

HKF and TSH thank Universiti Sains Malaysia (USM) for the Research University Grant (1001/PFIZIK/811160). TSH also thanks USM for the award of a research fellowship.

References

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