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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Jun 25;70(Pt 7):o818. doi: 10.1107/S1600536814014603

2-Bromo-1-[1-(4-bromo­phen­yl)-5-methyl-1H-1,2,3-triazol-4-yl]ethanone

Alexander S Bunev a,*, Marina A Troshina a, Gennady I Ostapenko a, Andzhela P Pavlova b, Victor N Khrustalev c
PMCID: PMC4120528  PMID: 25161595

Abstract

The asymmetric unit of the title compound, C11H9Br2N3O, contains two crystallographically independent mol­ecules with similar geometries; the Br—C—C=O torsion angles are 1.2 (4) and −2.8 (4)°, and the benzene and triazole rings are inclined o one another by 51.90 (16) and 51.88 (16)°. The two molecules are related by a pseudo-screw 21 axis directed along [100]. In the crystal, mol­ecules are linked into a three-dimensional network by weak C—H⋯O and C—H⋯N hydrogen bonds and secondary Br⋯Br [3.5991 (8) and 3.6503 (9) Å] inter­actions.

Keywords: crystal structure

Related literature  

For applications of 1,2,3-triazoles, see recent reviews by Agalave et al. (2011); Thirumurugan et al. (2013). For the crystal structures of related compounds, see: Danence et al. (2011); Zeghada et al. (2011); Abdel-Wahab, Abdel-Latif et al. (2013); Abdel-Wahab, Mohamed et al. (2013).graphic file with name e-70-0o818-scheme1.jpg

Experimental  

Crystal data  

  • C11H9Br2N3O

  • M r = 359.03

  • Monoclinic, Inline graphic

  • a = 3.9699 (10) Å

  • b = 19.437 (5) Å

  • c = 15.402 (4) Å

  • β = 90.908 (3)°

  • V = 1188.3 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 6.81 mm−1

  • T = 100 K

  • 0.30 × 0.03 × 0.03 mm

Data collection  

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2003) T min = 0.235, T max = 0.822

  • 18272 measured reflections

  • 6924 independent reflections

  • 6426 reflections with I > 2σ(I)

  • R int = 0.028

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.028

  • wR(F 2) = 0.067

  • S = 1.04

  • 6924 reflections

  • 309 parameters

  • 2 restraints

  • H-atom parameters constrained

  • Δρmax = 0.72 e Å−3

  • Δρmin = −0.59 e Å−3

  • Absolute structure: Flack (1983), 3428 Friedel pairs

  • Absolute structure parameter: 0.032 (7)

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2001); 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.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814014603/cv5467sup1.cif

e-70-0o818-sup1.cif (30.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814014603/cv5467Isup2.hkl

e-70-0o818-Isup2.hkl (338.8KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814014603/cv5467Isup3.cml

CCDC reference: 1009335

Additional supporting information: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C10—H10⋯O1i 0.95 2.44 3.205 (4) 137
C13—H13B⋯N6ii 0.99 2.49 3.467 (4) 170
C21—H21⋯O2iii 0.95 2.45 3.210 (4) 137
C24—H24B⋯N3 0.99 2.49 3.482 (4) 177

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

The authors are grateful to the Ministry of Education and Science of the Russian Federation (State program No. 426).

supplementary crystallographic information

S1. Comment

1-H-1,2,3-Triazole occupies a special place in heterocyclic chemistry because it is the core structure of many agents of various interests (used as pharmaceuticals, afrochemicals etc.). These compounds and their derivatives demonstrate antiviral, antimicrobial, anticancer activities as well as the inhibition activity of VIM-2 Metallo-β-Lactamase, and α-Glucosidases (Agalave et al., 2011; Thirumurugan et al., 2013). In this work, the title compound was prepared by the reaction of 1-(1-(4-bromophenyl)-5-methyl-1H-1,2,3-triazol-4-yl)ethanone with bromine (Figure 1), and its structure was unambiguously established by the X-ray diffraction study.

The title compound (I) crystallizes in the non-centrosymmetric monoclinic space group Pn with two crystallographically independent molecules in the asymmetric unit (Figure 2). The two crystallographically independent molecules are related by pseudo-screw axis 21 directed in [100] and, consequently, have very similar geometries (Figure 3). The position of the pseudo-screw axis 21 with the approximate coordinates of (x, 0.75, 0.55) is shifted relative to the crystallographic position of (x, 0.75, 0.75) by ca. 0.20 Å towards the c axis, apparently, due to the formation of the more dense crystal packing as well as different non-valent intermolecular interactions.

The bond lengths and angles within the molecules of I are in a good agreement with those found in the related compounds (Danence et al. 2011; Zeghada et al. 2011; Abdel-Wahab, Abdel-Latif et al. 2013; Abdel-Wahab, Mohamed et al. 2013). The 2-bromo-1-ethanone substituent in the molecules of I has a significantly flattened conformation (the Br–C–C═O torsion angles are 1.2 (4) and -2.8 (4)° for the two independent molecules, respectively), with the carbonyl group directed toward the methyl substituent, and lies almost within the triazole plane (r.m.s. deviations are 0.037 and 0.023 Å for the two independent molecules, respectively) (Figure 2). The bromo-benzene substituent is twisted by 52.30 (6) and 51.81 (6)° (for the two independent molecules, respectively) relative to this main plane of the molecule.

In the crystal, the molecules of I are linked into three-dimensional framework by intermolecular C–H···O and C–H···N hydrogen bonds (Table 1) as well as secondary Br1···Br2i (3.5991 (8) Å) and Br3···Br4ii (3.6503 (9) Å) interactions [symmetry codes: (i) x, y, z+1; (ii) x, y, z-1].

S2. Experimental

Bromine (1.6 g, 10 mmol) was slowly added to a solution of 1-(1-(4-bromophenyl)-5-methyl-1H-1,2,3-triazol-4-yl)ethanone (2.8 g, 10 mmol) in AcOH (30 mL). The mixture was stirred at 80 oC for 20 min. Then the reaction mixture was cooled to room temperature. The crude precipitate formed was filtrated, washed with H2O (20 mL), dried, and re-crystallized from EtOH. Yield is 83%. The single-crystals of the product I were obtained by slow crystallization from EtOH. M.p. = 398-399 K. IR (KBr), ν/cm-1: 3301, 1693, 1550, 1495, 1181, 972, 872. 1H NMR (600 MHz, DMSO-d6, 304 K): 2.55 (s, 3H), 4.88 (s, 2H), 7.62 (d, 2H, J = 8.8), 7.87 (d, 2H, J = 8.8). Anal. Calcd for C11H9Br2N3O: C, 42.00; H, 2.88. Found: C, 42.07; H, 2.92.

S3. Refinement

The absolute configuration of I was objectively determined by the refinement of Flack parameter (3428 (99%) Friedel pairs measured) to 0.032 (7). The calculated Hooft parameter is equal to 0.023 (6).

All hydrogen atoms were placed in the calculated positions with C–H = 0.95 (aryl-H), 0.98 (methyl-H) and 0.99 (methylene-H) Å and refined in the riding model with fixed isotropic displacement parameters: Uiso(H) = 1.2-1.5Ueq(C).

Figures

Fig. 1.

Fig. 1.

The synthesis of 7-nitro-2-phenylimidazo[2,1-b][1,3]benzothiazole.

Fig. 2.

Fig. 2.

Two independent molecules in the asymmetric unit of I. Displacement ellipsoids are presented at the 50% probability level. H atoms are depicted as small spheres of arbitrary radius.

Fig. 3.

Fig. 3.

Superposition of the two independent molecules of I.

Crystal data

C11H9Br2N3O F(000) = 696
Mr = 359.03 Dx = 2.007 Mg m3
Monoclinic, Pn Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P -2yac Cell parameters from 9920 reflections
a = 3.9699 (10) Å θ = 2.5–32.2°
b = 19.437 (5) Å µ = 6.81 mm1
c = 15.402 (4) Å T = 100 K
β = 90.908 (3)° Needle, colourless
V = 1188.3 (5) Å3 0.30 × 0.03 × 0.03 mm
Z = 4

Data collection

Bruker APEXII CCD diffractometer 6924 independent reflections
Radiation source: fine-focus sealed tube 6426 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.028
φ and ω scans θmax = 30.0°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2003) h = −5→5
Tmin = 0.235, Tmax = 0.822 k = −26→27
18272 measured reflections l = −21→21

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.028 H-atom parameters constrained
wR(F2) = 0.067 w = 1/[σ2(Fo2) + (0.0221P)2 + 0.4369P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.001
6924 reflections Δρmax = 0.72 e Å3
309 parameters Δρmin = −0.59 e Å3
2 restraints Absolute structure: Flack (1983), 3428 Friedel pairs
Primary atom site location: structure-invariant direct methods Absolute structure parameter: 0.032 (7)

Special details

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
Br1 1.07896 (7) 0.863924 (17) 1.13454 (2) 0.02912 (7)
Br2 0.64876 (8) 0.877518 (19) 0.33776 (2) 0.03474 (8)
O1 0.8585 (6) 0.94649 (11) 0.50458 (14) 0.0356 (5)
N1 0.7274 (6) 0.85632 (12) 0.75006 (16) 0.0257 (5)
N2 0.5627 (7) 0.79965 (16) 0.71724 (18) 0.0297 (6)
N3 0.5412 (7) 0.80839 (14) 0.63358 (19) 0.0281 (5)
C4 0.6933 (8) 0.86928 (14) 0.61085 (19) 0.0251 (5)
C5 0.8151 (7) 0.90045 (14) 0.68650 (18) 0.0250 (5)
C6 0.8065 (7) 0.85860 (15) 0.84105 (19) 0.0257 (5)
C7 0.9625 (7) 0.80248 (15) 0.87919 (18) 0.0270 (6)
H7 1.0134 0.7630 0.8454 0.032*
C8 1.0442 (8) 0.80396 (16) 0.9666 (2) 0.0290 (6)
H8 1.1526 0.7658 0.9936 0.035*
C9 0.9654 (7) 0.86206 (14) 1.01434 (18) 0.0243 (5)
C10 0.8081 (8) 0.91854 (15) 0.97703 (19) 0.0282 (6)
H10 0.7562 0.9578 1.0111 0.034*
C11 0.7278 (8) 0.91690 (15) 0.8897 (2) 0.0281 (6)
H11 0.6197 0.9551 0.8627 0.034*
C12 0.7233 (7) 0.89258 (15) 0.52097 (19) 0.0258 (5)
C13 0.5797 (8) 0.84371 (17) 0.4533 (2) 0.0270 (6)
H13A 0.3354 0.8377 0.4627 0.032*
H13B 0.6890 0.7982 0.4598 0.032*
C14 1.0031 (8) 0.96530 (16) 0.7007 (2) 0.0304 (6)
H14A 1.1297 0.9626 0.7557 0.046*
H14B 0.8445 1.0039 0.7027 0.046*
H14C 1.1598 0.9724 0.6530 0.046*
Br3 0.55988 (7) 0.633881 (18) −0.03542 (2) 0.03091 (8)
Br4 0.09749 (12) 0.62103 (2) 0.75847 (3) 0.04919 (11)
O2 0.3422 (6) 0.55351 (11) 0.59535 (15) 0.0374 (5)
N4 0.2428 (7) 0.64530 (13) 0.34827 (17) 0.0287 (5)
N5 0.0796 (7) 0.70220 (15) 0.3795 (2) 0.0320 (6)
N6 0.0522 (7) 0.69383 (14) 0.46281 (19) 0.0304 (5)
C15 0.2015 (8) 0.63260 (15) 0.4854 (2) 0.0264 (6)
C16 0.3230 (8) 0.60064 (15) 0.41271 (19) 0.0268 (5)
C17 0.3215 (7) 0.64193 (15) 0.2580 (2) 0.0274 (6)
C18 0.4783 (8) 0.69686 (15) 0.21998 (19) 0.0281 (6)
H18 0.5373 0.7362 0.2535 0.034*
C19 0.5504 (8) 0.69455 (16) 0.1318 (2) 0.0274 (6)
H19 0.6588 0.7321 0.1044 0.033*
C20 0.4609 (7) 0.63628 (15) 0.08477 (19) 0.0261 (6)
C21 0.3038 (7) 0.58060 (15) 0.12237 (19) 0.0278 (6)
H21 0.2471 0.5412 0.0888 0.033*
C22 0.2301 (8) 0.58320 (15) 0.21009 (19) 0.0272 (6)
H22 0.1196 0.5458 0.2373 0.033*
C23 0.2154 (8) 0.60812 (15) 0.5765 (2) 0.0286 (6)
C24 0.0729 (9) 0.65717 (17) 0.6432 (2) 0.0287 (6)
H24A −0.1653 0.6671 0.6279 0.034*
H24B 0.1990 0.7011 0.6412 0.034*
C25 0.5068 (8) 0.53557 (16) 0.4007 (2) 0.0300 (6)
H25A 0.6422 0.5385 0.3482 0.045*
H25B 0.3455 0.4976 0.3949 0.045*
H25C 0.6551 0.5273 0.4511 0.045*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.03673 (15) 0.02734 (16) 0.02318 (14) −0.00060 (12) −0.00311 (11) −0.00161 (13)
Br2 0.04801 (19) 0.03298 (17) 0.02315 (15) −0.00318 (14) −0.00196 (12) 0.00142 (13)
O1 0.0514 (14) 0.0268 (11) 0.0287 (11) −0.0091 (10) −0.0011 (10) 0.0018 (8)
N1 0.0319 (12) 0.0221 (11) 0.0229 (11) −0.0024 (9) 0.0001 (9) −0.0005 (9)
N2 0.0389 (14) 0.0273 (15) 0.0229 (13) −0.0062 (11) −0.0002 (10) −0.0017 (11)
N3 0.0363 (13) 0.0253 (13) 0.0226 (11) −0.0035 (11) −0.0004 (9) −0.0014 (11)
C4 0.0283 (13) 0.0211 (13) 0.0257 (13) 0.0016 (10) −0.0003 (11) −0.0007 (10)
C5 0.0290 (13) 0.0198 (12) 0.0261 (13) −0.0008 (10) −0.0028 (10) −0.0014 (10)
C6 0.0297 (13) 0.0254 (13) 0.0220 (12) 0.0005 (11) −0.0024 (11) −0.0008 (10)
C7 0.0344 (15) 0.0219 (13) 0.0247 (13) 0.0007 (11) 0.0026 (11) −0.0026 (10)
C8 0.0351 (14) 0.0228 (14) 0.0291 (15) 0.0025 (12) 0.0024 (11) 0.0005 (13)
C9 0.0293 (14) 0.0223 (13) 0.0213 (12) −0.0028 (10) −0.0010 (10) −0.0015 (10)
C10 0.0336 (15) 0.0216 (13) 0.0293 (14) 0.0007 (11) −0.0020 (12) −0.0028 (11)
C11 0.0320 (14) 0.0233 (13) 0.0291 (14) 0.0050 (11) −0.0009 (11) 0.0005 (11)
C12 0.0301 (13) 0.0233 (13) 0.0239 (13) 0.0005 (10) −0.0027 (10) −0.0004 (10)
C13 0.0317 (15) 0.0263 (16) 0.0230 (15) 0.0013 (12) 0.0022 (12) −0.0030 (13)
C14 0.0377 (16) 0.0213 (14) 0.0321 (15) −0.0044 (12) −0.0067 (13) 0.0017 (11)
Br3 0.03856 (16) 0.02766 (17) 0.02664 (16) 0.00068 (13) 0.00437 (12) −0.00241 (13)
Br4 0.0812 (3) 0.0374 (2) 0.02920 (19) 0.00705 (19) 0.00878 (18) 0.00159 (15)
O2 0.0526 (14) 0.0267 (11) 0.0331 (12) 0.0070 (10) 0.0034 (10) 0.0033 (9)
N4 0.0356 (13) 0.0220 (11) 0.0284 (12) 0.0018 (9) −0.0011 (10) −0.0014 (9)
N5 0.0417 (15) 0.0234 (14) 0.0309 (15) 0.0055 (11) −0.0008 (11) −0.0035 (12)
N6 0.0375 (13) 0.0245 (13) 0.0291 (13) 0.0048 (11) −0.0032 (10) −0.0029 (11)
C15 0.0299 (14) 0.0241 (14) 0.0252 (13) −0.0010 (11) 0.0035 (12) −0.0016 (10)
C16 0.0305 (14) 0.0222 (13) 0.0279 (13) −0.0015 (11) 0.0034 (11) 0.0000 (11)
C17 0.0275 (14) 0.0255 (14) 0.0292 (14) 0.0026 (11) −0.0005 (11) −0.0028 (11)
C18 0.0335 (15) 0.0225 (13) 0.0282 (14) −0.0024 (11) −0.0031 (11) −0.0016 (11)
C19 0.0340 (14) 0.0202 (13) 0.0279 (14) −0.0024 (12) −0.0035 (11) 0.0025 (13)
C20 0.0278 (14) 0.0250 (14) 0.0253 (13) 0.0018 (10) −0.0006 (11) −0.0027 (10)
C21 0.0336 (15) 0.0228 (13) 0.0269 (13) −0.0001 (11) −0.0003 (11) −0.0062 (10)
C22 0.0318 (14) 0.0240 (13) 0.0258 (13) −0.0060 (11) −0.0002 (11) −0.0021 (11)
C23 0.0332 (14) 0.0227 (13) 0.0300 (14) −0.0027 (11) 0.0014 (12) −0.0037 (11)
C24 0.0369 (15) 0.0241 (15) 0.0251 (15) −0.0011 (13) 0.0013 (12) 0.0015 (13)
C25 0.0358 (16) 0.0249 (15) 0.0294 (14) 0.0001 (12) 0.0040 (12) 0.0007 (11)

Geometric parameters (Å, º)

Br1—C9 1.899 (3) Br3—C20 1.899 (3)
Br2—C13 1.920 (3) Br4—C24 1.911 (3)
O1—C12 1.206 (4) O2—C23 1.208 (4)
N1—C5 1.351 (4) N4—C16 1.353 (4)
N1—N2 1.373 (4) N4—N5 1.373 (4)
N1—C6 1.432 (4) N4—C17 1.432 (4)
N2—N3 1.301 (4) N5—N6 1.299 (4)
N3—C4 1.376 (4) N6—C15 1.372 (4)
C4—C5 1.393 (4) C15—C16 1.375 (4)
C4—C12 1.463 (4) C15—C23 1.482 (4)
C5—C14 1.479 (4) C16—C25 1.473 (4)
C6—C7 1.381 (4) C17—C18 1.372 (4)
C6—C11 1.396 (4) C17—C22 1.404 (4)
C7—C8 1.380 (4) C18—C19 1.393 (5)
C7—H7 0.9500 C18—H18 0.9500
C8—C9 1.386 (4) C19—C20 1.388 (4)
C8—H8 0.9500 C19—H19 0.9500
C9—C10 1.384 (4) C20—C21 1.381 (4)
C10—C11 1.378 (4) C21—C22 1.388 (4)
C10—H10 0.9500 C21—H21 0.9500
C11—H11 0.9500 C22—H22 0.9500
C12—C13 1.515 (4) C23—C24 1.516 (4)
C13—H13A 0.9900 C24—H24A 0.9900
C13—H13B 0.9900 C24—H24B 0.9900
C14—H14A 0.9800 C25—H25A 0.9800
C14—H14B 0.9800 C25—H25B 0.9800
C14—H14C 0.9800 C25—H25C 0.9800
C5—N1—N2 111.7 (2) C16—N4—N5 111.5 (3)
C5—N1—C6 129.4 (2) C16—N4—C17 129.1 (3)
N2—N1—C6 118.7 (2) N5—N4—C17 119.3 (3)
N3—N2—N1 106.5 (3) N6—N5—N4 107.0 (3)
N2—N3—C4 110.0 (3) N5—N6—C15 108.5 (3)
N3—C4—C5 108.0 (3) N6—C15—C16 109.9 (3)
N3—C4—C12 123.3 (3) N6—C15—C23 121.9 (3)
C5—C4—C12 128.6 (3) C16—C15—C23 128.2 (3)
N1—C5—C4 103.9 (2) N4—C16—C15 103.1 (3)
N1—C5—C14 124.7 (3) N4—C16—C25 124.8 (3)
C4—C5—C14 131.4 (3) C15—C16—C25 132.1 (3)
C7—C6—C11 121.0 (3) C18—C17—C22 121.6 (3)
C7—C6—N1 118.8 (3) C18—C17—N4 119.1 (3)
C11—C6—N1 120.2 (3) C22—C17—N4 119.3 (3)
C8—C7—C6 119.7 (3) C17—C18—C19 119.5 (3)
C8—C7—H7 120.2 C17—C18—H18 120.2
C6—C7—H7 120.2 C19—C18—H18 120.2
C7—C8—C9 118.9 (3) C20—C19—C18 118.7 (3)
C7—C8—H8 120.6 C20—C19—H19 120.6
C9—C8—H8 120.6 C18—C19—H19 120.6
C10—C9—C8 122.0 (3) C21—C20—C19 122.3 (3)
C10—C9—Br1 119.2 (2) C21—C20—Br3 119.4 (2)
C8—C9—Br1 118.7 (2) C19—C20—Br3 118.3 (2)
C11—C10—C9 118.9 (3) C20—C21—C22 118.9 (3)
C11—C10—H10 120.6 C20—C21—H21 120.6
C9—C10—H10 120.6 C22—C21—H21 120.6
C10—C11—C6 119.5 (3) C21—C22—C17 119.0 (3)
C10—C11—H11 120.3 C21—C22—H22 120.5
C6—C11—H11 120.3 C17—C22—H22 120.5
O1—C12—C4 120.7 (3) O2—C23—C15 121.2 (3)
O1—C12—C13 124.4 (3) O2—C23—C24 123.3 (3)
C4—C12—C13 114.9 (3) C15—C23—C24 115.5 (3)
C12—C13—Br2 111.4 (2) C23—C24—Br4 112.6 (2)
C12—C13—H13A 109.3 C23—C24—H24A 109.1
Br2—C13—H13A 109.3 Br4—C24—H24A 109.1
C12—C13—H13B 109.3 C23—C24—H24B 109.1
Br2—C13—H13B 109.3 Br4—C24—H24B 109.1
H13A—C13—H13B 108.0 H24A—C24—H24B 107.8
C5—C14—H14A 109.5 C16—C25—H25A 109.5
C5—C14—H14B 109.5 C16—C25—H25B 109.5
H14A—C14—H14B 109.5 H25A—C25—H25B 109.5
C5—C14—H14C 109.5 C16—C25—H25C 109.5
H14A—C14—H14C 109.5 H25A—C25—H25C 109.5
H14B—C14—H14C 109.5 H25B—C25—H25C 109.5
C5—N1—N2—N3 −1.0 (4) C16—N4—N5—N6 −0.7 (4)
C6—N1—N2—N3 −176.0 (3) C17—N4—N5—N6 −177.2 (3)
N1—N2—N3—C4 0.9 (4) N4—N5—N6—C15 1.0 (4)
N2—N3—C4—C5 −0.5 (4) N5—N6—C15—C16 −1.0 (4)
N2—N3—C4—C12 177.5 (3) N5—N6—C15—C23 179.5 (3)
N2—N1—C5—C4 0.7 (3) N5—N4—C16—C15 0.0 (3)
C6—N1—C5—C4 175.0 (3) C17—N4—C16—C15 176.2 (3)
N2—N1—C5—C14 −178.3 (3) N5—N4—C16—C25 −178.4 (3)
C6—N1—C5—C14 −4.0 (5) C17—N4—C16—C25 −2.2 (5)
N3—C4—C5—N1 −0.2 (3) N6—C15—C16—N4 0.6 (3)
C12—C4—C5—N1 −178.0 (3) C23—C15—C16—N4 180.0 (3)
N3—C4—C5—C14 178.8 (3) N6—C15—C16—C25 178.8 (3)
C12—C4—C5—C14 1.0 (5) C23—C15—C16—C25 −1.8 (6)
C5—N1—C6—C7 −124.6 (3) C16—N4—C17—C18 −126.4 (3)
N2—N1—C6—C7 49.3 (4) N5—N4—C17—C18 49.5 (4)
C5—N1—C6—C11 55.1 (4) C16—N4—C17—C22 54.9 (4)
N2—N1—C6—C11 −131.0 (3) N5—N4—C17—C22 −129.2 (3)
C11—C6—C7—C8 −0.4 (5) C22—C17—C18—C19 −0.2 (5)
N1—C6—C7—C8 179.3 (3) N4—C17—C18—C19 −178.8 (3)
C6—C7—C8—C9 0.3 (5) C17—C18—C19—C20 0.0 (5)
C7—C8—C9—C10 −0.1 (5) C18—C19—C20—C21 −0.2 (5)
C7—C8—C9—Br1 −179.9 (2) C18—C19—C20—Br3 179.9 (2)
C8—C9—C10—C11 −0.1 (5) C19—C20—C21—C22 0.6 (5)
Br1—C9—C10—C11 179.7 (2) Br3—C20—C21—C22 −179.4 (2)
C9—C10—C11—C6 0.0 (5) C20—C21—C22—C17 −0.8 (4)
C7—C6—C11—C10 0.2 (5) C18—C17—C22—C21 0.7 (5)
N1—C6—C11—C10 −179.5 (3) N4—C17—C22—C21 179.3 (3)
N3—C4—C12—O1 179.9 (3) N6—C15—C23—O2 178.6 (3)
C5—C4—C12—O1 −2.6 (5) C16—C15—C23—O2 −0.7 (5)
N3—C4—C12—C13 −1.2 (4) N6—C15—C23—C24 −3.5 (4)
C5—C4—C12—C13 176.3 (3) C16—C15—C23—C24 177.1 (3)
O1—C12—C13—Br2 1.2 (4) O2—C23—C24—Br4 −2.8 (4)
C4—C12—C13—Br2 −177.6 (2) C15—C23—C24—Br4 179.4 (2)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C10—H10···O1i 0.95 2.44 3.205 (4) 137
C13—H13B···N6ii 0.99 2.49 3.467 (4) 170
C21—H21···O2iii 0.95 2.45 3.210 (4) 137
C24—H24B···N3 0.99 2.49 3.482 (4) 177

Symmetry codes: (i) x−1/2, −y+2, z+1/2; (ii) x+1, y, z; (iii) x−1/2, −y+1, z−1/2.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: CV5467).

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 datablock(s) global, I. DOI: 10.1107/S1600536814014603/cv5467sup1.cif

e-70-0o818-sup1.cif (30.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814014603/cv5467Isup2.hkl

e-70-0o818-Isup2.hkl (338.8KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814014603/cv5467Isup3.cml

CCDC reference: 1009335

Additional supporting information: crystallographic information; 3D view; checkCIF report


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