Abstract
In the title salt, C20H20N3O4 +·Br−, the dihedral angle between the benzene rings is 8.69 (16)°, and those between the benzene rings and the triazole ring are 69.98 (18) and 72.17 (18)°. In the crystal, C—H⋯Br hydrogen bonds link the cations and anions into chains along the c axis.
Related literature
For general background to triazole derivatives, see: Zanardi et al. (2011) ▶. For a related structure, see: Huang et al. (2010 ▶).
Experimental
Crystal data
C20H20N3O4 +·Br−
M r = 446.30
Orthorhombic,
a = 33.6880 (15) Å
b = 4.7962 (3) Å
c = 12.3337 (6) Å
V = 1992.81 (18) Å3
Z = 4
Cu Kα radiation
μ = 3.08 mm−1
T = 173 K
0.40 × 0.32 × 0.31 mm
Data collection
Oxford Diffraction Xcalibur Atlas Gemini Ultra diffractometer
Absorption correction: multi-scan (ABSPACK in CrysAlis PRO; Oxford Diffraction, 2006 ▶) T min = 0.372, T max = 0.449
6375 measured reflections
2709 independent reflections
2541 reflections with I > 2σ(I)
R int = 0.027
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.069
S = 1.05
2709 reflections
255 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.37 e Å−3
Δρmin = −0.24 e Å−3
Absolute structure: Flack (1983 ▶), 840 Friedel pairs
Flack parameter: 0.021 (18)
Data collection: CrysAlis PRO (Oxford Diffraction, 2006 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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: WinGX (Farrugia, 1999) ▶ and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812016728/ng5263sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016728/ng5263Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812016728/ng5263Isup3.cml
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 |
|---|---|---|---|---|
| C1—H1⋯Br1 | 0.95 | 2.61 | 3.461 (3) | 149 |
| C3—H3A⋯Br1 | 0.99 | 2.91 | 3.795 (4) | 149 |
| C2—H2⋯Br1i | 0.95 | 2.75 | 3.657 (3) | 161 |
Symmetry code: (i)
.
Acknowledgments
This work was funded by the 211 Project of Guangdong Province.
supplementary crystallographic information
Comment
1H-1,2,4-Triazole, like imidazole and benzimidazole, can be N-alkylated to form N-heterocyclic carbine (Zanardi et al., 2011).
In an earlier report, we presented a N-heterocyclic benzimidazole derivative. The crystal structure consists of infinite chains connected via C—H···Br and C—H···O hydrogen bonds; it also shows π···π stacking interactions (Huang et al., 2010).
In this work, we report the structure of a triazole-based N-heterocyclic carbene, 1,4-bis[4-(methoxycarbonyl)benzyl]-1H-1,2,4-triazolium bromide (Fig. 1).
In the crystal structure, the dihedral angles between the triazole ring system and the two (C4–C9) and (C13–C18) benzene rings are 69.98 (18) ° and 72.17 (18) °, respectively; the dihedral angle between the two benzene rings is 8.69 (16) °.
The bromide anions and cations form infinite hydrogen bonding chains along the c-axis via C—H···Br hydrogen bonds between the bromide anions and carbineen atoms of triazole ring and ethylene linkage (Fig. 2, Table 1).
Experimental
4-(Methoxycarbonyl)benzyl bromide (2.28 g, 10.0 mmol) was slowly added to a solution of 1H-1,2,4-triazole (0.35 g, 5.0 mmol) in acetonitrile (25 ml) and the resulting mixture was stirred under reflux for 8 h.
The solvent was evaporated under reduced pressure. The solid residue was recrystallized in methanol, and colorless block crystals were obtained after few days, yield 1.42 g, 63.5%.
Elemental analysis, calcd (%) for C20H20N3BrO4: C 53.82, H 4.52, N 9.42; found(%): C 53.80, H 4.60, N 9.41.
The FAB mass spectrum showed tje ions at 447.
Refinement
The C-bound H atoms were positioned geometrically and were included in the refinement in the riding-model approximation, with distances 0.98 (CH3), 0.99 (CH2) and 0.95 Å (aromatic and triazole); Uiso(H) = xUeq(attached atom), where x = 1.5 for methyl C and 1.2 for all other C.
Figures
Fig. 1.
Perspective view showing 30% probability displacement ellipsoids and the atom-numbering scheme.
Fig. 2.
Crystal packing of the title compound. Dashed lines indicate hydrogen bonds. Symmetry: I = -x + 1, -y + 1, z + 1/2; II = -x + 1, -y + 2, z + 1/2. H atoms not involved in the hydrogen bond interactions have been omitted.
Crystal data
| C20H20N3O4+·Br− | Dx = 1.488 Mg m−3 |
| Mr = 446.30 | Cu Kα radiation, λ = 1.5418 Å |
| Orthorhombic, Pca21 | Cell parameters from 3691 reflections |
| a = 33.6880 (15) Å | θ = 3.6–66.9° |
| b = 4.7962 (3) Å | µ = 3.08 mm−1 |
| c = 12.3337 (6) Å | T = 173 K |
| V = 1992.81 (18) Å3 | Block, colorless |
| Z = 4 | 0.40 × 0.32 × 0.31 mm |
| F(000) = 912 |
Data collection
| Oxford Diffraction Xcalibur Atlas Gemini Ultra diffractometer | 2709 independent reflections |
| Radiation source: Enhance Ultra (Cu) X-ray Source | 2541 reflections with I > 2σ(I) |
| Mirror monochromator | Rint = 0.027 |
| Detector resolution: 10.5058 pixels mm-1 | θmax = 66.9°, θmin = 4.4° |
| φ and ω scans | h = −40→39 |
| Absorption correction: multi-scan (ABSPACK in CrysAlis PRO; Oxford Diffraction, 2006) | k = −5→4 |
| Tmin = 0.372, Tmax = 0.449 | l = −11→14 |
| 6375 measured reflections |
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)] = 0.027 | H-atom parameters constrained |
| wR(F2) = 0.069 | w = 1/[σ2(Fo2) + (0.0373P)2 + 0.0837P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max < 0.001 |
| 2709 reflections | Δρmax = 0.37 e Å−3 |
| 255 parameters | Δρmin = −0.24 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 840 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.021 (18) |
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 | ||
| C1 | 0.47864 (8) | 0.6564 (6) | 0.2417 (3) | 0.0375 (7) | |
| H1 | 0.4887 | 0.7596 | 0.1819 | 0.045* | |
| C2 | 0.47240 (9) | 0.3718 (7) | 0.3756 (3) | 0.0452 (7) | |
| H2 | 0.4788 | 0.2350 | 0.4285 | 0.054* | |
| C3 | 0.40894 (9) | 0.8422 (7) | 0.2458 (3) | 0.0480 (8) | |
| H3A | 0.4184 | 0.9793 | 0.1917 | 0.058* | |
| H3B | 0.3980 | 0.9465 | 0.3083 | 0.058* | |
| C4 | 0.37667 (8) | 0.6644 (6) | 0.1961 (3) | 0.0441 (7) | |
| C5 | 0.34867 (10) | 0.5364 (9) | 0.2611 (3) | 0.0554 (9) | |
| H5 | 0.3490 | 0.5665 | 0.3373 | 0.067* | |
| C6 | 0.32036 (11) | 0.3655 (9) | 0.2160 (3) | 0.0599 (10) | |
| H6 | 0.3017 | 0.2741 | 0.2616 | 0.072* | |
| C7 | 0.31867 (9) | 0.3249 (7) | 0.1051 (3) | 0.0450 (7) | |
| C8 | 0.34607 (8) | 0.4583 (7) | 0.0390 (4) | 0.0538 (7) | |
| H8 | 0.3449 | 0.4351 | −0.0374 | 0.065* | |
| C9 | 0.37509 (10) | 0.6255 (8) | 0.0851 (3) | 0.0533 (9) | |
| H9 | 0.3941 | 0.7143 | 0.0399 | 0.064* | |
| C10 | 0.28761 (9) | 0.1331 (7) | 0.0608 (4) | 0.0518 (10) | |
| C11 | 0.26013 (14) | −0.0757 (11) | −0.0946 (4) | 0.0807 (13) | |
| H11A | 0.2335 | −0.0263 | −0.0690 | 0.121* | |
| H11B | 0.2662 | −0.2681 | −0.0735 | 0.121* | |
| H11C | 0.2612 | −0.0592 | −0.1737 | 0.121* | |
| C12 | 0.53934 (10) | 0.3639 (7) | 0.2875 (3) | 0.0456 (8) | |
| H12A | 0.5389 | 0.2054 | 0.2361 | 0.055* | |
| H12B | 0.5492 | 0.2936 | 0.3580 | 0.055* | |
| C13 | 0.56784 (9) | 0.5850 (7) | 0.2453 (3) | 0.0389 (7) | |
| C14 | 0.59021 (9) | 0.7440 (7) | 0.3159 (3) | 0.0421 (7) | |
| H14 | 0.5868 | 0.7241 | 0.3919 | 0.051* | |
| C15 | 0.61770 (9) | 0.9330 (7) | 0.2758 (3) | 0.0454 (7) | |
| H15 | 0.6334 | 1.0398 | 0.3246 | 0.054* | |
| C16 | 0.62246 (8) | 0.9668 (7) | 0.1643 (3) | 0.0428 (7) | |
| C17 | 0.59997 (10) | 0.8069 (8) | 0.0951 (3) | 0.0521 (8) | |
| H17 | 0.6030 | 0.8288 | 0.0190 | 0.063* | |
| C18 | 0.57294 (9) | 0.6139 (8) | 0.1348 (3) | 0.0475 (7) | |
| H18 | 0.5580 | 0.5021 | 0.0861 | 0.057* | |
| C19 | 0.65221 (11) | 1.1610 (8) | 0.1181 (4) | 0.0541 (10) | |
| C20 | 0.70101 (11) | 1.5049 (8) | 0.1569 (5) | 0.0781 (14) | |
| H20A | 0.7055 | 1.6461 | 0.2130 | 0.117* | |
| H20B | 0.6921 | 1.5960 | 0.0901 | 0.117* | |
| H20C | 0.7258 | 1.4045 | 0.1429 | 0.117* | |
| N1 | 0.44256 (8) | 0.6675 (5) | 0.2823 (2) | 0.0398 (6) | |
| N2 | 0.43770 (8) | 0.4859 (7) | 0.3659 (2) | 0.0497 (8) | |
| N3 | 0.49824 (8) | 0.4702 (6) | 0.3018 (2) | 0.0345 (5) | |
| O1 | 0.26382 (8) | 0.0139 (6) | 0.1165 (3) | 0.0724 (8) | |
| O2 | 0.28892 (9) | 0.1106 (6) | −0.0466 (3) | 0.0679 (7) | |
| O3 | 0.65877 (9) | 1.1836 (7) | 0.0219 (3) | 0.0767 (10) | |
| O4 | 0.67098 (7) | 1.3101 (5) | 0.1933 (3) | 0.0648 (7) | |
| Br1 | 0.479859 (9) | 1.16298 (6) | 0.04187 (3) | 0.04923 (11) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0373 (15) | 0.0360 (17) | 0.0391 (17) | −0.0023 (11) | 0.0009 (12) | 0.0032 (13) |
| C2 | 0.0461 (17) | 0.051 (2) | 0.0381 (17) | −0.0054 (13) | −0.0026 (13) | 0.0080 (14) |
| C3 | 0.0408 (15) | 0.0435 (19) | 0.060 (2) | 0.0051 (13) | −0.0021 (15) | −0.0033 (15) |
| C4 | 0.0349 (14) | 0.0423 (18) | 0.0550 (19) | 0.0042 (11) | −0.0035 (14) | −0.0035 (15) |
| C5 | 0.0490 (18) | 0.073 (3) | 0.0444 (19) | −0.0087 (16) | 0.0028 (15) | −0.0006 (17) |
| C6 | 0.0504 (18) | 0.080 (3) | 0.050 (2) | −0.0217 (17) | 0.0059 (16) | 0.0001 (18) |
| C7 | 0.0335 (14) | 0.049 (2) | 0.0527 (19) | 0.0010 (12) | 0.0005 (13) | −0.0019 (15) |
| C8 | 0.0473 (15) | 0.070 (2) | 0.0442 (15) | −0.0054 (13) | 0.006 (2) | −0.003 (2) |
| C9 | 0.0431 (16) | 0.066 (2) | 0.0507 (18) | −0.0115 (15) | 0.0083 (14) | 0.0001 (16) |
| C10 | 0.0411 (14) | 0.0516 (18) | 0.063 (3) | 0.0008 (13) | −0.0052 (17) | −0.0019 (19) |
| C11 | 0.083 (3) | 0.087 (3) | 0.072 (3) | −0.020 (2) | −0.022 (3) | −0.009 (3) |
| C12 | 0.0394 (16) | 0.0411 (18) | 0.056 (2) | 0.0024 (13) | −0.0035 (16) | 0.0029 (15) |
| C13 | 0.0333 (14) | 0.0384 (17) | 0.0450 (18) | 0.0048 (12) | −0.0016 (13) | 0.0034 (15) |
| C14 | 0.0405 (15) | 0.0466 (17) | 0.0392 (16) | 0.0031 (12) | −0.0009 (13) | 0.0001 (14) |
| C15 | 0.0393 (15) | 0.0486 (19) | 0.0483 (18) | −0.0006 (12) | −0.0026 (13) | −0.0061 (15) |
| C16 | 0.0367 (14) | 0.0421 (18) | 0.0494 (17) | 0.0055 (12) | 0.0017 (13) | 0.0057 (14) |
| C17 | 0.0513 (18) | 0.066 (3) | 0.0386 (16) | −0.0032 (16) | −0.0007 (15) | 0.0064 (16) |
| C18 | 0.0474 (17) | 0.055 (2) | 0.0405 (17) | −0.0066 (13) | −0.0061 (14) | −0.0029 (15) |
| C19 | 0.0439 (17) | 0.051 (2) | 0.068 (3) | 0.0036 (14) | 0.0061 (18) | 0.0162 (19) |
| C20 | 0.0489 (19) | 0.049 (2) | 0.137 (4) | −0.0081 (16) | 0.016 (2) | 0.009 (2) |
| N1 | 0.0370 (12) | 0.0420 (16) | 0.0402 (14) | −0.0050 (10) | −0.0018 (12) | −0.0007 (11) |
| N2 | 0.0437 (14) | 0.064 (2) | 0.0408 (16) | −0.0075 (13) | 0.0009 (12) | 0.0105 (14) |
| N3 | 0.0365 (11) | 0.0365 (14) | 0.0304 (12) | −0.0044 (9) | 0.0003 (9) | 0.0020 (11) |
| O1 | 0.0623 (16) | 0.082 (2) | 0.0729 (19) | −0.0267 (15) | 0.0071 (14) | −0.0048 (16) |
| O2 | 0.0654 (16) | 0.0780 (19) | 0.0603 (16) | −0.0199 (14) | −0.0075 (14) | −0.0071 (15) |
| O3 | 0.0720 (17) | 0.087 (2) | 0.071 (3) | −0.0134 (14) | 0.0174 (17) | 0.0213 (16) |
| O4 | 0.0499 (13) | 0.0555 (16) | 0.089 (2) | −0.0115 (10) | 0.0067 (14) | 0.0025 (15) |
| Br1 | 0.06480 (19) | 0.04233 (17) | 0.04057 (16) | −0.00337 (13) | −0.0031 (2) | 0.0041 (2) |
Geometric parameters (Å, º)
| C1—N1 | 1.316 (4) | C11—H11B | 0.9800 |
| C1—N3 | 1.335 (4) | C11—H11C | 0.9800 |
| C1—H1 | 0.9500 | C12—N3 | 1.486 (5) |
| C2—N2 | 1.296 (4) | C12—C13 | 1.522 (5) |
| C2—N3 | 1.345 (4) | C12—H12A | 0.9900 |
| C2—H2 | 0.9500 | C12—H12B | 0.9900 |
| C3—N1 | 1.479 (4) | C13—C18 | 1.381 (5) |
| C3—C4 | 1.512 (4) | C13—C14 | 1.381 (5) |
| C3—H3A | 0.9900 | C14—C15 | 1.387 (5) |
| C3—H3B | 0.9900 | C14—H14 | 0.9500 |
| C4—C5 | 1.382 (5) | C15—C16 | 1.394 (5) |
| C4—C9 | 1.383 (5) | C15—H15 | 0.9500 |
| C5—C6 | 1.376 (5) | C16—C17 | 1.376 (5) |
| C5—H5 | 0.9500 | C16—C19 | 1.482 (5) |
| C6—C7 | 1.382 (5) | C17—C18 | 1.388 (5) |
| C6—H6 | 0.9500 | C17—H17 | 0.9500 |
| C7—C8 | 1.388 (5) | C18—H18 | 0.9500 |
| C7—C10 | 1.497 (5) | C19—O3 | 1.212 (6) |
| C8—C9 | 1.386 (5) | C19—O4 | 1.331 (5) |
| C8—H8 | 0.9500 | C20—O4 | 1.449 (4) |
| C9—H9 | 0.9500 | C20—H20A | 0.9800 |
| C10—O1 | 1.200 (5) | C20—H20B | 0.9800 |
| C10—O2 | 1.331 (6) | C20—H20C | 0.9800 |
| C11—O2 | 1.445 (5) | N1—N2 | 1.359 (4) |
| C11—H11A | 0.9800 | ||
| N1—C1—N3 | 105.8 (3) | C13—C12—H12A | 109.0 |
| N1—C1—H1 | 127.1 | N3—C12—H12B | 109.0 |
| N3—C1—H1 | 127.1 | C13—C12—H12B | 109.0 |
| N2—C2—N3 | 111.9 (3) | H12A—C12—H12B | 107.8 |
| N2—C2—H2 | 124.1 | C18—C13—C14 | 119.9 (3) |
| N3—C2—H2 | 124.1 | C18—C13—C12 | 119.1 (3) |
| N1—C3—C4 | 110.8 (3) | C14—C13—C12 | 120.9 (3) |
| N1—C3—H3A | 109.5 | C13—C14—C15 | 120.1 (3) |
| C4—C3—H3A | 109.5 | C13—C14—H14 | 120.0 |
| N1—C3—H3B | 109.5 | C15—C14—H14 | 120.0 |
| C4—C3—H3B | 109.5 | C14—C15—C16 | 120.3 (3) |
| H3A—C3—H3B | 108.1 | C14—C15—H15 | 119.9 |
| C5—C4—C9 | 119.3 (3) | C16—C15—H15 | 119.9 |
| C5—C4—C3 | 120.4 (3) | C17—C16—C15 | 119.0 (3) |
| C9—C4—C3 | 120.3 (3) | C17—C16—C19 | 118.9 (3) |
| C6—C5—C4 | 120.2 (3) | C15—C16—C19 | 122.0 (3) |
| C6—C5—H5 | 119.9 | C16—C17—C18 | 120.9 (3) |
| C4—C5—H5 | 119.9 | C16—C17—H17 | 119.5 |
| C5—C6—C7 | 120.9 (3) | C18—C17—H17 | 119.5 |
| C5—C6—H6 | 119.6 | C13—C18—C17 | 119.8 (3) |
| C7—C6—H6 | 119.6 | C13—C18—H18 | 120.1 |
| C6—C7—C8 | 119.3 (3) | C17—C18—H18 | 120.1 |
| C6—C7—C10 | 118.4 (3) | O3—C19—O4 | 123.2 (4) |
| C8—C7—C10 | 122.3 (3) | O3—C19—C16 | 123.8 (4) |
| C9—C8—C7 | 119.7 (4) | O4—C19—C16 | 113.0 (3) |
| C9—C8—H8 | 120.2 | O4—C20—H20A | 109.5 |
| C7—C8—H8 | 120.2 | O4—C20—H20B | 109.5 |
| C4—C9—C8 | 120.7 (3) | H20A—C20—H20B | 109.5 |
| C4—C9—H9 | 119.6 | O4—C20—H20C | 109.5 |
| C8—C9—H9 | 119.6 | H20A—C20—H20C | 109.5 |
| O1—C10—O2 | 123.6 (4) | H20B—C20—H20C | 109.5 |
| O1—C10—C7 | 123.4 (4) | C1—N1—N2 | 112.0 (3) |
| O2—C10—C7 | 113.0 (3) | C1—N1—C3 | 127.9 (3) |
| O2—C11—H11A | 109.5 | N2—N1—C3 | 120.1 (3) |
| O2—C11—H11B | 109.5 | C2—N2—N1 | 103.4 (3) |
| H11A—C11—H11B | 109.5 | C1—N3—C2 | 106.9 (3) |
| O2—C11—H11C | 109.5 | C1—N3—C12 | 128.6 (3) |
| H11A—C11—H11C | 109.5 | C2—N3—C12 | 124.2 (3) |
| H11B—C11—H11C | 109.5 | C10—O2—C11 | 115.8 (4) |
| N3—C12—C13 | 112.9 (3) | C19—O4—C20 | 117.5 (4) |
| N3—C12—H12A | 109.0 | ||
| N1—C3—C4—C5 | 84.0 (4) | C14—C13—C18—C17 | −1.3 (5) |
| N1—C3—C4—C9 | −95.3 (4) | C12—C13—C18—C17 | −177.5 (3) |
| C9—C4—C5—C6 | 2.0 (6) | C16—C17—C18—C13 | 1.3 (5) |
| C3—C4—C5—C6 | −177.3 (3) | C17—C16—C19—O3 | −1.9 (6) |
| C4—C5—C6—C7 | −1.8 (6) | C15—C16—C19—O3 | 175.5 (4) |
| C5—C6—C7—C8 | 0.2 (6) | C17—C16—C19—O4 | 177.8 (3) |
| C5—C6—C7—C10 | 179.1 (3) | C15—C16—C19—O4 | −4.9 (5) |
| C6—C7—C8—C9 | 1.2 (5) | N3—C1—N1—N2 | −1.9 (4) |
| C10—C7—C8—C9 | −177.6 (3) | N3—C1—N1—C3 | 179.8 (3) |
| C5—C4—C9—C8 | −0.6 (6) | C4—C3—N1—C1 | 111.4 (4) |
| C3—C4—C9—C8 | 178.7 (3) | C4—C3—N1—N2 | −66.8 (4) |
| C7—C8—C9—C4 | −1.0 (5) | N3—C2—N2—N1 | −0.8 (4) |
| C6—C7—C10—O1 | 0.6 (5) | C1—N1—N2—C2 | 1.7 (4) |
| C8—C7—C10—O1 | 179.4 (3) | C3—N1—N2—C2 | −179.8 (3) |
| C6—C7—C10—O2 | −180.0 (4) | N1—C1—N3—C2 | 1.3 (4) |
| C8—C7—C10—O2 | −1.1 (5) | N1—C1—N3—C12 | 175.9 (3) |
| N3—C12—C13—C18 | −90.6 (4) | N2—C2—N3—C1 | −0.3 (4) |
| N3—C12—C13—C14 | 93.2 (4) | N2—C2—N3—C12 | −175.2 (3) |
| C18—C13—C14—C15 | 0.1 (5) | C13—C12—N3—C1 | 35.4 (5) |
| C12—C13—C14—C15 | 176.2 (3) | C13—C12—N3—C2 | −150.9 (3) |
| C13—C14—C15—C16 | 1.1 (5) | O1—C10—O2—C11 | −1.6 (6) |
| C14—C15—C16—C17 | −1.1 (5) | C7—C10—O2—C11 | 178.9 (3) |
| C14—C15—C16—C19 | −178.4 (3) | O3—C19—O4—C20 | −0.9 (5) |
| C15—C16—C17—C18 | −0.1 (5) | C16—C19—O4—C20 | 179.4 (3) |
| C19—C16—C17—C18 | 177.3 (3) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C1—H1···Br1 | 0.95 | 2.61 | 3.461 (3) | 149 |
| C3—H3A···Br1 | 0.99 | 2.91 | 3.795 (4) | 149 |
| C2—H2···Br1i | 0.95 | 2.75 | 3.657 (3) | 161 |
Symmetry code: (i) −x+1, −y+1, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5263).
References
- Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
- Flack, H. D. (1983). Acta Cryst. A39, 876–881.
- Huang, H.-R., Wen-Jiao, G., Du, Z.-Y., Fang, Y.-X. & Zhang, K. (2010). Acta Cryst. E66, o3064. [DOI] [PMC free article] [PubMed]
- Oxford Diffraction (2006). CrysAlis PRO. Oxford Diffraction Ltd., Abingdon, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
- Zanardi, A., Mata, J. A. & Peris, E. (2011). Eur. J. Inorg. Chem. pp. 416–421.
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/S1600536812016728/ng5263sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016728/ng5263Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812016728/ng5263Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


