Abstract
In the title salt, C15H16NO4 +.Br3 −, classical intramolecular O—H⋯O hydrogen bonds are found, which results in the co-planarity of the ester substituents with the quinolinium residue [C—C—C—O torsion angle = 1.0 (10)°]. The bromine anions are placed on both sides of heterocyclic cation and form Br⋯N contacts of 3.674 (9) and 3.860 (9) Å, which confirms the location of positive charge on the N atom. Non-classical intermolecular C—H⋯Br interactions stabilize the three-dimensional crystal structure. Moreover, anion⋯π interactions are noted [Br⋯ring centroid range = 3.367 (9)–3.697 (9) Å]. The partly saturated heterocycle is disordered over two sofa conformations with occupancies in the ratio 0.56 (2):0.44 (2).
Related literature
For general background, see: Ukrainets et al. (2004 ▶, 2007 ▶). For chemical bond lengths, see: Bürgi & Dunitz (1994 ▶).
Experimental
Crystal data
C15H16NO4 +·Br3 −
M r = 513.99
Triclinic,
a = 7.6491 (8) Å
b = 9.1729 (10) Å
c = 13.3722 (14) Å
α = 102.355 (9)°
β = 98.777 (9)°
γ = 98.093 (9)°
V = 891.06 (17) Å3
Z = 2
Mo Kα radiation
μ = 6.81 mm−1
T = 295 K
0.20 × 0.05 × 0.05 mm
Data collection
Agilent Xcalibur-3 CCD diffractometer
Absorption correction: multi-scan (CrysAlis RED; Agilent, 2011 ▶) T min = 0.343, T max = 0.727
10147 measured reflections
5106 independent reflections
1855 reflections with I > 2σ(I)
R int = 0.034
Refinement
R[F 2 > 2σ(F 2)] = 0.068
wR(F 2) = 0.217
S = 0.90
5106 reflections
224 parameters
5 restraints
H-atom parameters constrained
Δρmax = 1.02 e Å−3
Δρmin = −0.74 e Å−3
Data collection: CrysAlis CCD (Agilent, 2011 ▶); cell refinement: CrysAlis RED (Agilent, 2011 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812049276/aa2080sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812049276/aa2080Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812049276/aa2080Isup3.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 |
|---|---|---|---|---|
| O2—H2⋯O4 | 0.82 | 1.93 | 2.631 (7) | 142 |
| O1—H1⋯O3 | 0.82 | 1.73 | 2.459 (10) | 147 |
| C3—H3⋯Br1i | 0.93 | 2.90 | 3.810 (9) | 168 |
| C4—H4⋯Br2ii | 0.93 | 3.06 | 3.846 (9) | 143 |
| C10—H10B⋯Br2 | 0.97 | 2.99 | 3.936 (8) | 166 |
| C10—H10C⋯Br4iii | 0.97 | 2.92 | 3.752 (8) | 144 |
| C11A—H11B⋯Br4iii | 0.97 | 3.02 | 3.797 (17) | 138 |
Symmetry codes: (i)
; (ii)
; (iii)
.
supplementary crystallographic information
Comment
Bromination of alkyl 1-R-4-hydroxy-2-oxo-1,2-dihydroquinoline-3-carboxylates (R = H, alkyl, phenyl) by molecular bromine in the environment of acetic acid can pass on two directions (Ukrainets et al., 2004, 2007). However, the reaction of ethyl 7-hydroxy-5-oxo-2,3-dihydro-1H,5H-pyrido[3,2,1-ij]quinoline-6-carboxylate with bromine results in the 6-ethyloxycarbonyl-5,7-dihydroxy-2,3-dihydro-1H-pyrido[3,2,1-ij]quinolinium tribromide, I.
Two tribromide anions are located in special positions, the coordinates of the central atoms coincide with the center of symmetry so the asymmetric part of unit cell contains one cation and two halves of anions. The positive charge of the cation is located on the N atom which is bonded with three atoms and the N1═C9 bond (1.335 (6) Å) has double character (the mean value for Csp2═N bond is 1.329 (1) Å (Bürgi & Dunitz, 1994)).
The partly saturated heterocycle is disordered over two sofa conformations (A and B) with population in the ratio 0.56 (2)/0.44 (2). The deviations of the C11 atom from main plane C1/C2/N1/C10/C12 are -0.57 (1) and 0.59 (1) Å for conformers A and B, respectively. The ester substituent is coplanar to the planar fragment of tricycle (C9—C8—C13—O3 torsion angle is 1.0 (10)°) owing to the formation of the strong intramolecular hydrogen bonds O1—H1···O3 and O2—H2···O4 (Table 1). The formation of hydrogen bonds causes the elongation of the C13═O3 (1.243 (10) Å) and C7═C8 (1.376 (9) Å) bonds (the mean values are 1.210 (1) Å and 1.326 (1) Å, respectively) and the shortening of the C9—O1 (1.307 (8) Å), C7—O2 (1.299 (8) Å) bonds (the mean value is 1.333 (1) Å). The methylene atom from ethyl group of the substituent has ap-orientation relative to the C8—C13 bond and is turned relative to the C13—O4 bond (the C14—O4—C13—C8 and C13—O4—C14—C15 torsion angles are 175.7 (6)° and -155.4 (8)°, respectively).
Experimental
A solution of anhydrous bromine (0.52 ml, 0.01 mol) in anhydrous acetic acid (5 ml) was added with vigorous stirring to a solution of the ethyl 7-hydroxy-5-oxo-2,3-dihydro-1H,5H-pyrido[3,2,1-ij]quinoline-6-carboxylate (2.73 g, 0.01 mol) in anhydrous acetic acid (20 ml). A light-yellow precipitate was formed immediately. The crystals of I were filtered off, washed with acetic acid and dried to give the product (2.26 g, 44%); m.p. 360–362 K.
Refinement
The restrictions on the bond length of the ethyl group of the ester substituent and bond lengths in disordered fragment (1.54 Å) were applied. All H atoms were located from electron-density difference maps and were refined in the riding-motion approximation with Uiso(H) constrained to be 1.5 times Ueq of the carrier atom for the methyl and hydroxyl groups and 1.2 times Ueq of the carrier atom for the other atoms.
Figures
Fig. 1.
View of the title compound with the atom numbering scheme. The displacement ellipsoids are drawn at the 15% probability level. H atoms are presented as a small spheres of arbitrary radius. Intramolecular hydrogen bonds are indicated by dashed lines. Only major moiety of disorder group [s.o.f. = 0.56 (2)] are presented. Symmetry codes: (i) -x + 1, -y + 1, -z + 1; (ii) -x, -y, -z.
Crystal data
| C15H16NO4+·Br3− | Z = 2 |
| Mr = 513.99 | F(000) = 500 |
| Triclinic, P1 | Dx = 1.916 Mg m−3 |
| Hall symbol: -P 1 | Melting point = 360–362 K |
| a = 7.6491 (8) Å | Mo Kα radiation, λ = 0.71073 Å |
| b = 9.1729 (10) Å | Cell parameters from 1363 reflections |
| c = 13.3722 (14) Å | θ = 3.1–32.0° |
| α = 102.355 (9)° | µ = 6.81 mm−1 |
| β = 98.777 (9)° | T = 295 K |
| γ = 98.093 (9)° | Rod, light yellow |
| V = 891.06 (17) Å3 | 0.20 × 0.05 × 0.05 mm |
Data collection
| Agilent Xcalibur-3 CCD diffractometer | 5106 independent reflections |
| Radiation source: Enhance (Mo) X-Ray Source | 1855 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.034 |
| Detector resolution: 16.1827 pixels mm-1 | θmax = 30.0°, θmin = 3.1° |
| ω scans | h = −10→10 |
| Absorption correction: multi-scan (CrysAlis RED; Agilent, 2011) | k = −12→12 |
| Tmin = 0.343, Tmax = 0.727 | l = −18→18 |
| 10147 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)] = 0.068 | Hydrogen site location: difference Fourier map |
| wR(F2) = 0.217 | H-atom parameters constrained |
| S = 0.90 | w = 1/[σ2(Fo2) + (0.108P)2] where P = (Fo2 + 2Fc2)/3 |
| 5106 reflections | (Δ/σ)max < 0.001 |
| 224 parameters | Δρmax = 1.02 e Å−3 |
| 5 restraints | Δρmin = −0.74 e Å−3 |
Special details
| Experimental. Absorption correction: CrysAlis RED (Agilent Technologies, 2011). Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. |
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'s involving l.s. planes. |
| Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wRand 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 > 2σ(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 | Occ. (<1) | |
| Br1 | 0.5000 | 0.5000 | 0.5000 | 0.0803 (3) | |
| Br2 | 0.56781 (11) | 0.74499 (9) | 0.44305 (6) | 0.1062 (4) | |
| Br3 | 0.0000 | 0.0000 | 0.0000 | 0.1391 (6) | |
| Br4 | 0.06301 (17) | −0.24813 (17) | 0.03287 (9) | 0.1666 (6) | |
| N1 | 0.1821 (7) | 0.3314 (6) | 0.2533 (4) | 0.0753 (14) | |
| O1 | 0.4153 (7) | 0.3418 (7) | 0.1698 (5) | 0.1109 (17) | |
| H1 | 0.4995 | 0.2986 | 0.1580 | 0.166* | |
| O2 | 0.2437 (8) | −0.0849 (6) | 0.3048 (4) | 0.0989 (14) | |
| H2 | 0.3201 | −0.1217 | 0.2760 | 0.148* | |
| O3 | 0.5774 (8) | 0.1288 (8) | 0.1341 (4) | 0.131 (2) | |
| O4 | 0.5025 (7) | −0.0768 (7) | 0.1961 (4) | 0.1052 (16) | |
| C1 | 0.0665 (9) | 0.2577 (8) | 0.3053 (4) | 0.0726 (17) | |
| C2 | −0.0723 (9) | 0.3279 (8) | 0.3413 (6) | 0.0848 (19) | |
| C3 | −0.1792 (11) | 0.2510 (11) | 0.3935 (6) | 0.108 (2) | |
| H3 | −0.2679 | 0.2972 | 0.4209 | 0.129* | |
| C4 | −0.1624 (11) | 0.1110 (10) | 0.4074 (6) | 0.095 (2) | |
| H4 | −0.2438 | 0.0610 | 0.4394 | 0.114* | |
| C5 | −0.0296 (10) | 0.0449 (8) | 0.3754 (5) | 0.0853 (19) | |
| H5 | −0.0136 | −0.0483 | 0.3888 | 0.102* | |
| C6 | 0.0867 (9) | 0.1169 (8) | 0.3211 (4) | 0.0747 (17) | |
| C7 | 0.2325 (9) | 0.0461 (8) | 0.2845 (5) | 0.0774 (17) | |
| C8 | 0.3425 (9) | 0.1203 (8) | 0.2317 (5) | 0.0772 (17) | |
| C9 | 0.3130 (10) | 0.2649 (9) | 0.2176 (5) | 0.085 (2) | |
| C10 | 0.1679 (10) | 0.4818 (9) | 0.2325 (7) | 0.110 (3) | |
| H10A | 0.1998 | 0.4849 | 0.1654 | 0.132* | 0.56 (2) |
| H10B | 0.2520 | 0.5597 | 0.2855 | 0.132* | 0.56 (2) |
| H10C | 0.1017 | 0.4691 | 0.1624 | 0.132* | 0.44 (2) |
| H10D | 0.2871 | 0.5389 | 0.2378 | 0.132* | 0.44 (2) |
| C11A | −0.0241 (14) | 0.515 (2) | 0.2325 (11) | 0.113 (7) | 0.56 (2) |
| H11A | −0.0223 | 0.6214 | 0.2353 | 0.136* | 0.56 (2) |
| H11B | −0.1011 | 0.4569 | 0.1675 | 0.136* | 0.56 (2) |
| C11B | 0.0704 (18) | 0.5691 (14) | 0.3120 (14) | 0.117 (9) | 0.44 (2) |
| H11C | 0.1506 | 0.6019 | 0.3793 | 0.141* | 0.44 (2) |
| H11D | 0.0431 | 0.6591 | 0.2904 | 0.141* | 0.44 (2) |
| C12 | −0.1052 (12) | 0.4752 (10) | 0.3240 (7) | 0.126 (3) | |
| H12A | −0.0535 | 0.5536 | 0.3869 | 0.151* | 0.56 (2) |
| H12B | −0.2338 | 0.4734 | 0.3099 | 0.151* | 0.56 (2) |
| H12C | −0.1499 | 0.5296 | 0.3825 | 0.151* | 0.44 (2) |
| H12D | −0.1956 | 0.4597 | 0.2615 | 0.151* | 0.44 (2) |
| C13 | 0.4866 (11) | 0.0567 (11) | 0.1831 (5) | 0.092 (2) | |
| C14 | 0.6366 (11) | −0.1428 (11) | 0.1409 (8) | 0.140 (4) | |
| H14A | 0.7564 | −0.1079 | 0.1829 | 0.167* | |
| H14B | 0.6352 | −0.1137 | 0.0752 | 0.167* | |
| C15 | 0.5833 (15) | −0.3161 (11) | 0.1218 (10) | 0.173 (5) | |
| H15A | 0.6558 | −0.3649 | 0.0772 | 0.260* | |
| H15B | 0.4588 | −0.3470 | 0.0893 | 0.260* | |
| H15C | 0.6020 | −0.3444 | 0.1872 | 0.260* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1 | 0.0730 (5) | 0.0913 (7) | 0.0716 (5) | 0.0189 (5) | 0.0020 (4) | 0.0143 (5) |
| Br2 | 0.1086 (6) | 0.0994 (7) | 0.1052 (6) | 0.0040 (5) | 0.0010 (4) | 0.0359 (5) |
| Br3 | 0.0870 (7) | 0.2340 (17) | 0.0652 (6) | −0.0272 (9) | −0.0029 (5) | 0.0175 (7) |
| Br4 | 0.1423 (10) | 0.2122 (13) | 0.1221 (8) | −0.0008 (9) | 0.0014 (6) | 0.0283 (8) |
| N1 | 0.071 (3) | 0.071 (4) | 0.077 (3) | −0.003 (3) | 0.004 (3) | 0.019 (3) |
| O1 | 0.098 (4) | 0.133 (5) | 0.108 (4) | −0.009 (3) | 0.022 (3) | 0.061 (4) |
| O2 | 0.112 (4) | 0.082 (3) | 0.116 (4) | 0.034 (3) | 0.040 (3) | 0.028 (3) |
| O3 | 0.107 (4) | 0.179 (6) | 0.104 (4) | −0.004 (4) | 0.050 (3) | 0.027 (4) |
| O4 | 0.083 (3) | 0.110 (4) | 0.114 (4) | 0.011 (3) | 0.031 (3) | 0.002 (3) |
| C1 | 0.076 (4) | 0.076 (4) | 0.055 (3) | −0.003 (3) | −0.006 (3) | 0.017 (3) |
| C2 | 0.084 (4) | 0.082 (5) | 0.099 (5) | 0.026 (4) | 0.020 (4) | 0.034 (4) |
| C3 | 0.095 (5) | 0.125 (7) | 0.103 (5) | 0.021 (5) | 0.035 (4) | 0.016 (5) |
| C4 | 0.096 (5) | 0.104 (6) | 0.095 (5) | 0.029 (5) | 0.040 (4) | 0.024 (4) |
| C5 | 0.097 (5) | 0.083 (5) | 0.081 (4) | 0.009 (4) | 0.023 (4) | 0.030 (4) |
| C6 | 0.086 (4) | 0.080 (5) | 0.052 (3) | 0.007 (4) | −0.002 (3) | 0.019 (3) |
| C7 | 0.080 (4) | 0.076 (5) | 0.069 (4) | 0.007 (4) | 0.008 (3) | 0.012 (3) |
| C8 | 0.076 (4) | 0.084 (5) | 0.062 (3) | 0.002 (4) | 0.006 (3) | 0.010 (3) |
| C9 | 0.085 (5) | 0.096 (6) | 0.059 (3) | −0.017 (4) | −0.002 (3) | 0.019 (4) |
| C10 | 0.113 (6) | 0.086 (6) | 0.113 (6) | −0.014 (5) | −0.012 (5) | 0.027 (5) |
| C11A | 0.115 (13) | 0.103 (12) | 0.127 (14) | 0.022 (10) | 0.004 (10) | 0.052 (11) |
| C11B | 0.111 (16) | 0.081 (14) | 0.17 (2) | 0.015 (11) | 0.018 (16) | 0.060 (14) |
| C12 | 0.141 (8) | 0.099 (6) | 0.146 (8) | 0.029 (6) | 0.034 (6) | 0.038 (6) |
| C13 | 0.092 (5) | 0.102 (6) | 0.072 (4) | 0.014 (5) | 0.008 (4) | 0.009 (4) |
| C14 | 0.097 (6) | 0.154 (10) | 0.151 (8) | 0.033 (6) | 0.043 (6) | −0.019 (7) |
| C15 | 0.176 (11) | 0.169 (12) | 0.232 (13) | 0.074 (10) | 0.106 (10) | 0.096 (11) |
Geometric parameters (Å, º)
| Br1—Br2i | 2.5346 (8) | C7—C8 | 1.376 (9) |
| Br1—Br2 | 2.5346 (8) | C8—C9 | 1.423 (10) |
| Br3—Br4ii | 2.5057 (16) | C8—C13 | 1.489 (11) |
| Br3—Br4 | 2.5057 (16) | C10—C11A | 1.5398 (10) |
| N1—C9 | 1.340 (9) | C10—C11B | 1.5398 (10) |
| N1—C1 | 1.394 (8) | C10—H10A | 0.9700 |
| N1—C10 | 1.479 (9) | C10—H10B | 0.9700 |
| O1—C9 | 1.307 (8) | C10—H10C | 0.9700 |
| O1—H1 | 0.8200 | C10—H10D | 0.9700 |
| O2—C7 | 1.299 (8) | C11A—C12 | 1.5396 (10) |
| O2—H2 | 0.8200 | C11A—H11A | 0.9700 |
| O3—C13 | 1.243 (10) | C11A—H11B | 0.9700 |
| O4—C13 | 1.292 (9) | C11B—C12 | 1.5397 (10) |
| O4—C14 | 1.476 (9) | C11B—H11C | 0.9700 |
| C1—C6 | 1.378 (9) | C11B—H11D | 0.9700 |
| C1—C2 | 1.411 (10) | C12—H12A | 0.9700 |
| C2—C3 | 1.370 (10) | C12—H12B | 0.9700 |
| C2—C12 | 1.467 (11) | C12—H12C | 0.9700 |
| C3—C4 | 1.358 (10) | C12—H12D | 0.9700 |
| C3—H3 | 0.9300 | C14—C15 | 1.5395 (10) |
| C4—C5 | 1.334 (10) | C14—H14A | 0.9700 |
| C4—H4 | 0.9300 | C14—H14B | 0.9700 |
| C5—C6 | 1.411 (9) | C15—H15A | 0.9600 |
| C5—H5 | 0.9300 | C15—H15B | 0.9600 |
| C6—C7 | 1.462 (10) | C15—H15C | 0.9600 |
| Br2i—Br1—Br2 | 180.0 | C11B—C10—H10D | 109.7 |
| Br4ii—Br3—Br4 | 180.00 (8) | H10A—C10—H10D | 66.6 |
| C9—N1—C1 | 120.0 (6) | H10C—C10—H10D | 108.2 |
| C9—N1—C10 | 116.4 (6) | C12—C11A—C10 | 113.6 (7) |
| C1—N1—C10 | 123.6 (6) | C12—C11A—H11A | 108.9 |
| C9—O1—H1 | 109.5 | C10—C11A—H11A | 108.9 |
| C7—O2—H2 | 109.5 | C12—C11A—H11B | 108.9 |
| C13—O4—C14 | 112.8 (7) | C10—C11A—H11B | 108.9 |
| C6—C1—N1 | 120.4 (6) | H11A—C11A—H11B | 107.7 |
| C6—C1—C2 | 120.1 (6) | C12—C11B—C10 | 113.6 (7) |
| N1—C1—C2 | 119.5 (6) | C12—C11B—H11C | 108.9 |
| C3—C2—C1 | 116.7 (7) | C10—C11B—H11C | 108.9 |
| C3—C2—C12 | 120.4 (8) | C12—C11B—H11D | 108.9 |
| C1—C2—C12 | 122.9 (6) | C10—C11B—H11D | 108.9 |
| C4—C3—C2 | 123.5 (8) | H11C—C11B—H11D | 107.7 |
| C4—C3—H3 | 118.3 | C2—C12—C11A | 112.3 (9) |
| C2—C3—H3 | 118.3 | C2—C12—C11B | 109.9 (10) |
| C5—C4—C3 | 120.2 (7) | C2—C12—H12A | 109.1 |
| C5—C4—H4 | 119.9 | C11A—C12—H12A | 109.1 |
| C3—C4—H4 | 119.9 | C11B—C12—H12A | 68.9 |
| C4—C5—C6 | 119.7 (7) | C2—C12—H12B | 109.1 |
| C4—C5—H5 | 120.1 | C11A—C12—H12B | 109.1 |
| C6—C5—H5 | 120.1 | C11B—C12—H12B | 139.4 |
| C1—C6—C5 | 119.7 (7) | H12A—C12—H12B | 107.9 |
| C1—C6—C7 | 119.5 (6) | C2—C12—H12C | 109.7 |
| C5—C6—C7 | 120.7 (7) | C11A—C12—H12C | 136.4 |
| O2—C7—C8 | 126.0 (7) | C11B—C12—H12C | 109.7 |
| O2—C7—C6 | 115.3 (6) | H12B—C12—H12C | 66.2 |
| C8—C7—C6 | 118.7 (7) | C2—C12—H12D | 109.7 |
| C7—C8—C9 | 118.7 (7) | C11A—C12—H12D | 67.7 |
| C7—C8—C13 | 124.5 (7) | C11B—C12—H12D | 109.7 |
| C9—C8—C13 | 116.7 (7) | H12A—C12—H12D | 138.7 |
| O1—C9—N1 | 116.0 (7) | H12B—C12—H12D | 45.0 |
| O1—C9—C8 | 121.3 (8) | H12C—C12—H12D | 108.2 |
| N1—C9—C8 | 122.6 (6) | O3—C13—O4 | 125.5 (8) |
| N1—C10—C11A | 111.1 (8) | O3—C13—C8 | 120.9 (9) |
| N1—C10—C11B | 109.7 (9) | O4—C13—C8 | 113.6 (7) |
| N1—C10—H10A | 109.4 | O4—C14—C15 | 106.3 (8) |
| C11A—C10—H10A | 109.4 | O4—C14—H14A | 110.5 |
| C11B—C10—H10A | 139.2 | C15—C14—H14A | 110.5 |
| N1—C10—H10B | 109.4 | O4—C14—H14B | 110.5 |
| C11A—C10—H10B | 109.4 | C15—C14—H14B | 110.5 |
| C11B—C10—H10B | 68.8 | H14A—C14—H14B | 108.7 |
| H10A—C10—H10B | 108.0 | C14—C15—H15A | 109.5 |
| N1—C10—H10C | 109.7 | C14—C15—H15B | 109.5 |
| C11A—C10—H10C | 68.1 | H15A—C15—H15B | 109.5 |
| C11B—C10—H10C | 109.7 | C14—C15—H15C | 109.5 |
| H10B—C10—H10C | 138.4 | H15A—C15—H15C | 109.5 |
| N1—C10—H10D | 109.7 | H15B—C15—H15C | 109.5 |
| C11A—C10—H10D | 137.5 | ||
| C9—N1—C1—C6 | 0.6 (8) | C10—N1—C9—C8 | −179.9 (6) |
| C10—N1—C1—C6 | 179.4 (5) | C7—C8—C9—O1 | 178.7 (6) |
| C9—N1—C1—C2 | −179.1 (6) | C13—C8—C9—O1 | −4.2 (9) |
| C10—N1—C1—C2 | −0.3 (9) | C7—C8—C9—N1 | −0.2 (9) |
| C6—C1—C2—C3 | 1.5 (9) | C13—C8—C9—N1 | 176.9 (6) |
| N1—C1—C2—C3 | −178.8 (6) | C9—N1—C10—C11A | 155.4 (8) |
| C6—C1—C2—C12 | −177.9 (7) | C1—N1—C10—C11A | −23.5 (10) |
| N1—C1—C2—C12 | 1.8 (10) | C9—N1—C10—C11B | −157.4 (8) |
| C1—C2—C3—C4 | −3.0 (12) | C1—N1—C10—C11B | 23.7 (10) |
| C12—C2—C3—C4 | 176.4 (7) | N1—C10—C11A—C12 | 45.2 (15) |
| C2—C3—C4—C5 | 4.4 (13) | C11B—C10—C11A—C12 | −51.8 (8) |
| C3—C4—C5—C6 | −4.0 (11) | N1—C10—C11B—C12 | −48.6 (16) |
| N1—C1—C6—C5 | 178.9 (5) | C11A—C10—C11B—C12 | 51.8 (8) |
| C2—C1—C6—C5 | −1.4 (9) | C3—C2—C12—C11A | −158.5 (10) |
| N1—C1—C6—C7 | 1.0 (8) | C1—C2—C12—C11A | 20.9 (12) |
| C2—C1—C6—C7 | −179.3 (6) | C3—C2—C12—C11B | 154.1 (9) |
| C4—C5—C6—C1 | 2.6 (10) | C1—C2—C12—C11B | −26.5 (11) |
| C4—C5—C6—C7 | −179.5 (7) | C10—C11A—C12—C2 | −44.3 (16) |
| C1—C6—C7—O2 | 178.5 (5) | C10—C11A—C12—C11B | 51.8 (8) |
| C5—C6—C7—O2 | 0.6 (9) | C10—C11B—C12—C2 | 50.2 (17) |
| C1—C6—C7—C8 | −2.2 (8) | C10—C11B—C12—C11A | −51.8 (8) |
| C5—C6—C7—C8 | 179.9 (6) | C14—O4—C13—O3 | −3.2 (11) |
| O2—C7—C8—C9 | −179.0 (6) | C14—O4—C13—C8 | 175.7 (6) |
| C6—C7—C8—C9 | 1.8 (9) | C7—C8—C13—O3 | 178.0 (7) |
| O2—C7—C8—C13 | 4.1 (11) | C9—C8—C13—O3 | 1.0 (10) |
| C6—C7—C8—C13 | −175.1 (6) | C7—C8—C13—O4 | −1.0 (10) |
| C1—N1—C9—O1 | 180.0 (5) | C9—C8—C13—O4 | −177.9 (6) |
| C10—N1—C9—O1 | 1.1 (8) | C13—O4—C14—C15 | −155.4 (8) |
| C1—N1—C9—C8 | −1.0 (8) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x, −y, −z.
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O2—H2···O4 | 0.82 | 1.93 | 2.631 (7) | 142 |
| O1—H1···O3 | 0.82 | 1.73 | 2.459 (10) | 147 |
| C3—H3···Br1iii | 0.93 | 2.90 | 3.810 (9) | 168 |
| C4—H4···Br2iv | 0.93 | 3.06 | 3.846 (9) | 143 |
| C10—H10B···Br2 | 0.97 | 2.99 | 3.936 (8) | 166 |
| C10—H10C···Br4ii | 0.97 | 2.92 | 3.752 (8) | 144 |
| C11A—H11B···Br4ii | 0.97 | 3.02 | 3.797 (17) | 138 |
Symmetry codes: (ii) −x, −y, −z; (iii) x−1, y, z; (iv) x−1, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: AA2080).
References
- Agilent (2011). CrysAlis PRO and CrysAlis RED Agilent Technologies, Yarnton, Oxfordshire, England.
- Bürgi, H.-B. & Dunitz, J. D. (1994). Structure Correlation, Vol. 2, pp. 767–784. Weinheim: VCH.
- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Ukrainets, I. V., Petrushova, L. A., Sidorenko, L. V., Rybakov, V. B. & Chernyshev, V. V. (2004). Zh. Org. Farm. Khim. 2, 26–31.
- Ukrainets, I. V., Sidorenko, L. V. & Golovchenko, O. S. (2007). Chem. Heterocycl. Compd, pp. 1008–1013.
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) I, global. DOI: 10.1107/S1600536812049276/aa2080sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812049276/aa2080Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812049276/aa2080Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

