Abstract
In the title compound, C18H19N3O5, the 3,6-dihydro-2H-pyran ring adopts a half-chair, distorted towards a half-boat, conformation with Q T = 0.5276(14) Å. The benzene ring is twisted out of the place of the triazole ring [dihedral angle = 23.54 (8)°]. In the crystal, supramolecular layers in the ac plane are formed through C—H⋯O and C—H⋯π(triazole) interactions. These stack along the b axis being connected by C—H⋯N contacts.
Related literature
For background to the chemical attributes of C-glycosides, see: Ritchie et al. (2002 ▶); Hanessian & Lou (2000 ▶); Hultin (2005 ▶); Zou (2005 ▶). For chiral properties of C-glycosides, see: Nakata (2005 ▶); Nicolaou et al. (2008 ▶); Somsak (2001 ▶). For additional conformation analysis, see: Cremer & Pople (1975 ▶).
Experimental
Crystal data
C18H19N3O5
M r = 357.36
Monoclinic,
a = 4.79932 (7) Å
b = 16.6308 (2) Å
c = 10.76331 (14) Å
β = 93.225 (1)°
V = 857.73 (2) Å3
Z = 2
Cu Kα radiation
μ = 0.86 mm−1
T = 100 K
0.20 × 0.10 × 0.05 mm
Data collection
Agilent SuperNova Dual Cu at zero diffractometer with an Atlas detector
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010 ▶) T min = 0.848, T max = 0.959
5784 measured reflections
3369 independent reflections
3304 reflections with I > 2σ(I)
R int = 0.019
Refinement
R[F 2 > 2σ(F 2)] = 0.033
wR(F 2) = 0.084
S = 1.04
3369 reflections
237 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.14 e Å−3
Δρmin = −0.19 e Å−3
Absolute structure: Flack (1983 ▶), 1591 Friedel pairs
Flack parameter: −0.09 (15)
Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SIR92 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶), DIAMOND (Brandenburg, 2006 ▶) and MarvinSketch (ChemAxon, 2009 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811037305/hg5093sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811037305/hg5093Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811037305/hg5093Isup3.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 |
|---|---|---|---|---|
| C7—H7⋯O4i | 0.95 | 2.29 | 3.2207 (19) | 167 |
| C9—H9⋯Cg1ii | 1.00 | 2.68 | 3.5362 (16) | 144 |
| C16—H16a⋯N3iii | 0.98 | 2.62 | 3.463 (2) | 145 |
| C16—H16b⋯O2ii | 0.98 | 2.59 | 3.570 (2) | 177 |
| C18—H18a⋯O1iv | 0.98 | 2.54 | 3.516 (2) | 174 |
| C18—H18c⋯O4v | 0.98 | 2.45 | 3.400 (2) | 164 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
.
Acknowledgments
We thank FAPESP (07/59404-2 to HAS), CNPq (300613/2007 to HAS, and 306532/2009-3 to JZ-S) and CAPES (808/2009 to JZ-S) for financial support. We also thank the University of Malaya for support of the crystallographic facility.
supplementary crystallographic information
Comment
The chemistry and biological activity of C-glycosides has experienced increased attention due to their structural similarity to carbohydrates but also due to their resistance to metabolic processes. Such attributes may lead to improved biological profiles as compared to their O-analogues (Ritchie et al. 2002; Hanessian & Lou, 2000; Hultin, 2005; Zou, 2005). In addition, C-glycosides have also been found embedded in the structure of several bioactive natural products (Nakata, 2005; Nicolaou et al. 2008), and served as chiral building blocks for the stereoselective synthesis of optically active compounds (Somsak, 2001).
The title compound, (I), Fig. 1, was prepared in connection with on-going research into the synthesis of C-glycosides. The absolute structure was confirmed experimentally and shows the chirality at the C9, C12 and C13 atoms to be S, S, and R, respectively. The dihedral angle between the phenyl and the triazole ring is 23.54 (8) °. The 3,6-dihydro-2H-pyran ring has a distorted half-chair conformation with the O1 atom lying 0.6127 (16) Å above the plane defined by the C9–C13 atoms (r.m.s. deviation = 0.1231 Å). The ring puckering parameters are: q2 = 0.4198 (15) Å, q3 = 0.3195 (15) Å, QT = 0.5276 (14) Å and φ2 = 321.1 (2) ° (Cremer & Pople, 1975).
In the crystal packing, the molecules are linked through C–H···O, C–H···N and C–H···π interactions, Table 1. The short C—H···O contact, involving the trizaole-C—H and the carbonyl-O4 atoms, leads to chains along the b axis. These are linked along the a direction into a 2-D array via C—H···π interactions that occur between the methine-C—H and the ring centroid of the trizole ring. Fig. 2. The zigzag layers are stabilized by a number of weaker C–H···O interactions (Table 1) and stack along the b axis with the most significant interaction between them being of the type C—H···N, Fig. 3.
Experimental
The reaction was carried out in a two neck 25 ml flask under a nitrogen atmosphere. To copper iodide (96 mg, 0.5 mmol) was added a solution of ((2R,3S,6S)-3-acetoxy-6-((trimethylsilyl)ethynyl)- 3,6-dihydro-2H-pyran-2-yl)methyl acetate (155 mg, 0.5 mmol) in 2 ml of THF, a solution of phenyl azide (71.4 mg, 0.6 mmol) in 3.5 ml of THF, and finally, drop wise, tetra-n-butyl ammonium fluoride (TBAF) (0.6 ml, 0.6 mmol) was added. The mixture was sonicated in an ultrasound bath for 90 minutes. The reaction mixture was then quenched with 20 ml of ammonium chloride and extracted with 3 x 15 ml of ethyl acetate. The organic phase was washed with 3 x 15 ml of water, dried with MgSO4 and then the solvent evaporated in a rota-vapor. The product was purified through a chromatographic column using ethyl acetate/hexane (1:3) as the eluent. Crystals were grown by slow evaporation from a solution of 15% of acetyl acetate in hexane at 293 K; M.pt: 379–382 K. 1H-NMR (CDCl3, p.p.m., 300 MHz): δ 7.99 (s, 1H); 7.74 (d, 2H, J = 7.8 Hz); 7.51 (m, 3H), 6.29 (m, 1H); 6.01 (d, 1H, J = 10.3 Hz); 5.61 (s, 1H); 5.35 (dd, 1H, J = 2.0 Hz, J = 7.8 Hz); 4.26 (d, 1H, J = 5.6 Hz); d, 1H, J = 2.9 Hz); 4.00 (ddd, 1H, J = 3.0 Hz, J = 5.6 Hz, J = 8.3 Hz); 2.08 (s, 6H); 13C (CDCl3, 75 MHz) δ (p.p.m.) 170.81; 170.38; 146.97; 137.05; 129.88; 129,58; 129,01; 125,96; 120,66; 120,39; 69,78; 67.67; 65.02; 63.08; 21.08; 20.87. HRMS calcd for C18H19N3O5 357.1325. Found: 357.1328.
Refinement
The H atoms were geometrically placed (C–H = 0.95–1.00 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) and Uiso(H) = 1.5Ueq(methyl-C).
Figures
Fig. 1.
The molecular structure of compound (I) showing atom labelling scheme and displacement ellipsoids at the 50% probability level (arbitrary spheres for the H atoms).
Fig. 2.
A view in projection down the c axis showing the supramolecular array sustained by relatviely strong C—H···O contacts (orange dashed lines) formed along the b direction and C—H···π contacts (purple dashed lines) formed along the a direction.
Fig. 3.
A view in projection down the a axis highlighting the stacking of zigzag layers along the b direction. The C—H···O, C—H···π and C—H···N interactions are shown as orange, purple and blue dashed lines, respectively.
Crystal data
| C18H19N3O5 | F(000) = 376 |
| Mr = 357.36 | Dx = 1.384 Mg m−3 |
| Monoclinic, P21 | Cu Kα radiation, λ = 1.54184 Å |
| Hall symbol: P 2yb | Cell parameters from 4088 reflections |
| a = 4.79932 (7) Å | θ = 2.7–74.0° |
| b = 16.6308 (2) Å | µ = 0.86 mm−1 |
| c = 10.76331 (14) Å | T = 100 K |
| β = 93.225 (1)° | Prism, colourless |
| V = 857.73 (2) Å3 | 0.20 × 0.10 × 0.05 mm |
| Z = 2 |
Data collection
| Agilent SuperNova Dual Cu at zero diffractometer with an Atlas detector | 3369 independent reflections |
| Radiation source: fine-focus sealed tube | 3304 reflections with I > 2σ(I) |
| graphite | Rint = 0.019 |
| Detector resolution: 10.4041 pixels mm-1 | θmax = 74.2°, θmin = 4.1° |
| ω scans | h = −5→5 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −20→20 |
| Tmin = 0.848, Tmax = 0.959 | l = −13→8 |
| 5784 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)] = 0.033 | H-atom parameters constrained |
| wR(F2) = 0.084 | w = 1/[σ2(Fo2) + (0.0525P)2 + 0.1259P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.04 | (Δ/σ)max < 0.001 |
| 3369 reflections | Δρmax = 0.14 e Å−3 |
| 237 parameters | Δρmin = −0.19 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 1591 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: −0.09 (15) |
Special details
| 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 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 > 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 | ||
| O1 | −0.1199 (2) | 0.49978 (6) | 0.39298 (9) | 0.0183 (2) | |
| O2 | 0.1131 (3) | 0.41952 (8) | 0.69075 (13) | 0.0374 (3) | |
| O3 | 0.0424 (2) | 0.54932 (7) | 0.63709 (10) | 0.0230 (2) | |
| O4 | 0.0156 (3) | 0.75452 (8) | 0.58495 (11) | 0.0298 (3) | |
| O5 | 0.1489 (2) | 0.70479 (7) | 0.40355 (11) | 0.0226 (2) | |
| N1 | 0.2553 (3) | 0.37406 (8) | 0.10112 (11) | 0.0163 (2) | |
| N2 | 0.2724 (3) | 0.44506 (8) | 0.03950 (12) | 0.0205 (3) | |
| N3 | 0.1016 (3) | 0.49499 (8) | 0.09098 (12) | 0.0202 (3) | |
| C1 | 0.4329 (3) | 0.30870 (9) | 0.07023 (15) | 0.0174 (3) | |
| C2 | 0.5395 (4) | 0.30667 (10) | −0.04686 (15) | 0.0231 (3) | |
| H2 | 0.4855 | 0.3461 | −0.1074 | 0.028* | |
| C3 | 0.7260 (4) | 0.24640 (11) | −0.07433 (16) | 0.0274 (3) | |
| H3 | 0.8035 | 0.2451 | −0.1536 | 0.033* | |
| C4 | 0.7999 (4) | 0.18788 (10) | 0.01356 (17) | 0.0265 (3) | |
| H4 | 0.9275 | 0.1466 | −0.0056 | 0.032* | |
| C5 | 0.6871 (4) | 0.18983 (10) | 0.12911 (17) | 0.0278 (4) | |
| H5 | 0.7362 | 0.1494 | 0.1888 | 0.033* | |
| C6 | 0.5023 (3) | 0.25052 (10) | 0.15854 (15) | 0.0232 (3) | |
| H6 | 0.4251 | 0.2520 | 0.2379 | 0.028* | |
| C7 | 0.0740 (3) | 0.37932 (9) | 0.19199 (13) | 0.0177 (3) | |
| H7 | 0.0251 | 0.3385 | 0.2485 | 0.021* | |
| C8 | −0.0244 (3) | 0.45681 (9) | 0.18467 (13) | 0.0160 (3) | |
| C9 | −0.2265 (3) | 0.49831 (9) | 0.26498 (13) | 0.0176 (3) | |
| H9 | −0.4020 | 0.4658 | 0.2614 | 0.021* | |
| C10 | −0.3016 (3) | 0.58149 (9) | 0.21885 (15) | 0.0192 (3) | |
| H10 | −0.4012 | 0.5874 | 0.1406 | 0.023* | |
| C11 | −0.2323 (3) | 0.64660 (9) | 0.28465 (14) | 0.0200 (3) | |
| H11 | −0.2926 | 0.6977 | 0.2543 | 0.024* | |
| C12 | −0.0613 (3) | 0.64194 (9) | 0.40561 (14) | 0.0193 (3) | |
| H12 | −0.1821 | 0.6498 | 0.4774 | 0.023* | |
| C13 | 0.0863 (3) | 0.56087 (9) | 0.41504 (14) | 0.0181 (3) | |
| H13 | 0.2238 | 0.5577 | 0.3488 | 0.022* | |
| C14 | 0.2357 (3) | 0.54349 (10) | 0.53946 (14) | 0.0225 (3) | |
| H14A | 0.3170 | 0.4888 | 0.5388 | 0.027* | |
| H14B | 0.3896 | 0.5825 | 0.5550 | 0.027* | |
| C15 | −0.0055 (3) | 0.48239 (10) | 0.70412 (15) | 0.0247 (3) | |
| C16 | −0.2217 (4) | 0.49774 (14) | 0.79520 (16) | 0.0342 (4) | |
| H16A | −0.1650 | 0.4725 | 0.8749 | 0.051* | |
| H16B | −0.4003 | 0.4750 | 0.7636 | 0.051* | |
| H16C | −0.2422 | 0.5558 | 0.8070 | 0.051* | |
| C17 | 0.1610 (3) | 0.75859 (9) | 0.49755 (14) | 0.0201 (3) | |
| C18 | 0.3763 (4) | 0.82174 (10) | 0.47939 (18) | 0.0270 (4) | |
| H18A | 0.3102 | 0.8734 | 0.5100 | 0.041* | |
| H18B | 0.4096 | 0.8263 | 0.3907 | 0.041* | |
| H18C | 0.5505 | 0.8069 | 0.5256 | 0.041* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0217 (5) | 0.0174 (5) | 0.0160 (5) | −0.0037 (4) | 0.0037 (4) | −0.0012 (4) |
| O2 | 0.0421 (8) | 0.0277 (7) | 0.0423 (8) | −0.0015 (6) | 0.0020 (6) | 0.0073 (6) |
| O3 | 0.0284 (6) | 0.0250 (6) | 0.0162 (5) | −0.0015 (5) | 0.0055 (4) | −0.0001 (4) |
| O4 | 0.0357 (7) | 0.0314 (7) | 0.0232 (6) | −0.0047 (5) | 0.0090 (5) | −0.0096 (5) |
| O5 | 0.0253 (6) | 0.0199 (5) | 0.0236 (6) | −0.0061 (4) | 0.0104 (5) | −0.0069 (4) |
| N1 | 0.0186 (6) | 0.0138 (6) | 0.0165 (6) | −0.0001 (5) | 0.0014 (5) | 0.0012 (5) |
| N2 | 0.0269 (7) | 0.0157 (6) | 0.0193 (6) | 0.0015 (5) | 0.0053 (5) | 0.0025 (5) |
| N3 | 0.0234 (6) | 0.0184 (6) | 0.0194 (6) | 0.0005 (5) | 0.0055 (5) | 0.0002 (5) |
| C1 | 0.0170 (7) | 0.0150 (6) | 0.0203 (7) | −0.0005 (6) | 0.0013 (5) | −0.0042 (6) |
| C2 | 0.0259 (8) | 0.0236 (7) | 0.0201 (8) | 0.0013 (6) | 0.0037 (6) | −0.0024 (6) |
| C3 | 0.0283 (8) | 0.0291 (9) | 0.0253 (8) | 0.0004 (7) | 0.0064 (6) | −0.0080 (7) |
| C4 | 0.0239 (8) | 0.0201 (8) | 0.0355 (9) | 0.0033 (6) | 0.0016 (7) | −0.0088 (7) |
| C5 | 0.0312 (9) | 0.0201 (8) | 0.0319 (9) | 0.0042 (7) | −0.0014 (7) | 0.0011 (7) |
| C6 | 0.0266 (8) | 0.0203 (7) | 0.0228 (7) | 0.0027 (7) | 0.0027 (6) | 0.0007 (6) |
| C7 | 0.0182 (7) | 0.0176 (7) | 0.0174 (7) | −0.0019 (6) | 0.0029 (5) | 0.0005 (6) |
| C8 | 0.0162 (7) | 0.0162 (7) | 0.0156 (7) | −0.0027 (5) | 0.0010 (5) | −0.0019 (5) |
| C9 | 0.0172 (7) | 0.0180 (7) | 0.0177 (7) | −0.0022 (6) | 0.0025 (5) | −0.0017 (6) |
| C10 | 0.0161 (7) | 0.0209 (8) | 0.0210 (7) | 0.0008 (5) | 0.0033 (5) | 0.0009 (6) |
| C11 | 0.0189 (7) | 0.0186 (7) | 0.0233 (8) | 0.0015 (6) | 0.0074 (6) | 0.0012 (6) |
| C12 | 0.0195 (7) | 0.0173 (7) | 0.0219 (8) | −0.0037 (6) | 0.0078 (6) | −0.0030 (6) |
| C13 | 0.0180 (7) | 0.0190 (7) | 0.0178 (7) | −0.0037 (6) | 0.0057 (5) | −0.0021 (5) |
| C14 | 0.0210 (7) | 0.0280 (8) | 0.0188 (7) | −0.0011 (6) | 0.0045 (6) | −0.0012 (6) |
| C15 | 0.0238 (8) | 0.0304 (9) | 0.0195 (7) | −0.0080 (7) | −0.0032 (6) | 0.0028 (6) |
| C16 | 0.0289 (9) | 0.0513 (12) | 0.0226 (8) | −0.0084 (9) | 0.0036 (7) | 0.0073 (8) |
| C17 | 0.0205 (7) | 0.0174 (7) | 0.0221 (7) | 0.0028 (6) | −0.0005 (6) | −0.0031 (6) |
| C18 | 0.0266 (8) | 0.0196 (8) | 0.0349 (9) | −0.0029 (6) | 0.0016 (7) | −0.0030 (6) |
Geometric parameters (Å, °)
| O1—C13 | 1.4289 (17) | C7—C8 | 1.373 (2) |
| O1—C9 | 1.4425 (17) | C7—H7 | 0.9500 |
| O2—C15 | 1.203 (2) | C8—C9 | 1.503 (2) |
| O3—C15 | 1.353 (2) | C9—C10 | 1.507 (2) |
| O3—C14 | 1.4435 (18) | C9—H9 | 1.0000 |
| O4—C17 | 1.204 (2) | C10—C11 | 1.326 (2) |
| O5—C17 | 1.3494 (19) | C10—H10 | 0.9500 |
| O5—C12 | 1.4537 (18) | C11—C12 | 1.501 (2) |
| N1—C7 | 1.3482 (19) | C11—H11 | 0.9500 |
| N1—N2 | 1.3591 (18) | C12—C13 | 1.524 (2) |
| N1—C1 | 1.4320 (19) | C12—H12 | 1.0000 |
| N2—N3 | 1.3113 (19) | C13—C14 | 1.511 (2) |
| N3—C8 | 1.3617 (19) | C13—H13 | 1.0000 |
| C1—C6 | 1.384 (2) | C14—H14A | 0.9900 |
| C1—C2 | 1.387 (2) | C14—H14B | 0.9900 |
| C2—C3 | 1.387 (2) | C15—C16 | 1.489 (2) |
| C2—H2 | 0.9500 | C16—H16A | 0.9800 |
| C3—C4 | 1.389 (3) | C16—H16B | 0.9800 |
| C3—H3 | 0.9500 | C16—H16C | 0.9800 |
| C4—C5 | 1.384 (3) | C17—C18 | 1.494 (2) |
| C4—H4 | 0.9500 | C18—H18A | 0.9800 |
| C5—C6 | 1.392 (2) | C18—H18B | 0.9800 |
| C5—H5 | 0.9500 | C18—H18C | 0.9800 |
| C6—H6 | 0.9500 | ||
| C13—O1—C9 | 112.08 (11) | C9—C10—H10 | 119.1 |
| C15—O3—C14 | 117.93 (13) | C10—C11—C12 | 121.97 (14) |
| C17—O5—C12 | 117.77 (12) | C10—C11—H11 | 119.0 |
| C7—N1—N2 | 110.90 (12) | C12—C11—H11 | 119.0 |
| C7—N1—C1 | 129.40 (13) | O5—C12—C11 | 107.19 (12) |
| N2—N1—C1 | 119.55 (12) | O5—C12—C13 | 108.46 (12) |
| N3—N2—N1 | 106.72 (12) | C11—C12—C13 | 109.44 (12) |
| N2—N3—C8 | 109.38 (13) | O5—C12—H12 | 110.6 |
| C6—C1—C2 | 121.36 (14) | C11—C12—H12 | 110.6 |
| C6—C1—N1 | 119.64 (14) | C13—C12—H12 | 110.6 |
| C2—C1—N1 | 118.96 (14) | O1—C13—C14 | 107.51 (12) |
| C3—C2—C1 | 119.13 (15) | O1—C13—C12 | 107.63 (12) |
| C3—C2—H2 | 120.4 | C14—C13—C12 | 115.09 (13) |
| C1—C2—H2 | 120.4 | O1—C13—H13 | 108.8 |
| C2—C3—C4 | 120.28 (15) | C14—C13—H13 | 108.8 |
| C2—C3—H3 | 119.9 | C12—C13—H13 | 108.8 |
| C4—C3—H3 | 119.9 | O3—C14—C13 | 109.89 (12) |
| C5—C4—C3 | 119.84 (15) | O3—C14—H14A | 109.7 |
| C5—C4—H4 | 120.1 | C13—C14—H14A | 109.7 |
| C3—C4—H4 | 120.1 | O3—C14—H14B | 109.7 |
| C4—C5—C6 | 120.51 (16) | C13—C14—H14B | 109.7 |
| C4—C5—H5 | 119.7 | H14A—C14—H14B | 108.2 |
| C6—C5—H5 | 119.7 | O2—C15—O3 | 123.73 (16) |
| C1—C6—C5 | 118.85 (15) | O2—C15—C16 | 125.44 (17) |
| C1—C6—H6 | 120.6 | O3—C15—C16 | 110.83 (16) |
| C5—C6—H6 | 120.6 | C15—C16—H16A | 109.5 |
| N1—C7—C8 | 104.66 (13) | C15—C16—H16B | 109.5 |
| N1—C7—H7 | 127.7 | H16A—C16—H16B | 109.5 |
| C8—C7—H7 | 127.7 | C15—C16—H16C | 109.5 |
| N3—C8—C7 | 108.34 (13) | H16A—C16—H16C | 109.5 |
| N3—C8—C9 | 122.66 (13) | H16B—C16—H16C | 109.5 |
| C7—C8—C9 | 128.96 (14) | O4—C17—O5 | 123.09 (14) |
| O1—C9—C8 | 110.58 (12) | O4—C17—C18 | 125.26 (14) |
| O1—C9—C10 | 111.38 (12) | O5—C17—C18 | 111.64 (14) |
| C8—C9—C10 | 112.47 (12) | C17—C18—H18A | 109.5 |
| O1—C9—H9 | 107.4 | C17—C18—H18B | 109.5 |
| C8—C9—H9 | 107.4 | H18A—C18—H18B | 109.5 |
| C10—C9—H9 | 107.4 | C17—C18—H18C | 109.5 |
| C11—C10—C9 | 121.71 (14) | H18A—C18—H18C | 109.5 |
| C11—C10—H10 | 119.1 | H18B—C18—H18C | 109.5 |
| C7—N1—N2—N3 | −0.21 (17) | C7—C8—C9—O1 | 60.2 (2) |
| C1—N1—N2—N3 | −176.19 (13) | N3—C8—C9—C10 | 7.9 (2) |
| N1—N2—N3—C8 | −0.02 (16) | C7—C8—C9—C10 | −174.61 (14) |
| C7—N1—C1—C6 | −21.1 (2) | O1—C9—C10—C11 | 9.9 (2) |
| N2—N1—C1—C6 | 154.08 (15) | C8—C9—C10—C11 | −114.87 (16) |
| C7—N1—C1—C2 | 161.09 (15) | C9—C10—C11—C12 | 3.5 (2) |
| N2—N1—C1—C2 | −23.8 (2) | C17—O5—C12—C11 | 124.32 (14) |
| C6—C1—C2—C3 | −2.0 (2) | C17—O5—C12—C13 | −117.60 (14) |
| N1—C1—C2—C3 | 175.82 (14) | C10—C11—C12—O5 | 135.30 (15) |
| C1—C2—C3—C4 | 1.4 (2) | C10—C11—C12—C13 | 17.9 (2) |
| C2—C3—C4—C5 | −0.1 (3) | C9—O1—C13—C14 | −165.40 (12) |
| C3—C4—C5—C6 | −0.7 (3) | C9—O1—C13—C12 | 70.07 (14) |
| C2—C1—C6—C5 | 1.2 (2) | O5—C12—C13—O1 | −169.07 (11) |
| N1—C1—C6—C5 | −176.58 (15) | C11—C12—C13—O1 | −52.44 (15) |
| C4—C5—C6—C1 | 0.2 (3) | O5—C12—C13—C14 | 71.10 (15) |
| N2—N1—C7—C8 | 0.34 (16) | C11—C12—C13—C14 | −172.27 (13) |
| C1—N1—C7—C8 | 175.81 (14) | C15—O3—C14—C13 | 117.54 (15) |
| N2—N3—C8—C7 | 0.23 (17) | O1—C13—C14—O3 | −63.44 (16) |
| N2—N3—C8—C9 | 178.14 (13) | C12—C13—C14—O3 | 56.45 (17) |
| N1—C7—C8—N3 | −0.34 (16) | C14—O3—C15—O2 | 3.6 (2) |
| N1—C7—C8—C9 | −178.08 (14) | C14—O3—C15—C16 | −176.58 (13) |
| C13—O1—C9—C8 | 78.46 (14) | C12—O5—C17—O4 | 3.6 (2) |
| C13—O1—C9—C10 | −47.37 (15) | C12—O5—C17—C18 | −177.05 (14) |
| N3—C8—C9—O1 | −117.28 (15) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C7—H7···O4i | 0.95 | 2.29 | 3.2207 (19) | 167 |
| C9—H9···Cg1ii | 1.00 | 2.68 | 3.5362 (16) | 144 |
| C16—H16a···N3iii | 0.98 | 2.62 | 3.463 (2) | 145 |
| C16—H16b···O2ii | 0.98 | 2.59 | 3.570 (2) | 177 |
| C18—H18a···O1iv | 0.98 | 2.54 | 3.516 (2) | 174 |
| C18—H18c···O4v | 0.98 | 2.45 | 3.400 (2) | 164 |
Symmetry codes: (i) −x, y−1/2, −z+1; (ii) x−1, y, z; (iii) x, y, z+1; (iv) −x, y+1/2, −z+1; (v) x+1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5093).
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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/S1600536811037305/hg5093sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811037305/hg5093Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811037305/hg5093Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



