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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 29;67(Pt 5):o1214. doi: 10.1107/S1600536811014292

Ethyl 1-benzyl-1,2,3,3a,4,10b-hexa­hydro­pyrrolo­[2′,3′:3,4]pyrrolo­[1,2-a]benzimidazole-2-carboxyl­ate

Liping Meng a, James C Fettinger a, Mark J Kurth a,*
PMCID: PMC3089295  PMID: 21754512

Abstract

The title mol­ecule, C22H23N3O2, was obtained via an intra­molecular cyclo­addition of an azomethine ylide and an alkene tethered by a benzimidazole unit. The benzoimidazole unit is essentially planar, with an r.m.s. deviation of 0.0087 Å from the nine constituent atoms. It has a cis fusion of the two pyrrolidine rings as well as a cis ester appendage. The two pyrrolidine rings rings have envelope conformations. The crystal packing is stabilized by aromatic π–π stacking of parallel benzimidazole ring systems, with a centroid-to-centroid distance of 3.518 (6) Å. Weak inter­molecular C—H⋯O contacts may also play a role in the stability of the packing.

Related literature

Polycyclic nitro­gen-containing heterocycles form the basic skeleton of numerous alkaloids and physiologically active compounds, see: Southon & Buckingham (1989). Conformational studies have been reported for related pyrrolidino[3,4-b]pyrrolidine-2-carboxyl­ates obtained from intra­molecular cyclo­addition of azomethine ylides, see: Cheng et al. (2001); Meng et al. (2007). For related literature on the pharmaceutical properties of benzimidazole and pyrrolidine, see: Gudmundsson et al. (2000); Hamilton & Steiner (1997). For related literature on the azomethine ylide cycloaddition in similar systems, Pedrosa et al. (2006); Yang et al. (2006).graphic file with name e-67-o1214-scheme1.jpg

Experimental

Crystal data

  • C22H23N3O2

  • M r = 361.43

  • Monoclinic, Inline graphic

  • a = 9.2498 (5) Å

  • b = 13.8999 (7) Å

  • c = 14.2258 (7) Å

  • β = 90.345 (1)°

  • V = 1829.00 (16) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 90 K

  • 0.39 × 0.16 × 0.13 mm

Data collection

  • Bruker SMART1000 CCD area-detector diffractometer

  • Absorption correction: numerical (SADABS; Blessing, 1995; Sheldrick, 2007) T min = 0.962, T max = 0.989

  • 16147 measured reflections

  • 4194 independent reflections

  • 3080 reflections with I > 2σ(I)

  • R int = 0.037

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.095

  • S = 1.09

  • 4194 reflections

  • 336 parameters

  • All H-atom parameters refined

  • Δρmax = 0.37 e Å−3

  • Δρmin = −0.27 e Å−3

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL/PC (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811014292/wn2427sup1.cif

e-67-o1214-sup1.cif (21.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014292/wn2427Isup2.hkl

e-67-o1214-Isup2.hkl (205.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

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

D—H⋯A D—H H⋯A DA D—H⋯A
C11—H11B⋯O12i 1.005 (15) 2.399 (15) 3.3344 (17) 154.5 (12)
C18—H18⋯O12ii 0.968 (15) 2.514 (16) 3.3505 (17) 144.6 (12)

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

Acknowledgments

The authors thank the National Science Foundation (grant No. CHE-0910870) and the National Institutes of Health (grant No. GM0891583) for financial support of this work.

supplementary crystallographic information

Comment

Polycyclic nitrogen-containing heterocycles form the basic skeleton of numerous alkaloids and physiologically active compounds (Southon & Buckingham, 1989). The title polycyclic N-heterocycle, ethyl 1-benzylpyrrolidino[2',3':3,4]pyrrolidino[1,2-a] benzimidazole-2-carboxylate, was obtained via an intramolecular azomethine ylide cycloaddition and possesses two medicinally relevant pharmacophores – benzimidazole and pyrrolidine (Gudmundsson et al., 2000; Hamilton & Steiner, 1997)– in one rigid molecule; the title compound may afford important bioactivity.

In the structure of the title compound (Fig. 1), the benzoimidazole unit is essentially planar, with a root mean square deviation of 0.0087 Å from the nine constituent atoms. The two pyrrolidine rings have envelope forms and are cis fused, which is consistent with conventional azomethine ylide cycloadditions in similar systems (Pedrosa et al., 2006; Yang et al., 2006). However, unlike the previously reported analogues obtained from an intramolecular azomethine ylide and alkene cycloaddition tethered by an oxazolidin-2-one (Cheng et al., 2001), the ester appendage in the title structure was unambiguously assigned as cis to the angular protons H2A and H10A by X-ray crystallography. The crystal packing (Fig. 2) exhibits π–π stacking of parallel benzimidazole ring systems, with a Cg1···Cg2 distance of 3.518 Å [Cg1 and Cg2 are the centroids of the C3A–C8A benzene ring in one molecule and the C2B/N2/C3A/C8A/N8 imidazole ring in the other molecule, respectively]. Intermolecular C—H···O contacts may also play a role in the stability of the packing.

Experimental

The title compound was prepared from 1-allyl-1H-benzimidazole-2-carbaldehyde, N-benzylglycine ethyl ester hydrochloride, and triethylamine according to the procedure reported by Meng et al. (2007). Colourless blocks of the title compound were obtained by recrystallization from EtOAc/n-hexane 1:1 with slow evaporation at room temperature. These crystals were suitable for X-ray crystallography.

Refinement

H atoms were located directly in a difference Fourier map and then allowed to refine freely throughout the final convergence stage. The final structure was refined to convergence [Δ/σ≤ 0.001]. The final difference Fourier map was featureless, indicating that the structure is both correct and complete.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound. Ellipsoids are drawn at the 50% probability level. H atoms are represented as small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

The crystal packing of the title compound with a view of the C—H···O (dashed lines) and π–π interactions.

Crystal data

C22H23N3O2 F(000) = 768
Mr = 361.43 Dx = 1.313 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 7133 reflections
a = 9.2498 (5) Å θ = 2.6–27.5°
b = 13.8999 (7) Å µ = 0.09 mm1
c = 14.2258 (7) Å T = 90 K
β = 90.345 (1)° Block, colourless
V = 1829.00 (16) Å3 0.39 × 0.16 × 0.13 mm
Z = 4

Data collection

Bruker SMART1000 CCD area-detector diffractometer 4194 independent reflections
Radiation source: fine-focus sealed tube 3080 reflections with I > 2σ(I)
graphite Rint = 0.037
ω and φ scans θmax = 27.5°, θmin = 2.1°
Absorption correction: numerical (SADABS; Blessing, 1995; Sheldrick, 2007) h = −12→12
Tmin = 0.962, Tmax = 0.989 k = −18→18
16147 measured reflections l = −18→18

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)] = 0.037 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.095 All H-atom parameters refined
S = 1.09 w = 1/[σ2(Fo2) + (0.0417P)2 + 0.3839P] where P = (Fo2 + 2Fc2)/3
4194 reflections (Δ/σ)max = 0.001
336 parameters Δρmax = 0.37 e Å3
0 restraints Δρmin = −0.27 e Å3

Special details

Experimental. A colourless block with approximate orthogonal dimensions 0.39 × 0.16 × 0.13 mm3 was placed and optically centered on the Bruker SMART1000 CCD system at -183°C. The initial unit cell was indexed using a least-squares analysis of a random set of reflections collected from three series of 0.3° wide ω scans, 10 s per frame, and 25 frames per series that were well distributed in reciprocal space. Four ω-scan data frame series were collected [Mo Kα] with 0.3° wide scans, 30 s per frame and 606, 435, 606, 435 frames collected per series at varying φ angles (φ = 0°, 90°, 180°, 270°), respectively.
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. The crystal to detector distance was 4.123 cm, thus providing a complete sphere of data to 2θmax = 55.06°. A total of 23465 reflections were collected and corrected for Lorentz and polarization effects and absorption using Blessing's method (Blessing, 1995) as incorporated into the program SADABS with 4390 unique. All crystallographic calculations were performed on a personal computer (PC) with a Pentium 3.20 GHz processor and 1 GB of extended memory. The SHELXTL program package was implemented to determine the probable space group and set up the initial files. System symmetry, systematic absences and intensity statistics indicated the centrosymmetric monoclinic non-standard space group P21/n (No. 14). The structure was determined by direct methods with the successful location of a majority of the molecule within the asymmetric unit using the program XS. The structure was refined with XL. The 23465 data collected were merged based upon identical indices yielding 16536 data [R(int) = 0.0245] that were truncated to 2θmax = 55.0° resulting in 16147 data that were further merged during least-squares refinement to 4194 unique data [R(int) = 0.0373]. A single least-squares difference Fourier cycle was required to locate the remaining non-H atoms. All non-H atoms were refined anisotropically. 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 0.11370 (13) 0.83406 (9) 0.93388 (9) 0.0171 (3)
H1 0.1841 (15) 0.8014 (10) 0.8905 (10) 0.016 (3)*
N1 −0.03076 (11) 0.79245 (7) 0.92753 (7) 0.0167 (2)
C2A −0.02373 (14) 0.70281 (9) 0.98214 (9) 0.0168 (3)
H2A −0.1230 (16) 0.6828 (10) 0.9972 (10) 0.021 (4)*
C2B 0.05845 (13) 0.61970 (9) 0.93939 (9) 0.0164 (3)
N2 0.04725 (11) 0.56851 (8) 0.86159 (7) 0.0188 (2)
C3A 0.15526 (14) 0.49885 (9) 0.87233 (9) 0.0178 (3)
C4 0.19276 (15) 0.42310 (10) 0.81285 (9) 0.0215 (3)
H4 0.1418 (16) 0.4118 (10) 0.7547 (11) 0.024 (4)*
C5 0.30288 (15) 0.36208 (10) 0.84115 (10) 0.0239 (3)
H5 0.3296 (16) 0.3071 (11) 0.8029 (11) 0.024 (4)*
C6 0.37646 (15) 0.37548 (10) 0.92687 (10) 0.0231 (3)
H6 0.4508 (16) 0.3301 (11) 0.9460 (10) 0.025 (4)*
C7 0.34082 (14) 0.44980 (10) 0.98730 (10) 0.0205 (3)
H7 0.3892 (16) 0.4588 (10) 1.0466 (11) 0.023 (4)*
C8A 0.22957 (14) 0.51062 (9) 0.95859 (9) 0.0176 (3)
N8 0.16544 (11) 0.58997 (8) 0.99883 (7) 0.0173 (2)
C9 0.16669 (15) 0.63878 (10) 1.08991 (9) 0.0191 (3)
H9A 0.2688 (16) 0.6555 (10) 1.1086 (10) 0.021 (4)*
H9B 0.1242 (15) 0.5967 (10) 1.1379 (10) 0.022 (4)*
C10A 0.07245 (14) 0.72792 (9) 1.06910 (9) 0.0180 (3)
H10A 0.0137 (14) 0.7435 (9) 1.1239 (10) 0.013 (3)*
C11 0.15928 (15) 0.81681 (10) 1.03687 (9) 0.0193 (3)
H11A 0.2653 (18) 0.8059 (11) 1.0440 (11) 0.029 (4)*
H11B 0.1335 (16) 0.8755 (11) 1.0745 (11) 0.025 (4)*
C12 0.11502 (14) 0.93996 (9) 0.90881 (9) 0.0182 (3)
O12 0.01249 (10) 0.98789 (7) 0.88602 (7) 0.0248 (2)
C13 0.27147 (16) 1.07485 (10) 0.89143 (10) 0.0225 (3)
H13A 0.2190 (16) 1.1145 (11) 0.9382 (11) 0.023 (4)*
H13B 0.2268 (16) 1.0867 (10) 0.8302 (11) 0.022 (4)*
O13 0.25101 (10) 0.97384 (6) 0.91573 (6) 0.0201 (2)
C14 0.43191 (16) 1.09273 (11) 0.89238 (11) 0.0251 (3)
H14A 0.4769 (18) 1.0798 (12) 0.9539 (13) 0.037 (5)*
H14B 0.4516 (18) 1.1615 (13) 0.8784 (11) 0.038 (5)*
H14C 0.4819 (17) 1.0527 (12) 0.8441 (12) 0.035 (4)*
C15 −0.08571 (14) 0.78122 (10) 0.83087 (9) 0.0179 (3)
H15A −0.0297 (15) 0.7327 (10) 0.7948 (10) 0.018 (4)*
H15B −0.0739 (15) 0.8460 (11) 0.8007 (10) 0.018 (4)*
C16 −0.24288 (14) 0.75165 (9) 0.82970 (9) 0.0178 (3)
C17 −0.28700 (15) 0.66465 (10) 0.79108 (9) 0.0205 (3)
H17 −0.2161 (17) 0.6209 (11) 0.7651 (11) 0.030 (4)*
C18 −0.43276 (15) 0.63824 (10) 0.79093 (9) 0.0228 (3)
H18 −0.4629 (16) 0.5773 (11) 0.7644 (11) 0.027 (4)*
C19 −0.53434 (15) 0.69891 (11) 0.83067 (9) 0.0232 (3)
H19 −0.6361 (17) 0.6801 (11) 0.8303 (10) 0.024 (4)*
C20 −0.49157 (15) 0.78651 (10) 0.86906 (9) 0.0224 (3)
H20 −0.5630 (16) 0.8300 (11) 0.8959 (10) 0.022 (4)*
C21 −0.34683 (14) 0.81280 (10) 0.86831 (9) 0.0205 (3)
H21 −0.3146 (16) 0.8746 (11) 0.8952 (10) 0.022 (4)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0135 (6) 0.0187 (6) 0.0189 (6) 0.0002 (5) 0.0018 (5) −0.0014 (5)
N1 0.0149 (5) 0.0182 (6) 0.0170 (5) −0.0009 (4) −0.0002 (4) 0.0011 (4)
C2A 0.0146 (6) 0.0196 (7) 0.0161 (6) −0.0012 (5) 0.0012 (5) 0.0005 (5)
C2B 0.0145 (6) 0.0186 (6) 0.0162 (6) −0.0027 (5) 0.0009 (5) 0.0025 (5)
N2 0.0194 (6) 0.0191 (6) 0.0180 (5) 0.0006 (4) 0.0011 (4) 0.0000 (4)
C3A 0.0165 (6) 0.0193 (6) 0.0177 (6) −0.0013 (5) 0.0030 (5) 0.0042 (5)
C4 0.0244 (7) 0.0236 (7) 0.0164 (7) −0.0002 (6) 0.0044 (5) 0.0006 (5)
C5 0.0251 (7) 0.0226 (7) 0.0242 (7) 0.0017 (6) 0.0096 (6) 0.0001 (6)
C6 0.0172 (7) 0.0221 (7) 0.0300 (8) 0.0013 (6) 0.0049 (6) 0.0053 (6)
C7 0.0159 (7) 0.0225 (7) 0.0230 (7) −0.0026 (5) 0.0004 (5) 0.0050 (5)
C8A 0.0173 (6) 0.0179 (6) 0.0177 (6) −0.0027 (5) 0.0028 (5) 0.0026 (5)
N8 0.0170 (6) 0.0184 (5) 0.0165 (5) −0.0004 (4) −0.0005 (4) 0.0013 (4)
C9 0.0207 (7) 0.0208 (7) 0.0157 (6) −0.0023 (5) −0.0014 (5) −0.0002 (5)
C10A 0.0179 (6) 0.0216 (7) 0.0146 (6) −0.0013 (5) 0.0022 (5) −0.0014 (5)
C11 0.0194 (7) 0.0182 (7) 0.0204 (7) −0.0005 (5) −0.0029 (5) 0.0004 (5)
C12 0.0187 (7) 0.0213 (7) 0.0146 (6) 0.0013 (5) 0.0022 (5) −0.0021 (5)
O12 0.0232 (5) 0.0226 (5) 0.0284 (5) 0.0044 (4) −0.0022 (4) 0.0015 (4)
C13 0.0289 (8) 0.0154 (7) 0.0233 (7) −0.0024 (6) −0.0026 (6) 0.0023 (5)
O13 0.0207 (5) 0.0161 (5) 0.0235 (5) −0.0020 (4) 0.0003 (4) 0.0015 (4)
C14 0.0297 (8) 0.0199 (7) 0.0257 (8) −0.0066 (6) −0.0002 (6) 0.0008 (6)
C15 0.0159 (6) 0.0221 (7) 0.0156 (6) 0.0008 (5) 0.0010 (5) 0.0000 (5)
C16 0.0173 (7) 0.0229 (7) 0.0130 (6) 0.0012 (5) −0.0013 (5) 0.0031 (5)
C17 0.0201 (7) 0.0248 (7) 0.0164 (6) 0.0032 (6) −0.0009 (5) 0.0009 (5)
C18 0.0242 (7) 0.0247 (7) 0.0193 (7) −0.0027 (6) −0.0052 (5) 0.0014 (6)
C19 0.0165 (7) 0.0322 (8) 0.0209 (7) −0.0019 (6) −0.0033 (5) 0.0043 (6)
C20 0.0171 (7) 0.0305 (8) 0.0195 (7) 0.0047 (6) −0.0005 (5) 0.0010 (6)
C21 0.0206 (7) 0.0232 (7) 0.0177 (6) 0.0010 (6) −0.0011 (5) −0.0008 (5)

Geometric parameters (Å, °)

C1—N1 1.4582 (16) C10A—C11 1.5448 (18)
C1—C12 1.5147 (18) C10A—H10A 0.977 (14)
C1—C11 1.5409 (18) C11—H11A 0.997 (16)
C1—H1 1.008 (14) C11—H11B 1.005 (15)
N1—C2A 1.4696 (16) C12—O12 1.2019 (16)
N1—C15 1.4714 (16) C12—O13 1.3462 (15)
C2A—C2B 1.5126 (18) C13—O13 1.4584 (16)
C2A—C10A 1.5590 (17) C13—C14 1.505 (2)
C2A—H2A 0.984 (15) C13—H13A 0.993 (15)
C2B—N2 1.3193 (16) C13—H13B 0.976 (15)
C2B—N8 1.3620 (16) C14—H14A 0.983 (18)
N2—C3A 1.3990 (17) C14—H14B 0.994 (18)
C3A—C4 1.3959 (18) C14—H14C 0.999 (17)
C3A—C8A 1.4125 (18) C15—C16 1.5108 (18)
C4—C5 1.383 (2) C15—H15A 0.994 (14)
C4—H4 0.963 (16) C15—H15B 1.004 (15)
C5—C6 1.405 (2) C16—C17 1.3885 (19)
C5—H5 0.971 (15) C16—C21 1.3982 (18)
C6—C7 1.385 (2) C17—C18 1.3973 (19)
C6—H6 0.971 (16) C17—H17 0.969 (16)
C7—C8A 1.3912 (18) C18—C19 1.386 (2)
C7—H7 0.961 (15) C18—H18 0.967 (16)
C8A—N8 1.3785 (16) C19—C20 1.391 (2)
N8—C9 1.4625 (16) C19—H19 0.977 (15)
C9—C10A 1.5425 (18) C20—C21 1.3879 (19)
C9—H9A 1.006 (15) C20—H20 0.975 (15)
C9—H9B 0.983 (15) C21—H21 0.986 (15)
N1—C1—C12 112.30 (10) C9—C10A—H10A 110.0 (8)
N1—C1—C11 104.04 (10) C11—C10A—H10A 110.6 (8)
C12—C1—C11 111.87 (11) C2A—C10A—H10A 111.4 (8)
N1—C1—H1 112.2 (8) C1—C11—C10A 105.48 (10)
C12—C1—H1 106.7 (8) C1—C11—H11A 112.6 (9)
C11—C1—H1 109.7 (8) C10A—C11—H11A 111.2 (9)
C1—N1—C2A 105.42 (10) C1—C11—H11B 108.4 (9)
C1—N1—C15 114.29 (10) C10A—C11—H11B 111.5 (9)
C2A—N1—C15 114.70 (10) H11A—C11—H11B 107.8 (12)
N1—C2A—C2B 117.12 (10) O12—C12—O13 124.14 (12)
N1—C2A—C10A 104.65 (10) O12—C12—C1 126.49 (12)
C2B—C2A—C10A 101.79 (10) O13—C12—C1 109.37 (11)
N1—C2A—H2A 108.5 (8) O13—C13—C14 106.64 (11)
C2B—C2A—H2A 110.1 (9) O13—C13—H13A 108.1 (9)
C10A—C2A—H2A 114.8 (8) C14—C13—H13A 112.9 (9)
N2—C2B—N8 114.23 (11) O13—C13—H13B 108.6 (9)
N2—C2B—C2A 135.40 (12) C14—C13—H13B 113.1 (9)
N8—C2B—C2A 110.31 (11) H13A—C13—H13B 107.4 (12)
C2B—N2—C3A 103.25 (11) C12—O13—C13 116.23 (10)
C4—C3A—N2 129.48 (12) C13—C14—H14A 112.9 (10)
C4—C3A—C8A 119.52 (12) C13—C14—H14B 109.8 (10)
N2—C3A—C8A 110.99 (11) H14A—C14—H14B 106.1 (14)
C5—C4—C3A 118.11 (13) C13—C14—H14C 111.3 (10)
C5—C4—H4 120.4 (9) H14A—C14—H14C 108.3 (14)
C3A—C4—H4 121.5 (9) H14B—C14—H14C 108.2 (13)
C4—C5—C6 121.55 (13) N1—C15—C16 111.48 (10)
C4—C5—H5 120.6 (9) N1—C15—H15A 112.1 (8)
C6—C5—H5 117.8 (9) C16—C15—H15A 108.3 (8)
C7—C6—C5 121.44 (13) N1—C15—H15B 105.5 (8)
C7—C6—H6 118.8 (9) C16—C15—H15B 110.3 (8)
C5—C6—H6 119.7 (9) H15A—C15—H15B 109.2 (11)
C6—C7—C8A 116.70 (13) C17—C16—C21 118.93 (12)
C6—C7—H7 122.1 (9) C17—C16—C15 121.45 (12)
C8A—C7—H7 121.2 (9) C21—C16—C15 119.62 (12)
N8—C8A—C7 133.13 (12) C16—C17—C18 120.71 (13)
N8—C8A—C3A 104.19 (11) C16—C17—H17 119.9 (9)
C7—C8A—C3A 122.68 (12) C18—C17—H17 119.3 (9)
C2B—N8—C8A 107.32 (10) C19—C18—C17 119.74 (13)
C2B—N8—C9 114.28 (11) C19—C18—H18 119.8 (9)
C8A—N8—C9 137.56 (11) C17—C18—H18 120.4 (9)
N8—C9—C10A 101.61 (10) C18—C19—C20 120.07 (13)
N8—C9—H9A 110.0 (8) C18—C19—H19 119.4 (9)
C10A—C9—H9A 113.2 (8) C20—C19—H19 120.6 (9)
N8—C9—H9B 109.8 (9) C21—C20—C19 119.96 (13)
C10A—C9—H9B 112.6 (9) C21—C20—H20 119.7 (9)
H9A—C9—H9B 109.4 (12) C19—C20—H20 120.3 (9)
C9—C10A—C11 113.90 (11) C20—C21—C16 120.58 (13)
C9—C10A—C2A 106.95 (10) C20—C21—H21 121.1 (9)
C11—C10A—C2A 103.81 (10) C16—C21—H21 118.4 (9)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C11—H11B···O12i 1.005 (15) 2.399 (15) 3.3344 (17) 154.5 (12)
C18—H18···O12ii 0.968 (15) 2.514 (16) 3.3505 (17) 144.6 (12)

Symmetry codes: (i) −x, −y+2, −z+2; (ii) −x−1/2, y−1/2, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WN2427).

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 datablocks global, I. DOI: 10.1107/S1600536811014292/wn2427sup1.cif

e-67-o1214-sup1.cif (21.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014292/wn2427Isup2.hkl

e-67-o1214-Isup2.hkl (205.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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