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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Feb 11;65(Pt 3):o501–o502. doi: 10.1107/S1600536809004255

4-(9-Anthr­yl)-1-phenylspiro­[azetidine-3,9′-xanthen]-2-one

Ísmail Çelik a, Mehmet Akkurt b,*, Aliasghar Jarrahpour c, Edris Ebrahimi c, Orhan Büyükgüngör d
PMCID: PMC2968600  PMID: 21582166

Abstract

The β-lactam ring of the title compound, C35H23NO2, is nearly planar with a maximum deviation of 0.003 (3) Å from the mean plane. It makes dihedral angles of 17.4 (2), 85.22 (17) and 65.39 (16)°, respectively, with the phenyl, xanthene and anthracene ring systems. In the crystal structure, there are intra­molecular C—H⋯O and C—H⋯N contacts and mol­ecules are also linked by C—H⋯π inter­actions.

Related literature

For general background on β-lactam anti­biotics, see: Banik et al. (2003); Jarrahpour & Khalili (2007); Miller (2000); Palomo et al. (2004). For the crystal structures of related compounds, see: Akkurt, Jarrahpour et al. (2008); Akkurt, Karaca et al. (2008); Pınar et al. (2006). For geometric analysis, see: Cremer & Pople (1975).graphic file with name e-65-0o501-scheme1.jpg

Experimental

Crystal data

  • C35H23NO2

  • M r = 489.54

  • Monoclinic, Inline graphic

  • a = 13.6906 (8) Å

  • b = 13.3085 (7) Å

  • c = 17.3527 (10) Å

  • β = 127.548 (4)°

  • V = 2506.7 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 295 (2) K

  • 0.24 × 0.18 × 0.14 mm

Data collection

  • STOE IPDS 2 diffractometer

  • Absorption correction: integration (X-RED32; Stoe & Cie, 2002) T min = 0.981, T max = 0.989

  • 19631 measured reflections

  • 5191 independent reflections

  • 2442 reflections with I > 2σ(I)

  • R int = 0.067

Refinement

  • R[F 2 > 2σ(F 2)] = 0.051

  • wR(F 2) = 0.110

  • S = 0.90

  • 5191 reflections

  • 343 parameters

  • H-atom parameters constrained

  • Δρmax = 0.23 e Å−3

  • Δρmin = −0.13 e Å−3

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809004255/is2388sup1.cif

e-65-0o501-sup1.cif (30.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809004255/is2388Isup2.hkl

e-65-0o501-Isup2.hkl (249.1KB, 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
C2—H2⋯N1 0.93 2.28 2.964 (4) 130
C31—H31⋯O2 0.93 2.48 3.092 (3) 124
C3—H3⋯Cg1i 0.93 2.86 3.601 (3) 138
C11—H11⋯Cg2ii 0.93 2.63 3.543 (3) 166

Symmetry codes: (i) Inline graphic; (ii) Inline graphic. Cg1 and Cg2 are the centroids of the benzene ring (C8–C13) and phenyl ring (C30–C35), respectively.

Acknowledgments

The authors acknowledge the Faculty of Arts and Sciences, Ondokuz Mayıs University, Turkey, for the use of the Stoe IPDS 2 diffractometer (purchased under grant F.279 of the University Research Fund).

supplementary crystallographic information

Comment

The stereo selective synthesis of β-lactams has received considerable attention over recent years because of their wide variety of biological activities (Miller, 2000), in particular, asymmetric synthesis by means of a Staudinger ketene–imine reaction has been extensively studied (Palomo et al., 2004). Several syntheses of spiro-β-lactams are available in the literature (Jarrahpour & Khalili, 2007; Pınar et al., 2006; Akkurt, Jarrahpour et al., 2008; Akkurt, Karaca et al., 2008). The synthesis of polycyclic aromatic β-lactams from polyaromatic imines have been reported in literature (Banik et al., 2003).

The β-lactam unit in (I) (Fig. 1) is essentially planar, with a maximum deviation of 0.003 (3) Å from the mean plane. The β-lactam ring makes a dihedral angle of 17.4 (2)° with the phenyl ring C30—C35. In the xanthene ring system, attached at C16, the benzene rings (C17–C22) and (C23–C28) are almost planar, the dihedral angle between them 17.20 (14)°. Its central ring, C16/C17/C22/O1/C23/C28, is not planar, with puckering parameters: QT = 0.247 (3) Å, θ = 98.9 (7)° and φ = 355.1 (7)° (Cremer & Pople, 1975). The mean plane of the xanthene ring system forms the dihedral angles of 85.22 (17) and 85.62 (13)°, with the β-lactam ring and the phenyl ring, respectively. The anthracene ring system, attached at C15, is almost planar, with maximum deviations of 0.041 (2) Å for C1, -0.049 (3) Å for C4 and, -0.067 (2) Å for C13, makes dihedral angle of 65.39 (16), 80.60 (13) and 56.63 (8)°, with the β-lactam, the phenyl and the mean plane of the xanthene ring system, respectively.

In the crystal structure, there are intramolecular C—H···O and C—H···N contacts and molecules are linked to each other by C—H···π interactions between the adjacent molecules (Table 1 and Fig. 2) [Cg1 and Cg2 are the centroids of the benzene ring (C8–C13) and phenyl ring (C30–C35), respectively].

Experimental

A mixture of (E)—N-(antheracen-9-ylmethylene)aniline (0.30 g, 1.07 mmol) and triethylamine (0.73 g, 7.21 mmol), 9H-xanthen-9-carboxylic acid (0.49 g, 2.17 mmol) and tosyl chloride (0.42 g, 2.20 mmol) in CH2Cl2 (15 ml) was stirred at room temperature for 24 h. Then it was washed with HCl 1 N (20 ml) and saturated sodiumbicarbonate solution (20 ml), brine (20 ml), dried (Na2SO4) and the solvent was evaporated to give the crude product as a light yellow crystal which was then purified by recrystallization from ethyl acetate (Yield 63%). dec: 511–513 K. IR (KBr, cm-1): 1758 (CO β-lactam). 1H-NMR δ (p.p.m.): 6.34 (s, 1H, 4), 6.51–8.83 (m, ArH, 22H).13C-NMR δ (p.p.m.): 65.6 (C-3), 75.4 (C-4), 115.9–152.0 (aromatic carbon), 167.5 (CO β-lactam). Analysis calculated for C35H23NO2: C 85.87, H 4.74, N 2.86%. Found: C 85.87, H 4.74, N 2.86%.

Refinement

The H atoms were positioned geometrically and refined a riding model, with the C—H = 0.93 and 0.98 Å and with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The title molecular structure, with the atom-numbering scheme and 30% probability displacement ellipsoids

Fig. 2.

Fig. 2.

A view down the b axis of the packing of (I).

Crystal data

C35H23NO2 F(000) = 1024
Mr = 489.54 Dx = 1.297 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 12888 reflections
a = 13.6906 (8) Å θ = 1.5–28.1°
b = 13.3085 (7) Å µ = 0.08 mm1
c = 17.3527 (10) Å T = 295 K
β = 127.548 (4)° Block, colourless
V = 2506.7 (3) Å3 0.24 × 0.18 × 0.14 mm
Z = 4

Data collection

STOE IPDS 2 diffractometer 5191 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus 2442 reflections with I > 2σ(I)
plane graphite Rint = 0.067
Detector resolution: 6.67 pixels mm-1 θmax = 26.5°, θmin = 1.9°
ω scans h = −17→17
Absorption correction: integration (X-RED32; Stoe & Cie, 2002) k = −16→16
Tmin = 0.981, Tmax = 0.989 l = −21→21
19631 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)] = 0.051 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.110 H-atom parameters constrained
S = 0.90 w = 1/[σ2(Fo2) + (0.0406P)2] where P = (Fo2 + 2Fc2)/3
5191 reflections (Δ/σ)max < 0.001
343 parameters Δρmax = 0.23 e Å3
0 restraints Δρmin = −0.13 e Å3

Special details

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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 0.26666 (17) 0.35613 (13) 0.18443 (13) 0.0741 (7)
O2 0.23966 (18) 0.72931 (13) 0.19798 (13) 0.0792 (7)
N1 0.26629 (17) 0.67174 (14) 0.33789 (13) 0.0537 (7)
C1 0.0819 (2) 0.54484 (18) 0.34789 (15) 0.0537 (8)
C2 0.0287 (2) 0.6401 (2) 0.30421 (17) 0.0654 (9)
C3 −0.0826 (3) 0.6684 (2) 0.27919 (19) 0.0782 (11)
C4 −0.1483 (3) 0.6065 (3) 0.2989 (2) 0.0925 (13)
C5 −0.1006 (3) 0.5181 (3) 0.3433 (2) 0.0852 (11)
C6 0.0134 (2) 0.4829 (2) 0.36802 (18) 0.0630 (9)
C7 0.0576 (2) 0.3892 (2) 0.40911 (19) 0.0727 (11)
C8 0.1641 (2) 0.34938 (19) 0.42885 (16) 0.0587 (9)
C9 0.2069 (3) 0.2516 (2) 0.46931 (19) 0.0748 (11)
C10 0.3073 (3) 0.2113 (2) 0.4844 (2) 0.0771 (11)
C11 0.3703 (2) 0.2655 (2) 0.45823 (18) 0.0697 (10)
C12 0.3355 (2) 0.35957 (19) 0.42191 (16) 0.0577 (9)
C13 0.23202 (19) 0.40766 (18) 0.40696 (15) 0.0509 (8)
C14 0.19341 (19) 0.50727 (18) 0.37026 (14) 0.0495 (8)
C15 0.2778 (2) 0.56287 (16) 0.35636 (15) 0.0500 (8)
C16 0.2588 (2) 0.54946 (17) 0.25569 (15) 0.0521 (8)
C17 0.1450 (2) 0.49372 (19) 0.17648 (15) 0.0547 (8)
C18 0.0275 (2) 0.5320 (2) 0.13170 (17) 0.0684 (10)
C19 −0.0758 (2) 0.4769 (3) 0.06386 (19) 0.0788 (13)
C20 −0.0634 (3) 0.3830 (3) 0.03877 (19) 0.0809 (13)
C21 0.0515 (3) 0.3438 (2) 0.08025 (18) 0.0739 (11)
C22 0.1546 (2) 0.3999 (2) 0.14835 (17) 0.0590 (9)
C23 0.3694 (2) 0.4171 (2) 0.23285 (17) 0.0615 (9)
C24 0.4717 (3) 0.3782 (2) 0.24527 (19) 0.0751 (11)
C25 0.5788 (3) 0.4324 (3) 0.2946 (2) 0.0833 (13)
C26 0.5831 (3) 0.5262 (3) 0.3300 (2) 0.0841 (13)
C27 0.4806 (2) 0.5649 (2) 0.31657 (18) 0.0710 (10)
C28 0.3711 (2) 0.51099 (19) 0.26791 (16) 0.0556 (9)
C29 0.2507 (2) 0.66467 (19) 0.25206 (17) 0.0577 (9)
C30 0.3017 (2) 0.75205 (18) 0.40329 (16) 0.0544 (8)
C31 0.3090 (2) 0.8482 (2) 0.3781 (2) 0.0703 (10)
C32 0.3526 (3) 0.9250 (2) 0.4456 (2) 0.0847 (11)
C33 0.3860 (2) 0.9052 (2) 0.5366 (2) 0.0820 (11)
C34 0.3757 (2) 0.8104 (2) 0.56045 (19) 0.0736 (10)
C35 0.3336 (2) 0.7321 (2) 0.49401 (17) 0.0630 (9)
H2 0.07130 0.68380 0.29260 0.0780*
H3 −0.11600 0.72990 0.24850 0.0940*
H4 −0.22450 0.62690 0.28120 0.1110*
H5 −0.14300 0.47870 0.35840 0.1020*
H7 0.01420 0.35130 0.42410 0.0870*
H9 0.16430 0.21470 0.48570 0.0900*
H10 0.33450 0.14780 0.51200 0.0920*
H11 0.43750 0.23640 0.46600 0.0840*
H12 0.38030 0.39400 0.40620 0.0690*
H15 0.36340 0.54710 0.41060 0.0600*
H18 0.01840 0.59610 0.14790 0.0820*
H19 −0.15380 0.50350 0.03510 0.0950*
H20 −0.13320 0.34550 −0.00660 0.0970*
H21 0.05990 0.28020 0.06270 0.0890*
H24 0.46790 0.31520 0.22020 0.0900*
H25 0.64830 0.40610 0.30420 0.1000*
H26 0.65550 0.56350 0.36310 0.1010*
H27 0.48460 0.62850 0.34060 0.0850*
H31 0.28480 0.86160 0.31600 0.0840*
H32 0.35930 0.98990 0.42940 0.1020*
H33 0.41570 0.95670 0.58200 0.0980*
H34 0.39700 0.79780 0.62170 0.0880*
H35 0.32710 0.66740 0.51050 0.0760*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0753 (12) 0.0664 (12) 0.0832 (12) −0.0113 (10) 0.0496 (10) −0.0175 (10)
O2 0.1112 (14) 0.0678 (12) 0.0720 (11) −0.0093 (11) 0.0628 (11) 0.0030 (10)
N1 0.0632 (12) 0.0525 (13) 0.0528 (11) −0.0055 (10) 0.0392 (10) −0.0030 (9)
C1 0.0527 (13) 0.0623 (16) 0.0490 (13) −0.0030 (12) 0.0325 (11) −0.0062 (11)
C2 0.0601 (15) 0.0730 (19) 0.0648 (15) 0.0042 (14) 0.0390 (13) −0.0026 (14)
C3 0.0683 (18) 0.091 (2) 0.0712 (17) 0.0159 (16) 0.0404 (15) −0.0006 (15)
C4 0.0645 (18) 0.115 (3) 0.109 (2) 0.009 (2) 0.0585 (19) −0.008 (2)
C5 0.0673 (18) 0.097 (2) 0.114 (2) −0.0050 (17) 0.0669 (18) −0.009 (2)
C6 0.0554 (14) 0.0742 (19) 0.0702 (15) −0.0046 (13) 0.0438 (13) −0.0050 (14)
C7 0.0760 (18) 0.080 (2) 0.0831 (18) −0.0110 (16) 0.0593 (16) −0.0021 (16)
C8 0.0619 (15) 0.0625 (17) 0.0603 (15) −0.0054 (13) 0.0417 (13) −0.0004 (12)
C9 0.090 (2) 0.0675 (19) 0.0786 (18) −0.0088 (16) 0.0574 (17) 0.0034 (15)
C10 0.0818 (19) 0.0644 (18) 0.0797 (19) 0.0027 (16) 0.0465 (17) 0.0099 (14)
C11 0.0612 (16) 0.0695 (19) 0.0721 (17) 0.0044 (14) 0.0373 (14) 0.0034 (15)
C12 0.0494 (13) 0.0633 (17) 0.0566 (14) −0.0037 (12) 0.0303 (12) 0.0012 (12)
C13 0.0504 (13) 0.0579 (15) 0.0438 (12) −0.0076 (11) 0.0284 (11) −0.0050 (10)
C14 0.0453 (12) 0.0620 (16) 0.0435 (11) −0.0075 (11) 0.0283 (10) −0.0055 (11)
C15 0.0499 (12) 0.0560 (15) 0.0490 (12) −0.0044 (11) 0.0326 (11) −0.0024 (11)
C16 0.0563 (14) 0.0564 (15) 0.0499 (12) −0.0076 (12) 0.0356 (11) −0.0034 (11)
C17 0.0561 (14) 0.0660 (17) 0.0474 (12) −0.0059 (12) 0.0343 (12) −0.0012 (12)
C18 0.0636 (17) 0.0830 (19) 0.0585 (15) −0.0028 (15) 0.0371 (14) −0.0002 (14)
C19 0.0594 (17) 0.108 (3) 0.0619 (16) −0.0105 (17) 0.0333 (14) −0.0050 (16)
C20 0.0683 (19) 0.111 (3) 0.0595 (16) −0.0346 (19) 0.0369 (15) −0.0147 (17)
C21 0.087 (2) 0.079 (2) 0.0657 (17) −0.0253 (17) 0.0517 (16) −0.0161 (14)
C22 0.0625 (15) 0.0657 (18) 0.0586 (14) −0.0086 (14) 0.0420 (13) −0.0053 (13)
C23 0.0639 (16) 0.0690 (18) 0.0574 (14) −0.0034 (14) 0.0400 (13) −0.0035 (13)
C24 0.0736 (18) 0.089 (2) 0.0699 (17) 0.0089 (17) 0.0474 (16) −0.0057 (15)
C25 0.0657 (18) 0.121 (3) 0.0718 (18) 0.0061 (18) 0.0463 (16) −0.0052 (18)
C26 0.0598 (17) 0.125 (3) 0.0759 (18) −0.0160 (18) 0.0457 (15) −0.0142 (18)
C27 0.0675 (17) 0.089 (2) 0.0688 (16) −0.0162 (15) 0.0479 (14) −0.0145 (14)
C28 0.0586 (15) 0.0649 (17) 0.0520 (13) −0.0072 (13) 0.0382 (12) −0.0052 (12)
C29 0.0640 (15) 0.0623 (17) 0.0534 (14) −0.0100 (13) 0.0392 (12) −0.0027 (12)
C30 0.0539 (14) 0.0546 (16) 0.0584 (14) −0.0032 (12) 0.0361 (12) −0.0080 (12)
C31 0.0794 (18) 0.0630 (18) 0.0679 (16) −0.0004 (14) 0.0446 (15) −0.0034 (14)
C32 0.093 (2) 0.0632 (19) 0.095 (2) −0.0005 (16) 0.0558 (18) −0.0113 (17)
C33 0.0748 (19) 0.075 (2) 0.081 (2) −0.0019 (16) 0.0397 (17) −0.0241 (17)
C34 0.0698 (17) 0.081 (2) 0.0609 (16) 0.0058 (16) 0.0352 (14) −0.0108 (15)
C35 0.0648 (15) 0.0661 (17) 0.0597 (15) −0.0032 (13) 0.0387 (13) −0.0061 (13)

Geometric parameters (Å, °)

O1—C22 1.384 (4) C23—C28 1.384 (4)
O1—C23 1.379 (4) C24—C25 1.369 (5)
O2—C29 1.213 (3) C25—C26 1.377 (6)
N1—C15 1.472 (3) C26—C27 1.375 (6)
N1—C29 1.373 (3) C27—C28 1.390 (4)
N1—C30 1.412 (3) C30—C31 1.375 (4)
C1—C2 1.428 (4) C30—C35 1.379 (3)
C1—C6 1.442 (4) C31—C32 1.386 (4)
C1—C14 1.417 (4) C32—C33 1.376 (4)
C2—C3 1.359 (5) C33—C34 1.362 (4)
C3—C4 1.407 (6) C34—C35 1.392 (4)
C4—C5 1.338 (5) C2—H2 0.9300
C5—C6 1.422 (6) C3—H3 0.9300
C6—C7 1.380 (4) C4—H4 0.9300
C7—C8 1.384 (5) C5—H5 0.9300
C8—C9 1.424 (4) C7—H7 0.9300
C8—C13 1.429 (4) C9—H9 0.9300
C9—C10 1.344 (6) C10—H10 0.9300
C10—C11 1.396 (5) C11—H11 0.9300
C11—C12 1.351 (4) C12—H12 0.9300
C12—C13 1.427 (4) C15—H15 0.9800
C13—C14 1.426 (3) C18—H18 0.9300
C14—C15 1.510 (4) C19—H19 0.9300
C15—C16 1.612 (3) C20—H20 0.9300
C16—C17 1.502 (3) C21—H21 0.9300
C16—C28 1.508 (4) C24—H24 0.9300
C16—C29 1.536 (3) C25—H25 0.9300
C17—C18 1.388 (4) C26—H26 0.9300
C17—C22 1.376 (4) C27—H27 0.9300
C18—C19 1.376 (4) C31—H31 0.9300
C19—C20 1.368 (6) C32—H32 0.9300
C20—C21 1.373 (6) C33—H33 0.9300
C21—C22 1.383 (4) C34—H34 0.9300
C23—C24 1.381 (5) C35—H35 0.9300
O2···C27 3.410 (4) C29···H31 2.7700
O2···C31 3.092 (3) C29···H2 2.9500
O2···H31 2.4800 C30···H2 2.6600
O2···H25i 2.8200 C30···H11iv 2.8400
O2···H20ii 2.8700 C31···H11iv 3.0300
N1···C2 2.964 (4) C33···H19iii 2.9200
N1···H2 2.2800 C33···H11iv 3.0900
C1···C18 3.354 (3) C34···H20iii 2.8900
C2···C30 3.363 (4) C34···H11iv 2.9300
C2···N1 2.964 (4) C35···H15 3.0100
C2···C18 3.312 (4) C35···H11iv 2.8000
C3···C21iii 3.212 (4) H2···N1 2.2800
C4···C21iii 3.569 (5) H2···C15 2.8300
C11···C30iv 3.584 (4) H2···C29 2.9500
C12···C16 3.481 (3) H2···C30 2.6600
C13···C17 3.594 (3) H2···H18 2.4400
C14···C35 3.496 (3) H3···C21iii 2.9500
C14···C18 3.308 (3) H5···H7 2.4100
C16···C12 3.481 (3) H5···H25vii 2.5900
C17···C20ii 3.579 (4) H7···H5 2.4100
C17···C13 3.594 (3) H7···H9 2.4500
C18···C20ii 3.470 (5) H9···H7 2.4500
C18···C2 3.312 (4) H9···C21viii 2.9600
C18···C1 3.354 (3) H9···H21viii 2.4800
C18···C21ii 3.547 (4) H11···C30iv 2.8400
C18···C14 3.308 (3) H11···C31iv 3.0300
C19···C22ii 3.546 (4) H11···C33iv 3.0900
C20···C17ii 3.579 (4) H11···C34iv 2.9300
C20···C18ii 3.470 (5) H11···C35iv 2.8000
C21···C18ii 3.547 (4) H12···C15 2.5100
C21···C3v 3.212 (4) H12···C16 2.9300
C21···C4v 3.569 (5) H12···C23 2.9400
C22···C19ii 3.546 (4) H12···C28 2.8000
C27···O2 3.410 (4) H12···H15 2.0600
C30···C2 3.363 (4) H15···C12 2.5500
C30···C11iv 3.584 (4) H15···C27 2.9100
C31···O2 3.092 (3) H15···C35 3.0100
C35···C14 3.496 (3) H15···H12 2.0600
C1···H18 3.1000 H18···C1 3.1000
C2···H18 2.6900 H18···C2 2.6900
C3···H21iii 2.9700 H18···C29 2.6800
C4···H21iii 3.0100 H18···H2 2.4400
C12···H15 2.5500 H19···C33v 2.9200
C14···H35 2.9000 H20···C34v 2.8900
C15···H12 2.5100 H20···O2ii 2.8700
C15···H2 2.8300 H21···C3v 2.9700
C15···H35 2.7100 H21···C4v 3.0100
C16···H12 2.9300 H21···H9vi 2.4800
C21···H3v 2.9500 H25···H5ix 2.5900
C21···H9vi 2.9600 H25···O2x 2.8200
C23···H12 2.9400 H27···C29 2.6200
C24···H34iv 3.0000 H31···O2 2.4800
C25···H35iv 3.0900 H31···C29 2.7700
C27···H15 2.9100 H34···C24iv 3.0000
C28···H12 2.8000 H35···C14 2.9000
C29···H27 2.6200 H35···C15 2.7100
C29···H18 2.6800 H35···C25iv 3.0900
C22—O1—C23 117.8 (2) O2—C29—C16 135.4 (2)
C15—N1—C29 95.39 (18) N1—C29—C16 93.69 (19)
C15—N1—C30 129.15 (18) N1—C30—C31 120.3 (2)
C29—N1—C30 132.4 (2) N1—C30—C35 119.1 (2)
C2—C1—C6 116.1 (3) C31—C30—C35 120.5 (2)
C2—C1—C14 125.1 (3) C30—C31—C32 119.7 (3)
C6—C1—C14 118.9 (2) C31—C32—C33 120.0 (3)
C1—C2—C3 121.7 (3) C32—C33—C34 120.2 (3)
C2—C3—C4 121.2 (3) C33—C34—C35 120.6 (3)
C3—C4—C5 119.7 (4) C30—C35—C34 119.0 (2)
C4—C5—C6 121.6 (4) C1—C2—H2 119.00
C1—C6—C5 119.6 (3) C3—C2—H2 119.00
C1—C6—C7 119.8 (3) C2—C3—H3 119.00
C5—C6—C7 120.6 (3) C4—C3—H3 119.00
C6—C7—C8 122.6 (3) C3—C4—H4 120.00
C7—C8—C9 121.8 (3) C5—C4—H4 120.00
C7—C8—C13 119.0 (2) C4—C5—H5 119.00
C9—C8—C13 119.2 (3) C6—C5—H5 119.00
C8—C9—C10 121.7 (3) C6—C7—H7 119.00
C9—C10—C11 119.5 (3) C8—C7—H7 119.00
C10—C11—C12 121.2 (3) C8—C9—H9 119.00
C11—C12—C13 122.0 (3) C10—C9—H9 119.00
C8—C13—C12 116.3 (2) C9—C10—H10 120.00
C8—C13—C14 120.0 (3) C11—C10—H10 120.00
C12—C13—C14 123.7 (3) C10—C11—H11 119.00
C1—C14—C13 119.7 (3) C12—C11—H11 119.00
C1—C14—C15 125.8 (2) C11—C12—H12 119.00
C13—C14—C15 114.6 (2) C13—C12—H12 119.00
N1—C15—C14 121.8 (2) N1—C15—H15 109.00
N1—C15—C16 87.01 (16) C14—C15—H15 109.00
C14—C15—C16 119.02 (19) C16—C15—H15 109.00
C15—C16—C17 116.0 (2) C17—C18—H18 119.00
C15—C16—C28 114.08 (19) C19—C18—H18 119.00
C15—C16—C29 83.91 (17) C18—C19—H19 120.00
C17—C16—C28 111.2 (2) C20—C19—H19 120.00
C17—C16—C29 116.5 (2) C19—C20—H20 120.00
C28—C16—C29 112.8 (2) C21—C20—H20 120.00
C16—C17—C18 122.2 (2) C20—C21—H21 120.00
C16—C17—C22 120.2 (3) C22—C21—H21 120.00
C18—C17—C22 117.6 (2) C23—C24—H24 120.00
C17—C18—C19 121.3 (3) C25—C24—H24 120.00
C18—C19—C20 119.8 (3) C24—C25—H25 120.00
C19—C20—C21 120.4 (3) C26—C25—H25 120.00
C20—C21—C22 119.3 (3) C25—C26—H26 120.00
O1—C22—C17 122.8 (2) C27—C26—H26 120.00
O1—C22—C21 115.6 (3) C26—C27—H27 119.00
C17—C22—C21 121.6 (3) C28—C27—H27 119.00
O1—C23—C24 115.8 (2) C30—C31—H31 120.00
O1—C23—C28 122.5 (3) C32—C31—H31 120.00
C24—C23—C28 121.7 (3) C31—C32—H32 120.00
C23—C24—C25 119.9 (3) C33—C32—H32 120.00
C24—C25—C26 119.7 (4) C32—C33—H33 120.00
C25—C26—C27 120.2 (4) C34—C33—H33 120.00
C26—C27—C28 121.4 (3) C33—C34—H34 120.00
C16—C28—C23 120.2 (3) C35—C34—H34 120.00
C16—C28—C27 122.7 (2) C30—C35—H35 120.00
C23—C28—C27 117.1 (3) C34—C35—H35 121.00
O2—C29—N1 130.9 (2)
C23—O1—C22—C21 164.1 (2) N1—C15—C16—C29 0.4 (2)
C22—O1—C23—C24 −163.8 (2) C14—C15—C16—C17 8.8 (3)
C22—O1—C23—C28 16.9 (3) N1—C15—C16—C17 −116.2 (2)
C23—O1—C22—C17 −14.8 (4) N1—C15—C16—C28 112.6 (2)
C29—N1—C30—C31 10.4 (5) C14—C15—C16—C29 125.4 (2)
C29—N1—C30—C35 −167.0 (3) C14—C15—C16—C28 −122.3 (2)
C29—N1—C15—C16 −0.5 (2) C29—C16—C28—C27 29.6 (3)
C15—N1—C30—C35 −12.0 (5) C29—C16—C28—C23 −152.6 (2)
C30—N1—C15—C14 75.2 (4) C15—C16—C28—C27 −63.9 (3)
C15—N1—C29—C16 0.5 (2) C15—C16—C29—O2 177.0 (4)
C30—N1—C15—C16 −162.2 (3) C15—C16—C28—C23 113.9 (2)
C29—N1—C15—C14 −123.1 (2) C28—C16—C17—C18 −160.8 (2)
C30—N1—C29—C16 161.3 (3) C28—C16—C17—C22 21.6 (3)
C15—N1—C30—C31 165.4 (3) C29—C16—C17—C18 −29.7 (4)
C15—N1—C29—O2 −177.1 (4) C29—C16—C17—C22 152.7 (3)
C30—N1—C29—O2 −16.3 (6) C15—C16—C17—C18 66.7 (3)
C2—C1—C14—C13 −175.2 (2) C17—C16—C28—C23 −19.6 (3)
C2—C1—C6—C7 179.2 (2) C17—C16—C28—C27 162.6 (2)
C6—C1—C14—C15 −178.4 (2) C15—C16—C29—N1 −0.4 (2)
C14—C1—C6—C5 −178.1 (2) C15—C16—C17—C22 −110.9 (3)
C2—C1—C6—C5 0.6 (3) C28—C16—C29—N1 −114.0 (2)
C14—C1—C6—C7 0.5 (3) C28—C16—C29—O2 63.4 (4)
C14—C1—C2—C3 175.7 (2) C17—C16—C29—O2 −66.9 (5)
C6—C1—C14—C13 3.4 (3) C17—C16—C29—N1 115.7 (3)
C6—C1—C2—C3 −2.9 (3) C16—C17—C22—C21 175.7 (3)
C2—C1—C14—C15 3.1 (3) C22—C17—C18—C19 2.0 (4)
C1—C2—C3—C4 2.6 (4) C18—C17—C22—O1 176.8 (2)
C2—C3—C4—C5 0.2 (4) C16—C17—C18—C19 −175.6 (3)
C3—C4—C5—C6 −2.5 (5) C18—C17—C22—C21 −2.0 (4)
C4—C5—C6—C1 2.0 (4) C16—C17—C22—O1 −5.5 (4)
C4—C5—C6—C7 −176.6 (3) C17—C18—C19—C20 −0.8 (5)
C1—C6—C7—C8 −2.6 (4) C18—C19—C20—C21 −0.6 (5)
C5—C6—C7—C8 176.0 (3) C19—C20—C21—C22 0.6 (5)
C6—C7—C8—C13 0.7 (4) C20—C21—C22—C17 0.8 (5)
C6—C7—C8—C9 −178.6 (2) C20—C21—C22—O1 −178.2 (3)
C7—C8—C13—C14 3.3 (3) O1—C23—C24—C25 −178.4 (3)
C7—C8—C9—C10 177.0 (3) C28—C23—C24—C25 1.0 (4)
C13—C8—C9—C10 −2.3 (4) O1—C23—C28—C16 1.3 (4)
C9—C8—C13—C12 4.0 (3) C24—C23—C28—C16 −178.1 (2)
C7—C8—C13—C12 −175.3 (2) C24—C23—C28—C27 −0.1 (4)
C9—C8—C13—C14 −177.4 (2) O1—C23—C28—C27 179.2 (2)
C8—C9—C10—C11 −1.2 (4) C23—C24—C25—C26 −1.2 (5)
C9—C10—C11—C12 2.9 (4) C24—C25—C26—C27 0.5 (5)
C10—C11—C12—C13 −1.0 (4) C25—C26—C27—C28 0.3 (4)
C11—C12—C13—C8 −2.4 (3) C26—C27—C28—C16 177.4 (2)
C11—C12—C13—C14 179.0 (2) C26—C27—C28—C23 −0.6 (4)
C12—C13—C14—C15 −5.3 (3) N1—C30—C31—C32 −175.2 (3)
C8—C13—C14—C15 176.22 (19) C35—C30—C31—C32 2.1 (5)
C12—C13—C14—C1 173.2 (2) N1—C30—C35—C34 176.1 (3)
C8—C13—C14—C1 −5.4 (3) C31—C30—C35—C34 −1.3 (5)
C1—C14—C15—N1 14.0 (3) C30—C31—C32—C33 −1.3 (6)
C1—C14—C15—C16 −91.9 (3) C31—C32—C33—C34 −0.4 (6)
C13—C14—C15—C16 86.4 (2) C32—C33—C34—C35 1.2 (5)
C13—C14—C15—N1 −167.69 (18) C33—C34—C35—C30 −0.4 (5)

Symmetry codes: (i) −x+1, y+1/2, −z+1/2; (ii) −x, −y+1, −z; (iii) −x, y+1/2, −z+1/2; (iv) −x+1, −y+1, −z+1; (v) −x, y−1/2, −z+1/2; (vi) x, −y+1/2, z−1/2; (vii) x−1, y, z; (viii) x, −y+1/2, z+1/2; (ix) x+1, y, z; (x) −x+1, y−1/2, −z+1/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C2—H2···N1 0.93 2.28 2.964 (4) 130
C31—H31···O2 0.93 2.48 3.092 (3) 124
C3—H3···Cg1iii 0.93 2.86 3.601 (3) 138
C11—H11···Cg2iv 0.93 2.63 3.543 (3) 166

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS2388).

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/S1600536809004255/is2388sup1.cif

e-65-0o501-sup1.cif (30.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809004255/is2388Isup2.hkl

e-65-0o501-Isup2.hkl (249.1KB, hkl)

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


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