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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Dec 15;69(Pt 1):o100. doi: 10.1107/S1600536812050568

9-(4-Hy­droxy-3-meth­oxy­phen­yl)-3,3,6,6-tetra­methyl-1,2,3,4,5,6,7,8,9,10-deca­hydro­acridine-1,8-dione

Rajni Kant a,*, Vivek K Gupta a, Kamini Kapoor a, D R Patil b, P P Patil c, Madhukar B Deshmukh b
PMCID: PMC3588262  PMID: 23476363

Abstract

In the title mol­ecule, C24H29NO4, the central ring of the acridinedione system adopts a flat boat conformation and the four essentially planar atoms of this ring [maximum deviation = 0.001 (2) Å] form a dihedral angle of 85.99 (12)° with the benzene ring. The two outer rings of the acridinedione system adopt sofa conformations. In the crystal, O—H⋯O and N—H⋯O hydrogen bonds link the mol­ecules, forming a two-dimensional network parallel to (100).

Related literature  

For applications of acridines, see: Murugan et al. (1998); Josephrajan et al. (2005); Srividya et al. (1998,1996). For related structures, see: Balamurugan et al. (2009); Zhao & Teng (2008). For ring conformations, see: Duax & Norton (1975).graphic file with name e-69-0o100-scheme1.jpg

Experimental  

Crystal data  

  • C24H29NO4

  • M r = 395.48

  • Monoclinic, Inline graphic

  • a = 10.4828 (3) Å

  • b = 14.8973 (4) Å

  • c = 14.2059 (3) Å

  • β = 101.609 (2)°

  • V = 2173.09 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 K

  • 0.3 × 0.2 × 0.2 mm

Data collection  

  • Oxford Diffraction Xcalibur Sapphire3 diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.970, T max = 1.000

  • 63634 measured reflections

  • 4264 independent reflections

  • 2958 reflections with I > 2σ(I)

  • R int = 0.078

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.054

  • wR(F 2) = 0.116

  • S = 1.02

  • 4264 reflections

  • 267 parameters

  • H-atom parameters constrained

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 2010); 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: PLATON (Spek, 2009); software used to prepare material for publication: PLATON.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812050568/lh5567sup1.cif

e-69-0o100-sup1.cif (30.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050568/lh5567Isup2.hkl

e-69-0o100-Isup2.hkl (204.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812050568/lh5567Isup3.cml

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
O1—H1⋯O4i 0.82 2.12 2.800 (2) 141
N10—H10⋯O3ii 0.86 1.95 2.802 (2) 174

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

Acknowledgments

RK acknowledges the Department of Science & Technology for access to the single-crystal X-ray diffractometer sanctioned as a National Facility under project No. SR/S2/CMP-47/2003.

supplementary crystallographic information

Comment

Acridines, the earliest known antibiotics, are toxic towards bacteria. Some acridinedione derivatives show good inhibition against the pathogen Vibrio isolate-I (Josephrajan et al., 2005). Certain acridine-1,8-diones exhibit fluorescence activities (Murugan et al., 1998) and a few acridinedione derivatives also show photophysical (Srividya et al., 1998) and electrochemical properties (Srividya et al., 1996). Thus, the accurate description of crystal structures of substituted acridinediones are expected to provide useful information on the role of substituents in influencing molecular conformation which has a direct relationship to biological activity. This paper deals with the crystal structure of a 4-hydroxy-3-methoxyphenyl substituted tetramethyl acridinedione, (I).

In (I) (Fig.1), all bond lengths and angles are normal and correspond to those observed in related structures (Balamurugan et al.,2009; Zhao & Teng 2008). The central ring (C4A/C5A/C8A/C9A/C9/N10) of the acridinedione moiety adopts a boat conformation (ΔCs(N10) = 0.129 & ΔCs (C5A—C8A) = 10.84) and the four essentially planar atoms (C4A/C5A/C8A/C9A) of this ring (maximum deviation 0.001 (2)Å for all atoms) forms a dihedral angle of 85.99 (12)° with benzene ring. Both the outer rings adopt sofa conformations (ΔCs (C6) = 1.55; ΔCs (C3) = 7.45) (Duax & Norton, 1975). In the crystal, O1—H1···O4i and N10—H10···O3ii hydrogen bonds (Table 1) link molecules to form a two-dimensional network parallel to (100) (Fig. 2).

Experimental

In a 50 ml rounded bottom flask, a mixture of dimedone (2 mmole), 4-hydroxy, 3-methoxy benzaldehyde (1 mmole) and ammonium acetate (1.2 mmole) in mixture of aqueous ethanol (7 ml) was stirred at RT for 5 min. To this mixture 3-carboxymethyl-1-methylimidazolium(HSO4) (20 mol%) was added and the reaction mixture heated at 348-353K for 1.5 hrs. The progress of reaction was monitored by TLC. After completion of reaction, the mixture was cooled to RT and poured on iced water under stirring, The precipitate was filter and dried. The crude product were recrystallized from ethanol to afford X-ray quality crystals. M.P.: 568–571 K, Yield: 82%. IR(KBr): 3274,3168,3049,1623,1511,1370 cm-1. 1H NMR(300 MHz, DMSO-d6): δ = 8.7(s,1H,OH);7.7 (s, 1H, NH); 6.7 (s, 1H, Ar—H); 6.5(s,2H,Ar—H); 4.7 (s, 1H, CH); 3.67 (s, 3H, OCH3); 2.4–2.0 (m, 8H, CH2); 1.0 (s, 6H, CH3); 0.9 (s,6H, CH3).

Refinement

All H atoms were positioned geometrically and were treated as riding on their parent C atoms, with C—H distances of 0.93–0.96 Å and with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound with ellipsoids drawn at the 40% probability level. H atoms are shown as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

The packing arrangement of molecules viewed along the a axis. The dashed lines show intermolecular O—H···O and N—H···O hydrogen bonds.

Crystal data

C24H29NO4 F(000) = 848
Mr = 395.48 Dx = 1.209 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 22356 reflections
a = 10.4828 (3) Å θ = 3.5–29.2°
b = 14.8973 (4) Å µ = 0.08 mm1
c = 14.2059 (3) Å T = 293 K
β = 101.609 (2)° Block, yellow
V = 2173.09 (10) Å3 0.3 × 0.2 × 0.2 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur Sapphire3 diffractometer 4264 independent reflections
Radiation source: fine-focus sealed tube 2958 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.078
Detector resolution: 16.1049 pixels mm-1 θmax = 26.0°, θmin = 3.5°
ω scans h = −12→12
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) k = −18→18
Tmin = 0.970, Tmax = 1.000 l = −17→17
63634 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)] = 0.054 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.116 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0342P)2 + 1.3025P] where P = (Fo2 + 2Fc2)/3
4264 reflections (Δ/σ)max = 0.001
267 parameters Δρmax = 0.19 e Å3
0 restraints Δρmin = −0.17 e Å3

Special details

Experimental. CrysAlis PRO, Oxford Diffraction Ltd., Version 1.171.34.40 (release 27–08-2010 CrysAlis171. NET) (compiled Aug 27 2010,11:50:40) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
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
O1 0.36588 (15) 0.71186 (11) 0.15883 (12) 0.0579 (5)
H1 0.3497 0.6666 0.1872 0.087*
O2 0.50253 (16) 0.63379 (12) 0.31829 (13) 0.0679 (6)
O3 0.98444 (15) 0.78678 (10) 0.20508 (10) 0.0449 (4)
O4 0.74288 (15) 1.04026 (10) 0.34010 (10) 0.0474 (4)
C1 1.01925 (19) 0.76067 (13) 0.28878 (14) 0.0324 (5)
C2 1.1273 (2) 0.69369 (16) 0.31500 (15) 0.0443 (6)
H2A 1.2095 0.7257 0.3296 0.053*
H2B 1.1287 0.6558 0.2597 0.053*
C3 1.1169 (2) 0.63400 (15) 0.40043 (15) 0.0414 (5)
C4 1.0993 (2) 0.69384 (14) 0.48413 (14) 0.0365 (5)
H4A 1.0735 0.6569 0.5333 0.044*
H4B 1.1821 0.7215 0.5118 0.044*
C4A 0.99980 (18) 0.76586 (13) 0.45531 (13) 0.0282 (4)
C5 0.86618 (19) 0.92717 (14) 0.60844 (13) 0.0340 (5)
H5A 0.9431 0.9626 0.6337 0.041*
H5B 0.8581 0.8815 0.6556 0.041*
C5A 0.88328 (18) 0.88242 (13) 0.51737 (13) 0.0281 (4)
C6 0.74670 (19) 0.98788 (14) 0.59372 (15) 0.0364 (5)
C7 0.7532 (2) 1.04984 (13) 0.50920 (14) 0.0354 (5)
H7A 0.6723 1.0833 0.4935 0.043*
H7B 0.8229 1.0928 0.5294 0.043*
C8 0.77544 (18) 1.00365 (13) 0.41909 (14) 0.0312 (5)
C8A 0.83906 (18) 0.91691 (13) 0.42877 (13) 0.0277 (4)
C9 0.85163 (18) 0.86508 (12) 0.33895 (12) 0.0279 (4)
H9 0.8768 0.9076 0.2933 0.033*
C9A 0.95946 (18) 0.79613 (13) 0.36429 (13) 0.0276 (4)
N10 0.95340 (15) 0.80412 (11) 0.52928 (11) 0.0325 (4)
H10 0.9686 0.7784 0.5846 0.039*
C11 1.0003 (3) 0.57076 (16) 0.37230 (17) 0.0570 (7)
H11A 0.9227 0.6054 0.3505 0.085*
H11B 0.9906 0.5356 0.4271 0.085*
H11C 1.0144 0.5316 0.3217 0.085*
C12 1.2408 (3) 0.5783 (2) 0.43053 (19) 0.0732 (9)
H12A 1.2543 0.5424 0.3772 0.110*
H12B 1.2321 0.5399 0.4831 0.110*
H12C 1.3138 0.6176 0.4502 0.110*
C13 0.6240 (2) 0.92964 (19) 0.57391 (19) 0.0600 (7)
H13A 0.5489 0.9666 0.5736 0.090*
H13B 0.6297 0.8848 0.6231 0.090*
H13C 0.6163 0.9009 0.5125 0.090*
C14 0.7475 (3) 1.04393 (17) 0.68425 (17) 0.0587 (7)
H14A 0.8277 1.0769 0.7002 0.088*
H14B 0.7398 1.0049 0.7366 0.088*
H14C 0.6756 1.0851 0.6727 0.088*
C15 0.72117 (19) 0.82284 (13) 0.29120 (13) 0.0311 (5)
C16 0.6463 (2) 0.85976 (16) 0.21025 (17) 0.0591 (8)
H16 0.6756 0.9107 0.1832 0.071*
C17 0.5277 (3) 0.82234 (17) 0.16818 (18) 0.0640 (8)
H17 0.4781 0.8491 0.1138 0.077*
C18 0.4818 (2) 0.74704 (14) 0.20478 (15) 0.0393 (5)
C19 0.5562 (2) 0.70943 (14) 0.28684 (15) 0.0370 (5)
C20 0.67392 (19) 0.74706 (14) 0.32934 (14) 0.0362 (5)
H20 0.7225 0.7211 0.3846 0.043*
C21 0.5784 (3) 0.58366 (18) 0.3926 (2) 0.0686 (8)
H21A 0.6595 0.5680 0.3752 0.103*
H21B 0.5326 0.5299 0.4029 0.103*
H21C 0.5952 0.6187 0.4505 0.103*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0465 (10) 0.0494 (10) 0.0643 (11) −0.0135 (8) −0.0210 (8) 0.0109 (8)
O2 0.0477 (10) 0.0733 (12) 0.0732 (12) −0.0243 (9) −0.0107 (9) 0.0376 (10)
O3 0.0643 (10) 0.0500 (9) 0.0211 (8) −0.0007 (8) 0.0103 (7) −0.0018 (7)
O4 0.0625 (10) 0.0403 (9) 0.0365 (9) 0.0105 (8) 0.0028 (7) 0.0104 (7)
C1 0.0378 (11) 0.0354 (11) 0.0240 (10) −0.0080 (9) 0.0061 (8) −0.0028 (9)
C2 0.0458 (13) 0.0560 (14) 0.0338 (12) 0.0059 (11) 0.0144 (10) −0.0080 (11)
C3 0.0459 (13) 0.0448 (13) 0.0310 (11) 0.0142 (11) 0.0019 (9) −0.0036 (10)
C4 0.0364 (11) 0.0445 (12) 0.0262 (11) 0.0079 (10) 0.0002 (8) −0.0001 (9)
C4A 0.0280 (10) 0.0327 (11) 0.0233 (10) −0.0011 (8) 0.0040 (8) −0.0022 (8)
C5 0.0342 (11) 0.0421 (12) 0.0245 (10) 0.0040 (9) 0.0032 (8) −0.0001 (9)
C5A 0.0272 (10) 0.0317 (10) 0.0250 (10) −0.0007 (8) 0.0043 (8) 0.0000 (8)
C6 0.0327 (11) 0.0422 (12) 0.0352 (11) 0.0048 (10) 0.0091 (9) 0.0032 (9)
C7 0.0324 (11) 0.0332 (11) 0.0404 (12) 0.0022 (9) 0.0069 (9) 0.0003 (9)
C8 0.0262 (10) 0.0319 (11) 0.0333 (11) −0.0045 (9) 0.0005 (8) 0.0041 (9)
C8A 0.0271 (10) 0.0298 (10) 0.0250 (10) −0.0025 (8) 0.0026 (8) 0.0015 (8)
C9 0.0328 (10) 0.0291 (10) 0.0203 (9) −0.0022 (8) 0.0020 (8) 0.0047 (8)
C9A 0.0291 (10) 0.0313 (10) 0.0215 (9) −0.0037 (8) 0.0027 (7) −0.0014 (8)
N10 0.0404 (10) 0.0383 (10) 0.0185 (8) 0.0082 (8) 0.0057 (7) 0.0056 (7)
C11 0.0828 (19) 0.0430 (14) 0.0410 (14) −0.0041 (13) 0.0027 (13) −0.0003 (11)
C12 0.080 (2) 0.083 (2) 0.0525 (16) 0.0469 (17) 0.0048 (14) −0.0075 (15)
C13 0.0364 (13) 0.0738 (18) 0.0707 (18) −0.0037 (13) 0.0128 (12) 0.0242 (14)
C14 0.0721 (18) 0.0621 (16) 0.0480 (15) 0.0236 (14) 0.0269 (13) 0.0006 (12)
C15 0.0354 (11) 0.0303 (11) 0.0244 (10) −0.0007 (9) −0.0016 (8) −0.0002 (8)
C16 0.0675 (17) 0.0463 (14) 0.0490 (15) −0.0251 (13) −0.0232 (12) 0.0232 (11)
C17 0.0661 (17) 0.0524 (15) 0.0542 (16) −0.0174 (13) −0.0341 (13) 0.0244 (13)
C18 0.0362 (12) 0.0345 (11) 0.0408 (12) −0.0028 (10) −0.0072 (9) −0.0011 (10)
C19 0.0345 (11) 0.0377 (12) 0.0375 (12) −0.0035 (9) 0.0039 (9) 0.0061 (9)
C20 0.0352 (11) 0.0430 (12) 0.0274 (11) −0.0003 (10) −0.0008 (8) 0.0114 (9)
C21 0.0579 (17) 0.0636 (18) 0.083 (2) −0.0048 (14) 0.0111 (14) 0.0390 (16)

Geometric parameters (Å, º)

O1—C18 1.364 (2) C8—C8A 1.448 (3)
O1—H1 0.8200 C8A—C9 1.520 (3)
O2—C19 1.374 (2) C9—C9A 1.516 (3)
O2—C21 1.403 (3) C9—C15 1.534 (3)
O3—C1 1.234 (2) C9—H9 0.9800
O4—C8 1.232 (2) N10—H10 0.8600
C1—C9A 1.447 (3) C11—H11A 0.9600
C1—C2 1.499 (3) C11—H11B 0.9600
C2—C3 1.526 (3) C11—H11C 0.9600
C2—H2A 0.9700 C12—H12A 0.9600
C2—H2B 0.9700 C12—H12B 0.9600
C3—C4 1.527 (3) C12—H12C 0.9600
C3—C12 1.528 (3) C13—H13A 0.9600
C3—C11 1.532 (3) C13—H13B 0.9600
C4—C4A 1.495 (3) C13—H13C 0.9600
C4—H4A 0.9700 C14—H14A 0.9600
C4—H4B 0.9700 C14—H14B 0.9600
C4A—C9A 1.354 (2) C14—H14C 0.9600
C4A—N10 1.368 (2) C15—C16 1.370 (3)
C5—C5A 1.498 (3) C15—C20 1.386 (3)
C5—C6 1.525 (3) C16—C17 1.384 (3)
C5—H5A 0.9700 C16—H16 0.9300
C5—H5B 0.9700 C17—C18 1.364 (3)
C5A—C8A 1.352 (2) C17—H17 0.9300
C5A—N10 1.371 (2) C18—C19 1.384 (3)
C6—C7 1.527 (3) C19—C20 1.379 (3)
C6—C13 1.530 (3) C20—H20 0.9300
C6—C14 1.532 (3) C21—H21A 0.9600
C7—C8 1.512 (3) C21—H21B 0.9600
C7—H7A 0.9700 C21—H21C 0.9600
C7—H7B 0.9700
C18—O1—H1 109.5 C8A—C9—H9 107.9
C19—O2—C21 118.32 (18) C15—C9—H9 107.9
O3—C1—C9A 120.73 (19) C4A—C9A—C1 119.19 (18)
O3—C1—C2 120.74 (18) C4A—C9A—C9 121.81 (17)
C9A—C1—C2 118.50 (17) C1—C9A—C9 119.00 (16)
C1—C2—C3 114.46 (18) C4A—N10—C5A 121.63 (16)
C1—C2—H2A 108.6 C4A—N10—H10 119.2
C3—C2—H2A 108.6 C5A—N10—H10 119.2
C1—C2—H2B 108.6 C3—C11—H11A 109.5
C3—C2—H2B 108.6 C3—C11—H11B 109.5
H2A—C2—H2B 107.6 H11A—C11—H11B 109.5
C2—C3—C4 108.56 (18) C3—C11—H11C 109.5
C2—C3—C12 110.3 (2) H11A—C11—H11C 109.5
C4—C3—C12 109.17 (17) H11B—C11—H11C 109.5
C2—C3—C11 109.39 (18) C3—C12—H12A 109.5
C4—C3—C11 110.29 (19) C3—C12—H12B 109.5
C12—C3—C11 109.1 (2) H12A—C12—H12B 109.5
C4A—C4—C3 113.14 (16) C3—C12—H12C 109.5
C4A—C4—H4A 109.0 H12A—C12—H12C 109.5
C3—C4—H4A 109.0 H12B—C12—H12C 109.5
C4A—C4—H4B 109.0 C6—C13—H13A 109.5
C3—C4—H4B 109.0 C6—C13—H13B 109.5
H4A—C4—H4B 107.8 H13A—C13—H13B 109.5
C9A—C4A—N10 120.24 (17) C6—C13—H13C 109.5
C9A—C4A—C4 124.55 (17) H13A—C13—H13C 109.5
N10—C4A—C4 115.15 (16) H13B—C13—H13C 109.5
C5A—C5—C6 112.54 (16) C6—C14—H14A 109.5
C5A—C5—H5A 109.1 C6—C14—H14B 109.5
C6—C5—H5A 109.1 H14A—C14—H14B 109.5
C5A—C5—H5B 109.1 C6—C14—H14C 109.5
C6—C5—H5B 109.1 H14A—C14—H14C 109.5
H5A—C5—H5B 107.8 H14B—C14—H14C 109.5
C8A—C5A—N10 120.88 (17) C16—C15—C20 117.74 (19)
C8A—C5A—C5 123.82 (18) C16—C15—C9 121.04 (18)
N10—C5A—C5 115.24 (16) C20—C15—C9 121.21 (16)
C5—C6—C7 107.52 (16) C15—C16—C17 120.9 (2)
C5—C6—C13 109.03 (18) C15—C16—H16 119.5
C7—C6—C13 111.54 (18) C17—C16—H16 119.5
C5—C6—C14 110.03 (17) C18—C17—C16 121.4 (2)
C7—C6—C14 109.70 (18) C18—C17—H17 119.3
C13—C6—C14 109.01 (19) C16—C17—H17 119.3
C8—C7—C6 115.43 (17) O1—C18—C17 118.83 (19)
C8—C7—H7A 108.4 O1—C18—C19 122.98 (19)
C6—C7—H7A 108.4 C17—C18—C19 118.19 (19)
C8—C7—H7B 108.4 O2—C19—C20 125.45 (18)
C6—C7—H7B 108.4 O2—C19—C18 114.10 (18)
H7A—C7—H7B 107.5 C20—C19—C18 120.45 (19)
O4—C8—C8A 121.28 (18) C19—C20—C15 121.24 (18)
O4—C8—C7 120.51 (18) C19—C20—H20 119.4
C8A—C8—C7 118.18 (17) C15—C20—H20 119.4
C5A—C8A—C8 119.51 (18) O2—C21—H21A 109.5
C5A—C8A—C9 121.13 (17) O2—C21—H21B 109.5
C8—C8A—C9 119.33 (16) H21A—C21—H21B 109.5
C9A—C9—C8A 109.35 (14) O2—C21—H21C 109.5
C9A—C9—C15 112.51 (15) H21A—C21—H21C 109.5
C8A—C9—C15 111.07 (15) H21B—C21—H21C 109.5
C9A—C9—H9 107.9
O3—C1—C2—C3 −150.88 (19) N10—C4A—C9A—C9 −7.0 (3)
C9A—C1—C2—C3 31.0 (3) C4—C4A—C9A—C9 175.87 (18)
C1—C2—C3—C4 −52.0 (2) O3—C1—C9A—C4A 179.86 (19)
C1—C2—C3—C12 −171.60 (19) C2—C1—C9A—C4A −2.1 (3)
C1—C2—C3—C11 68.3 (2) O3—C1—C9A—C9 0.9 (3)
C2—C3—C4—C4A 46.2 (2) C2—C1—C9A—C9 178.97 (17)
C12—C3—C4—C4A 166.4 (2) C8A—C9—C9A—C4A 21.9 (2)
C11—C3—C4—C4A −73.7 (2) C15—C9—C9A—C4A −102.0 (2)
C3—C4—C4A—C9A −20.7 (3) C8A—C9—C9A—C1 −159.14 (16)
C3—C4—C4A—N10 162.08 (18) C15—C9—C9A—C1 76.9 (2)
C6—C5—C5A—C8A 26.8 (3) C9A—C4A—N10—C5A −11.1 (3)
C6—C5—C5A—N10 −156.02 (17) C4—C4A—N10—C5A 166.29 (17)
C5A—C5—C6—C7 −50.7 (2) C8A—C5A—N10—C4A 11.0 (3)
C5A—C5—C6—C13 70.3 (2) C5—C5A—N10—C4A −166.26 (17)
C5A—C5—C6—C14 −170.15 (18) C9A—C9—C15—C16 −133.8 (2)
C5—C6—C7—C8 50.7 (2) C8A—C9—C15—C16 103.3 (2)
C13—C6—C7—C8 −68.8 (2) C9A—C9—C15—C20 47.4 (2)
C14—C6—C7—C8 170.34 (18) C8A—C9—C15—C20 −75.6 (2)
C6—C7—C8—O4 157.24 (18) C20—C15—C16—C17 −0.1 (4)
C6—C7—C8—C8A −24.5 (2) C9—C15—C16—C17 −179.0 (2)
N10—C5A—C8A—C8 −174.53 (17) C15—C16—C17—C18 −0.9 (5)
C5—C5A—C8A—C8 2.5 (3) C16—C17—C18—O1 −178.3 (3)
N10—C5A—C8A—C9 7.2 (3) C16—C17—C18—C19 1.2 (4)
C5—C5A—C8A—C9 −175.83 (17) C21—O2—C19—C20 −8.0 (4)
O4—C8—C8A—C5A 174.37 (19) C21—O2—C19—C18 171.2 (2)
C7—C8—C8A—C5A −3.9 (3) O1—C18—C19—O2 −0.3 (3)
O4—C8—C8A—C9 −7.3 (3) C17—C18—C19—O2 −179.9 (2)
C7—C8—C8A—C9 174.46 (17) O1—C18—C19—C20 178.8 (2)
C5A—C8A—C9—C9A −21.9 (2) C17—C18—C19—C20 −0.7 (4)
C8—C8A—C9—C9A 159.82 (16) O2—C19—C20—C15 178.8 (2)
C5A—C8A—C9—C15 102.9 (2) C18—C19—C20—C15 −0.3 (3)
C8—C8A—C9—C15 −75.4 (2) C16—C15—C20—C19 0.6 (3)
N10—C4A—C9A—C1 174.02 (17) C9—C15—C20—C19 179.51 (19)
C4—C4A—C9A—C1 −3.1 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O1—H1···O4i 0.82 2.12 2.800 (2) 141
N10—H10···O3ii 0.86 1.95 2.802 (2) 174

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5567).

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 datablock(s) I, global. DOI: 10.1107/S1600536812050568/lh5567sup1.cif

e-69-0o100-sup1.cif (30.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050568/lh5567Isup2.hkl

e-69-0o100-Isup2.hkl (204.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812050568/lh5567Isup3.cml

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


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