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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jul 31;64(Pt 8):o1627. doi: 10.1107/S1600536808023271

2,2′-Bis(9-hydr­oxy-9-fluoren­yl)biphen­yl–ethyl acetate (1/1)

Lidiya Izotova a,*, Jamshid Ashurov a, Bakhtiyar Ibragimov a, Edwin Weber b
PMCID: PMC2962236  PMID: 21203317

Abstract

In the title host–guest compound, C38H26O2·C4H8O2, the ethyl acetate mol­ecule (guest), which adopts a fully extended conformation, and the biphenyl derivative (host) are connected via O—H⋯O hydrogen bonds [H⋯O = 1.90 (3) Å] into discrete assemblies. The hydro­carbon skeleton of the host mol­ecule deviates only slightly from C2 symmetry. The OH groups of the host are involved in intra­molecular O—H⋯O hydrogen bonding [H⋯O = 1.83 (3) Å].

Related literature

For related literature, see: Barbour et al. (1993); Ibragimov et al. (2001); Sardone (1996); Sumarna et al. (2003); Weber et al. (1993).graphic file with name e-64-o1627-scheme1.jpg

Experimental

Crystal data

  • C38H26O2·C4H8O2

  • M r = 602.69

  • Monoclinic, Inline graphic

  • a = 11.645 (2) Å

  • b = 16.364 (3) Å

  • c = 17.471 (3) Å

  • β = 97.72 (3)°

  • V = 3299.1 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 (2) K

  • 0.4 × 0.2 × 0.2 mm

Data collection

  • Stoe STADI4 diffractometer

  • Absorption correction: none

  • 5807 measured reflections

  • 5650 independent reflections

  • 3654 reflections with I > 2σ(I)

  • 3 standard reflections every 100 reflections intensity decay: 2.6%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.068

  • wR(F 2) = 0.141

  • S = 1.20

  • 5650 reflections

  • 424 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.24 e Å−3

  • Δρmin = −0.16 e Å−3

Data collection: STADI4 (Stoe & Cie, 1997); cell refinement: STADI4; data reduction: X-RED (Stoe & Cie, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP (Siemens, 1994); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808023271/gk2155sup1.cif

e-64-o1627-sup1.cif (24.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023271/gk2155Isup2.hkl

e-64-o1627-Isup2.hkl (276.6KB, 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
O2—H1⋯O3i 0.88 (4) 1.90 (4) 2.779 (3) 173 (4)
O1—H2⋯O2 0.93 (4) 1.84 (4) 2.739 (3) 161 (3)

Symmetry code: (i) Inline graphic.

supplementary crystallographic information

Comment

Crystalline inclusion compounds (clathrates, host–guest complexes) are of increasing importance in supramolecular chemistry because of their significant potential in addressing a variety of fundamental and practical issues. 2,2'-Bis(9-hydroxy-9-fluorenyl)biphenyl (I) is a host compound with good clathrate-forming ability and the crystal structures of its inclusion compounds with acetonitrile, cyclohexanone, n-propylamine (Barbour et al., 1993), acetone (three solvates) (Sardone, 1996; Ibragimov et al., 2001) and chloroform (two solvates) (Sumarna et al., 2003) were reported. Here, we report the crystal structure of a host–guest complex of (I) with ethyl acetate which resembles closely that of (I) with acetone (1/1) (Sardone, 1996). The molecule of (I) has three conformational degrees of freedom (rotation around the central aryl–aryl single bond and rotations around the aryl–fluorenyl bonds), however it exhibits considerable conformational rigidity due to the stabilizing effect of the intramolecular O—H···O hydrogen bond between the hydroxyl groups (Fig. 1, Table 1). The crystal packing is mainly stabilized by van der Waals forces (Fig.2).

Experimental

2,2'-Bis(9-hydroxy-9-fluorenyl)biphenyl was synthesized according to the procedure described by Weber et al., (1993). The stable in the air crystals were grown by slow evaporation from ethyl acetate solution.

Refinement

H atoms from the OH groups were located from difference Fourier maps and fully refined. The remaining H atoms were positioned geometrically (C—H 0.93–0.98 Å) and refined as riding on their carrier atoms with Uiso(H) = 1.2Ueq(C), except the methyl groups where Uiso(H) = 1.5Ueq(C).

Figures

Fig. 1.

Fig. 1.

Perspective view of the title compound, showing 30% probability displacement ellipsoids for the non-H atoms. Dashed lines represent hydrogen bonds.

Fig. 2.

Fig. 2.

Packing diagram of the title compound (I) viewed down the a axis. H atoms have been ommited for clarity. Hydrogen bonds are shown as dashed lines.

Crystal data

C38H26O2·C4H8O2 F000 = 1272
Mr = 602.69 Dx = 1.213 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 25 reflections
a = 11.645 (2) Å θ = 10–20º
b = 16.364 (3) Å µ = 0.08 mm1
c = 17.471 (3) Å T = 293 (2) K
β = 97.72 (3)º Block, colourless
V = 3299.1 (10) Å3 0.4 × 0.2 × 0.2 mm
Z = 4

Data collection

Stoe STADI4 diffractometer Rint = 0.0000
Radiation source: fine-focus sealed tube θmax = 25.0º
Monochromator: graphite θmin = 2.6º
T = 293(2) K h = −13→11
ω/2θ scans k = 0→19
Absorption correction: none l = 0→20
5650 measured reflections 3 standard reflections
5807 independent reflections every 100 reflections
3654 reflections with I > 2σ(I) intensity decay: 2.6%

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.068   w = 1/[σ2(Fo2) + (0.0281P)2 + 2.047P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.141 (Δ/σ)max < 0.001
S = 1.20 Δρmax = 0.24 e Å3
5650 reflections Δρmin = −0.16 e Å3
424 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0048 (4)
Secondary atom site location: difference Fourier map

Special details

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 0.70308 (18) 0.69051 (14) 0.20949 (13) 0.0518 (6)
O2 0.63649 (17) 0.85042 (13) 0.21819 (12) 0.0470 (5)
C1 0.8676 (3) 0.62161 (19) 0.1739 (2) 0.0511 (8)
C2 0.8325 (3) 0.5837 (2) 0.1044 (2) 0.0716 (11)
H2A 0.7765 0.6073 0.0681 0.086*
C3 0.8827 (4) 0.5090 (3) 0.0897 (3) 0.0937 (14)
H3A 0.8596 0.4822 0.0432 0.112*
C4 0.9657 (5) 0.4747 (3) 0.1430 (4) 0.0995 (17)
H4A 0.9982 0.4248 0.1321 0.119*
C5 1.0019 (3) 0.5126 (3) 0.2122 (3) 0.0828 (13)
H5A 1.0588 0.4889 0.2478 0.099*
C6 0.9523 (3) 0.5867 (2) 0.2280 (2) 0.0616 (10)
C7 0.9683 (3) 0.6387 (2) 0.2964 (2) 0.0633 (10)
C8 1.0404 (4) 0.6306 (3) 0.3666 (3) 0.0891 (14)
H8A 1.0925 0.5874 0.3749 0.107*
C9 1.0330 (5) 0.6877 (4) 0.4232 (3) 0.1026 (18)
H9A 1.0814 0.6831 0.4698 0.123*
C10 0.9559 (4) 0.7516 (3) 0.4126 (2) 0.0903 (14)
H10A 0.9510 0.7885 0.4526 0.108*
C11 0.8848 (3) 0.7614 (2) 0.3424 (2) 0.0701 (10)
H11A 0.8334 0.8050 0.3343 0.084*
C12 0.8930 (3) 0.7041 (2) 0.28501 (19) 0.0545 (9)
C13 0.8229 (3) 0.70131 (18) 0.20394 (17) 0.0460 (7)
C14 0.8464 (3) 0.77519 (18) 0.15426 (17) 0.0434 (7)
C15 0.9585 (3) 0.8074 (2) 0.16490 (18) 0.0527 (8)
H15A 1.0139 0.7835 0.2013 0.063*
C16 0.9899 (3) 0.8735 (2) 0.1234 (2) 0.0592 (9)
H16A 1.0655 0.8931 0.1315 0.071*
C17 0.9087 (3) 0.9100 (2) 0.07009 (19) 0.0597 (9)
H17A 0.9284 0.9551 0.0422 0.072*
C18 0.7978 (3) 0.87899 (19) 0.05842 (18) 0.0524 (8)
H18A 0.7434 0.9038 0.0219 0.063*
C19 0.7638 (3) 0.81209 (18) 0.09903 (16) 0.0433 (7)
C20 0.6441 (3) 0.77988 (17) 0.06964 (16) 0.0423 (7)
C21 0.6384 (3) 0.73514 (19) 0.00138 (17) 0.0523 (8)
H21A 0.7072 0.7234 −0.0180 0.063*
C22 0.5355 (3) 0.7074 (2) −0.03899 (18) 0.0584 (9)
H22A 0.5351 0.6771 −0.0840 0.070*
C23 0.4340 (3) 0.7258 (2) −0.01101 (18) 0.0578 (9)
H23A 0.3637 0.7078 −0.0371 0.069*
C24 0.4363 (3) 0.77059 (19) 0.05528 (18) 0.0514 (8)
H24A 0.3665 0.7831 0.0730 0.062*
C25 0.5396 (3) 0.79833 (17) 0.09746 (16) 0.0414 (7)
C26 0.5264 (2) 0.84892 (18) 0.16933 (16) 0.0424 (7)
C27 0.4832 (3) 0.93557 (18) 0.14954 (17) 0.0470 (8)
C28 0.5316 (3) 0.9954 (2) 0.10912 (19) 0.0614 (9)
H28A 0.5993 0.9855 0.0878 0.074*
C29 0.4774 (4) 1.0712 (2) 0.1008 (2) 0.0726 (11)
H29A 0.5088 1.1124 0.0733 0.087*
C30 0.3779 (4) 1.0858 (2) 0.1327 (2) 0.0762 (12)
H30A 0.3433 1.1370 0.1270 0.091*
C31 0.3284 (3) 1.0264 (2) 0.1728 (2) 0.0682 (10)
H31A 0.2605 1.0367 0.1938 0.082*
C32 0.3816 (3) 0.9507 (2) 0.18140 (17) 0.0511 (8)
C33 0.3506 (3) 0.8771 (2) 0.22174 (17) 0.0503 (8)
C34 0.2593 (3) 0.8615 (3) 0.2634 (2) 0.0678 (11)
H34A 0.2048 0.9018 0.2692 0.081*
C35 0.2510 (3) 0.7854 (3) 0.2959 (2) 0.0734 (12)
H35A 0.1899 0.7743 0.3235 0.088*
C36 0.3315 (3) 0.7256 (3) 0.28821 (19) 0.0673 (10)
H36A 0.3241 0.6746 0.3105 0.081*
C37 0.4236 (3) 0.7407 (2) 0.24757 (18) 0.0548 (9)
H37A 0.4785 0.7005 0.2425 0.066*
C38 0.4321 (3) 0.81679 (19) 0.21478 (16) 0.0451 (8)
C39 0.5324 (3) 0.5281 (3) 0.1162 (2) 0.0869 (13)
H39A 0.5772 0.4805 0.1328 0.130*
H39B 0.5655 0.5751 0.1437 0.130*
H39C 0.5330 0.5360 0.0618 0.130*
C40 0.4118 (4) 0.5169 (2) 0.1319 (2) 0.0696 (11)
C41 0.2259 (3) 0.5774 (3) 0.1255 (3) 0.0903 (13)
H41A 0.2232 0.5760 0.1807 0.108*
H41B 0.1883 0.5287 0.1026 0.108*
C42 0.1664 (4) 0.6520 (3) 0.0910 (3) 0.0979 (15)
H42A 0.0869 0.6516 0.1003 0.147*
H42B 0.1695 0.6527 0.0364 0.147*
H42C 0.2043 0.6997 0.1142 0.147*
O3 0.3748 (3) 0.45679 (18) 0.15903 (17) 0.0996 (10)
O4 0.3455 (2) 0.58069 (16) 0.11015 (16) 0.0795 (8)
H2 0.677 (3) 0.741 (2) 0.223 (2) 0.092 (14)*
H1 0.627 (3) 0.883 (2) 0.257 (2) 0.098 (15)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0430 (13) 0.0475 (14) 0.0667 (15) −0.0008 (11) 0.0142 (11) 0.0074 (12)
O2 0.0447 (13) 0.0490 (13) 0.0467 (13) 0.0032 (10) 0.0036 (10) −0.0076 (11)
C1 0.0485 (19) 0.0426 (19) 0.065 (2) −0.0026 (16) 0.0176 (17) 0.0049 (17)
C2 0.082 (3) 0.051 (2) 0.084 (3) 0.002 (2) 0.018 (2) −0.008 (2)
C3 0.119 (4) 0.057 (3) 0.112 (4) 0.005 (3) 0.040 (3) −0.018 (3)
C4 0.107 (4) 0.050 (3) 0.155 (5) 0.011 (3) 0.068 (4) 0.007 (3)
C5 0.063 (3) 0.059 (3) 0.132 (4) 0.013 (2) 0.037 (3) 0.035 (3)
C6 0.050 (2) 0.048 (2) 0.089 (3) 0.0038 (17) 0.021 (2) 0.021 (2)
C7 0.049 (2) 0.066 (2) 0.074 (3) −0.0098 (19) 0.0057 (19) 0.030 (2)
C8 0.071 (3) 0.097 (4) 0.094 (3) −0.016 (3) −0.007 (3) 0.050 (3)
C9 0.104 (4) 0.126 (5) 0.071 (3) −0.048 (4) −0.016 (3) 0.042 (3)
C10 0.099 (4) 0.116 (4) 0.054 (3) −0.047 (3) 0.007 (2) 0.004 (3)
C11 0.071 (3) 0.079 (3) 0.061 (2) −0.021 (2) 0.011 (2) 0.002 (2)
C12 0.053 (2) 0.057 (2) 0.053 (2) −0.0129 (18) 0.0085 (16) 0.0087 (17)
C13 0.0390 (18) 0.0460 (18) 0.0540 (19) −0.0014 (14) 0.0100 (14) 0.0024 (15)
C14 0.0471 (19) 0.0391 (17) 0.0466 (18) −0.0027 (14) 0.0155 (15) −0.0051 (14)
C15 0.047 (2) 0.056 (2) 0.055 (2) −0.0029 (17) 0.0090 (16) −0.0008 (17)
C16 0.056 (2) 0.063 (2) 0.063 (2) −0.0176 (18) 0.0205 (18) −0.0044 (19)
C17 0.073 (3) 0.053 (2) 0.056 (2) −0.0111 (19) 0.0217 (19) 0.0012 (17)
C18 0.061 (2) 0.048 (2) 0.0491 (19) −0.0008 (17) 0.0138 (16) 0.0026 (16)
C19 0.0537 (19) 0.0388 (17) 0.0392 (16) 0.0013 (15) 0.0131 (14) −0.0020 (14)
C20 0.0490 (19) 0.0391 (17) 0.0389 (16) 0.0011 (14) 0.0066 (14) 0.0019 (13)
C21 0.063 (2) 0.050 (2) 0.0453 (18) 0.0062 (17) 0.0116 (16) −0.0004 (15)
C22 0.083 (3) 0.051 (2) 0.0395 (18) −0.0038 (19) 0.0034 (18) −0.0082 (16)
C23 0.066 (2) 0.059 (2) 0.0458 (19) −0.0139 (18) −0.0034 (17) −0.0015 (17)
C24 0.051 (2) 0.054 (2) 0.0489 (19) −0.0045 (16) 0.0051 (16) 0.0017 (16)
C25 0.0466 (19) 0.0363 (16) 0.0411 (16) −0.0015 (14) 0.0054 (14) 0.0038 (13)
C26 0.0416 (18) 0.0440 (18) 0.0418 (17) 0.0010 (14) 0.0059 (14) −0.0029 (14)
C27 0.055 (2) 0.0431 (18) 0.0416 (17) 0.0042 (15) 0.0021 (15) −0.0021 (15)
C28 0.078 (3) 0.051 (2) 0.057 (2) 0.0031 (19) 0.0170 (19) −0.0005 (17)
C29 0.110 (3) 0.046 (2) 0.061 (2) 0.006 (2) 0.008 (2) 0.0046 (18)
C30 0.113 (4) 0.055 (2) 0.058 (2) 0.033 (2) 0.003 (2) −0.0008 (19)
C31 0.077 (3) 0.072 (3) 0.056 (2) 0.029 (2) 0.0095 (19) 0.002 (2)
C32 0.053 (2) 0.055 (2) 0.0449 (18) 0.0139 (17) 0.0031 (15) −0.0025 (16)
C33 0.0410 (19) 0.067 (2) 0.0424 (17) 0.0075 (17) 0.0030 (14) −0.0042 (16)
C34 0.044 (2) 0.102 (3) 0.058 (2) 0.012 (2) 0.0087 (17) 0.001 (2)
C35 0.052 (2) 0.117 (4) 0.052 (2) −0.015 (2) 0.0106 (18) 0.007 (2)
C36 0.067 (2) 0.083 (3) 0.051 (2) −0.018 (2) 0.0041 (19) 0.0135 (19)
C37 0.056 (2) 0.055 (2) 0.053 (2) −0.0053 (17) 0.0055 (17) 0.0032 (16)
C38 0.0438 (18) 0.052 (2) 0.0393 (17) −0.0020 (15) 0.0046 (14) −0.0004 (15)
C39 0.072 (3) 0.086 (3) 0.099 (3) 0.003 (2) −0.003 (2) 0.013 (3)
C40 0.086 (3) 0.062 (3) 0.057 (2) −0.009 (2) −0.004 (2) 0.015 (2)
C41 0.072 (3) 0.103 (4) 0.100 (3) −0.019 (3) 0.027 (3) 0.007 (3)
C42 0.071 (3) 0.095 (3) 0.130 (4) 0.000 (3) 0.024 (3) −0.001 (3)
O3 0.119 (2) 0.086 (2) 0.091 (2) −0.0147 (19) 0.0023 (18) 0.0400 (18)
O4 0.0705 (18) 0.0692 (18) 0.101 (2) −0.0052 (14) 0.0190 (15) 0.0229 (15)

Geometric parameters (Å, °)

O1—C13 1.423 (3) C22—C23 1.372 (5)
O1—H2 0.93 (4) C22—H22A 0.9300
O2—C26 1.442 (3) C23—C24 1.368 (4)
O2—H1 0.88 (4) C23—H23A 0.9300
C1—C2 1.375 (5) C24—C25 1.399 (4)
C1—C6 1.394 (4) C24—H24A 0.9300
C1—C13 1.524 (4) C25—C26 1.529 (4)
C2—C3 1.394 (5) C26—C27 1.528 (4)
C2—H2A 0.9300 C26—C38 1.532 (4)
C3—C4 1.369 (6) C27—C28 1.372 (4)
C3—H3A 0.9300 C27—C32 1.396 (4)
C4—C5 1.373 (6) C28—C29 1.391 (5)
C4—H4A 0.9300 C28—H28A 0.9300
C5—C6 1.388 (5) C29—C30 1.372 (5)
C5—H5A 0.9300 C29—H29A 0.9300
C6—C7 1.457 (5) C30—C31 1.370 (5)
C7—C12 1.382 (5) C30—H30A 0.9300
C7—C8 1.397 (5) C31—C32 1.384 (4)
C8—C9 1.370 (6) C31—H31A 0.9300
C8—H8A 0.9300 C32—C33 1.464 (4)
C9—C10 1.375 (7) C33—C38 1.386 (4)
C9—H9A 0.9300 C33—C34 1.390 (4)
C10—C11 1.394 (5) C34—C35 1.378 (5)
C10—H10A 0.9300 C34—H34A 0.9300
C11—C12 1.385 (5) C35—C36 1.374 (5)
C11—H11A 0.9300 C35—H35A 0.9300
C12—C13 1.537 (4) C36—C37 1.386 (5)
C13—C14 1.534 (4) C36—H36A 0.9300
C14—C15 1.396 (4) C37—C38 1.379 (4)
C14—C19 1.404 (4) C37—H37A 0.9300
C15—C16 1.378 (4) C39—C40 1.478 (5)
C15—H15A 0.9300 C39—H39A 0.9600
C16—C17 1.372 (5) C39—H39B 0.9600
C16—H16A 0.9300 C39—H39C 0.9600
C17—C18 1.377 (4) C40—O3 1.197 (4)
C17—H17A 0.9300 C40—O4 1.323 (4)
C18—C19 1.391 (4) C41—O4 1.454 (4)
C18—H18A 0.9300 C41—C42 1.491 (5)
C19—C20 1.514 (4) C41—H41A 0.9700
C20—C21 1.393 (4) C41—H41B 0.9700
C20—C25 1.403 (4) C42—H42A 0.9600
C21—C22 1.383 (4) C42—H42B 0.9600
C21—H21A 0.9300 C42—H42C 0.9600
C13—O1—H2 106 (2) C24—C23—H23A 120.0
C26—O2—H1 106 (3) C22—C23—H23A 120.0
C2—C1—C6 120.9 (3) C23—C24—C25 122.5 (3)
C2—C1—C13 128.0 (3) C23—C24—H24A 118.7
C6—C1—C13 111.1 (3) C25—C24—H24A 118.7
C1—C2—C3 118.5 (4) C24—C25—C20 118.2 (3)
C1—C2—H2A 120.8 C24—C25—C26 115.7 (3)
C3—C2—H2A 120.8 C20—C25—C26 126.1 (3)
C4—C3—C2 120.6 (5) O2—C26—C27 110.9 (2)
C4—C3—H3A 119.7 O2—C26—C25 108.4 (2)
C2—C3—H3A 119.7 C27—C26—C25 112.5 (2)
C3—C4—C5 121.3 (4) O2—C26—C38 110.0 (2)
C3—C4—H4A 119.4 C27—C26—C38 101.5 (2)
C5—C4—H4A 119.4 C25—C26—C38 113.4 (2)
C4—C5—C6 118.9 (4) C28—C27—C32 120.5 (3)
C4—C5—H5A 120.6 C28—C27—C26 129.3 (3)
C6—C5—H5A 120.6 C32—C27—C26 110.2 (3)
C5—C6—C1 119.9 (4) C27—C28—C29 118.6 (3)
C5—C6—C7 131.5 (4) C27—C28—H28A 120.7
C1—C6—C7 108.6 (3) C29—C28—H28A 120.7
C12—C7—C8 119.6 (4) C30—C29—C28 120.5 (4)
C12—C7—C6 109.0 (3) C30—C29—H29A 119.7
C8—C7—C6 131.4 (4) C28—C29—H29A 119.7
C9—C8—C7 118.7 (5) C31—C30—C29 121.4 (3)
C9—C8—H8A 120.6 C31—C30—H30A 119.3
C7—C8—H8A 120.6 C29—C30—H30A 119.3
C8—C9—C10 121.7 (5) C30—C31—C32 118.5 (3)
C8—C9—H9A 119.2 C30—C31—H31A 120.7
C10—C9—H9A 119.2 C32—C31—H31A 120.7
C9—C10—C11 120.3 (5) C31—C32—C27 120.4 (3)
C9—C10—H10A 119.8 C31—C32—C33 130.7 (3)
C11—C10—H10A 119.8 C27—C32—C33 108.8 (3)
C12—C11—C10 118.0 (4) C38—C33—C34 119.7 (3)
C12—C11—H11A 121.0 C38—C33—C32 109.1 (3)
C10—C11—H11A 121.0 C34—C33—C32 131.1 (3)
C7—C12—C11 121.6 (3) C35—C34—C33 118.9 (3)
C7—C12—C13 111.0 (3) C35—C34—H34A 120.6
C11—C12—C13 127.4 (3) C33—C34—H34A 120.6
O1—C13—C1 107.5 (2) C36—C35—C34 121.1 (3)
O1—C13—C14 112.8 (2) C36—C35—H35A 119.4
C1—C13—C14 112.6 (2) C34—C35—H35A 119.4
O1—C13—C12 110.2 (2) C35—C36—C37 120.5 (4)
C1—C13—C12 100.4 (3) C35—C36—H36A 119.7
C14—C13—C12 112.7 (3) C37—C36—H36A 119.7
C15—C14—C19 118.1 (3) C38—C37—C36 118.5 (3)
C15—C14—C13 117.2 (3) C38—C37—H37A 120.7
C19—C14—C13 124.8 (3) C36—C37—H37A 120.7
C16—C15—C14 122.4 (3) C37—C38—C33 121.2 (3)
C16—C15—H15A 118.8 C37—C38—C26 128.4 (3)
C14—C15—H15A 118.8 C33—C38—C26 110.3 (3)
C17—C16—C15 119.4 (3) C40—C39—H39A 109.5
C17—C16—H16A 120.3 C40—C39—H39B 109.5
C15—C16—H16A 120.3 H39A—C39—H39B 109.5
C16—C17—C18 119.2 (3) C40—C39—H39C 109.5
C16—C17—H17A 120.4 H39A—C39—H39C 109.5
C18—C17—H17A 120.4 H39B—C39—H39C 109.5
C17—C18—C19 122.7 (3) O3—C40—O4 122.3 (4)
C17—C18—H18A 118.7 O3—C40—C39 125.3 (4)
C19—C18—H18A 118.7 O4—C40—C39 112.4 (3)
C18—C19—C14 118.3 (3) O4—C41—C42 107.5 (3)
C18—C19—C20 114.4 (3) O4—C41—H41A 110.2
C14—C19—C20 126.7 (3) C42—C41—H41A 110.2
C21—C20—C25 117.8 (3) O4—C41—H41B 110.2
C21—C20—C19 114.2 (3) C42—C41—H41B 110.2
C25—C20—C19 127.6 (3) H41A—C41—H41B 108.5
C22—C21—C20 123.2 (3) C41—C42—H42A 109.5
C22—C21—H21A 118.4 C41—C42—H42B 109.5
C20—C21—H21A 118.4 H42A—C42—H42B 109.5
C23—C22—C21 118.4 (3) C41—C42—H42C 109.5
C23—C22—H22A 120.8 H42A—C42—H42C 109.5
C21—C22—H22A 120.8 H42B—C42—H42C 109.5
C24—C23—C22 120.0 (3) C40—O4—C41 117.0 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O2—H1···O3i 0.88 (4) 1.90 (4) 2.779 (3) 173 (4)
O1—H2···O2 0.93 (4) 1.84 (4) 2.739 (3) 161 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: GK2155).

References

  1. Barbour, L. J., Bourne, S. A., Caira, M. R., Nassimbeni, L. R., Weber, E., Skobridis, E. K. & Wierig, A. (1993). Supramol. Chem.1, 331–336.
  2. Ibragimov, B. T., Beketov, K. M., Weber, E., Seidel, J., Sumarna, O., Makhkamov, K. K. & Kohnke, K. (2001). J. Phys. Org. Chem.14, 697–703.
  3. Sardone, N. (1996). Private communication (refcode NABNIN). CCDC, Union Road, Cambridge, England.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Siemens (1994). XP Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
  6. Stoe & Cie (1997). STADI4 and X-RED Stoe & Cie, Darmstadt, Germany.
  7. Sumarna, O., Seidel, J., Weber, E., Seichter, W., Ibragimov, B. T. & Beketov, K. M. (2003). Cryst. Growth Des.3, 541–546.
  8. Weber, E., Skobridis, K., Wierig, A., Stathi, S., Nassimbeni, L. R. & Niven, M. L. (1993). Angew. Chem. Int. Ed. Engl.32, 606–608.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808023271/gk2155sup1.cif

e-64-o1627-sup1.cif (24.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023271/gk2155Isup2.hkl

e-64-o1627-Isup2.hkl (276.6KB, hkl)

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


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