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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jan 23;64(Pt 2):o490. doi: 10.1107/S1600536808001517

9-n-Butyl-9,9′-bi[9H-fluorene]

Shu-Qiang Yu a, Bin-Bin Hu a, Ping Lu a,*
PMCID: PMC2960402  PMID: 21201513

Abstract

In the title compound, C30H26, the dihedral angle between the two fluorene ring systems is 61.75 (4)°.

Related literature

For general background, see: Muller et al. (2003); Murahashi & Moritani (1967).graphic file with name e-64-0o490-scheme1.jpg

Experimental

Crystal data

  • C30H26

  • M r = 386.51

  • Monoclinic, Inline graphic

  • a = 27.164 (5) Å

  • b = 8.6369 (17) Å

  • c = 19.232 (4) Å

  • β = 104.28 (3)°

  • V = 4372.7 (15) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.07 mm−1

  • T = 298 (2) K

  • 0.46 × 0.38 × 0.35 mm

Data collection

  • Bruker SMART 1000 CCD area-detector diffractometer

  • Absorption correction: none

  • 20365 measured reflections

  • 4970 independent reflections

  • 2859 reflections with I > 2σ(I)

  • R int = 0.031

Refinement

  • R[F 2 > 2σ(F 2)] = 0.039

  • wR(F 2) = 0.122

  • S = 1.06

  • 4970 reflections

  • 273 parameters

  • H-atom parameters constrained

  • Δρmax = 0.18 e Å−3

  • Δρmin = −0.14 e Å−3

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and publCIF (Westrip, 2008).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808001517/xu2394sup1.cif

e-64-0o490-sup1.cif (23.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808001517/xu2394Isup2.hkl

e-64-0o490-Isup2.hkl (243.5KB, hkl)

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

Acknowledgments

The authors thank the National Natural Science Foundation of China (20674070) and the Natural Science Foundation of Zhejiang Province (R404109).

supplementary crystallographic information

Comment

Fluorene derivatives, including polyfluorenes and oligofluorenes, remain a subject of intense investigation in recent years because they are very promising candidates for blue light-emitting materials in organic light-emitting devices (Muller et al., 2003). The title compound, 9-n-butyl-9,9'-bi(9H-fluorene)(hereinafter abbreviated to bbf), is one of bifluorene derivatives (Murahashi & Moritani, 1967).

The asymmetric unit of the title compound contains only one bbf molecule (Fig. 1). Two fluorene rings are linked together through their 9-position carbon atoms (C1 and C14). The dihedral angle between the two fluorene rings is 61.75 (4)°. The centroid to centroid distance between stacked fluorene rings is ca 5.92 Å, which is very long and prevents π-π stacking (Fig. 2). All bond lengths and angles are normal.

Experimental

All chemicals were of reagent grade quality obtained from commercial sources and used as received, unless stated otherwise. n-Butylithium (8 ml, 2.5 M, 20 mmol) was added to fluorene (1.66 g, 10 mmol) in 40 ml dry tetrahydrofuran under nitrogen at -78 °C. Subsequently, BF3Et2O (0.21 g, 2 mmol) was added. Kept it for 1 h, and warmed it to room temperature and stirred it overnight. After reaction completion, solvent was evaporated under reduced pressure. The crude products were purified by column chromatography (silica gel) using n-hexane/dichloromethane as eluent. The title compound was obtained as white solid in 30% yield. Colorless single crystals were grown from slow evaporation of a saturated CH2Cl2 solution of the compound.

Refinement

H atoms were positioned geometrically and treated as riding, with C—H = 0.93 (aromatic), 0.97 (methylene) or 0.96 Å (methyl), Uiso(H) = 1.5Ueq(C) for methyl or Uiso(H) = 1.2Ueq(C) for others.

Figures

Fig. 1.

Fig. 1.

The molecular structure showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are shown as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

Partial packing view, H atoms are omitted for clarity.

Crystal data

C30H26 F000 = 1648
Mr = 386.51 Dx = 1.174 Mg m3
Monoclinic, C2/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 12421 reflections
a = 27.164 (5) Å θ = 3.0–27.4º
b = 8.6369 (17) Å µ = 0.07 mm1
c = 19.232 (4) Å T = 298 (2) K
β = 104.28 (3)º Chunk, colorless
V = 4372.7 (15) Å3 0.46 × 0.38 × 0.35 mm
Z = 8

Data collection

Bruker SMART 1000 CCD area-detector diffractometer 2859 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.031
Monochromator: graphite θmax = 27.4º
T = 298(2) K θmin = 3.1º
φ and ω scans h = −35→35
Absorption correction: none k = −11→10
20365 measured reflections l = −24→24
4970 independent reflections

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.039   w = 1/[σ2(Fo2) + (0.0595P)2 + 0.3188P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.122 (Δ/σ)max < 0.001
S = 1.06 Δρmax = 0.18 e Å3
4970 reflections Δρmin = −0.14 e Å3
273 parameters Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0038 (4)
Secondary atom site location: difference Fourier map

Special details

Experimental. 1H NMR (500 MHz, δ in p.p.m., CDCl3): 0.68-0.74 (m, 5H), 0.17-1.22 (m, 2H), 2.55-2.58 (m, 2H), 4.58 (s, 1H), 6.76 (d, 2H, J = 7.00 Hz), 6.86 (d, 2H, J = 7.00 Hz), 6.97 (t, 2H, J = 7.50 Hz), 7.08 (t, 2H, J = 7.50 Hz), 7.17-7.23 (m, 4H), 7.49 (d, 2H, J = 7.50 Hz); 13C NMR (125 MHz, δ in p.p.m., CDCl3): 14.15, 23.35, 26.45, 38.86, 55.48, 57.75, 119.39,119.62, 123.40, 125.84, 126.00, 126.90, 127.35, 141.59, 142.19, 144.37, 148.57; MS (EI): calcd for C30H26, 386.2; found, 386 (M+), 326, 313, 300, 221 (100), 179, 165, 152.
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
C1 0.11948 (5) 0.49033 (14) −0.00529 (6) 0.0446 (3)
C2 0.09626 (5) 0.61937 (15) −0.05656 (7) 0.0482 (3)
C3 0.05151 (6) 0.61827 (19) −0.11011 (7) 0.0622 (4)
H3 0.0322 0.5285 −0.1203 0.075*
C4 0.03611 (7) 0.7533 (2) −0.14825 (8) 0.0765 (5)
H4 0.0058 0.7547 −0.1836 0.092*
C5 0.06533 (8) 0.8858 (2) −0.13425 (9) 0.0788 (5)
H5 0.0546 0.9751 −0.1607 0.095*
C6 0.11021 (7) 0.88774 (17) −0.08167 (9) 0.0669 (4)
H6 0.1299 0.9770 −0.0728 0.080*
C7 0.12544 (5) 0.75404 (15) −0.04213 (7) 0.0501 (3)
C8 0.16888 (5) 0.72391 (15) 0.01911 (7) 0.0492 (3)
C9 0.20847 (6) 0.81905 (18) 0.05433 (9) 0.0648 (4)
H9 0.2109 0.9204 0.0392 0.078*
C10 0.24415 (6) 0.7601 (2) 0.11223 (9) 0.0730 (5)
H10 0.2707 0.8227 0.1365 0.088*
C11 0.24097 (6) 0.6098 (2) 0.13449 (8) 0.0679 (4)
H11 0.2653 0.5725 0.1737 0.082*
C12 0.20198 (5) 0.51323 (17) 0.09921 (7) 0.0562 (4)
H12 0.2003 0.4113 0.1141 0.067*
C13 0.16563 (5) 0.57100 (14) 0.04155 (6) 0.0453 (3)
C14 0.08081 (5) 0.43871 (14) 0.03910 (7) 0.0481 (3)
H14 0.0498 0.4014 0.0055 0.058*
C15 0.06633 (5) 0.56906 (16) 0.08363 (7) 0.0518 (3)
C16 0.04276 (5) 0.71006 (18) 0.06246 (9) 0.0617 (4)
H16 0.0342 0.7384 0.0143 0.074*
C17 0.03222 (6) 0.8079 (2) 0.11398 (10) 0.0757 (5)
H17 0.0167 0.9028 0.1002 0.091*
C18 0.04449 (7) 0.7664 (2) 0.18550 (10) 0.0828 (5)
H18 0.0371 0.8337 0.2193 0.099*
C19 0.06752 (7) 0.6270 (2) 0.20742 (9) 0.0744 (5)
H19 0.0755 0.5993 0.2556 0.089*
C20 0.07864 (5) 0.52777 (18) 0.15625 (7) 0.0566 (4)
C21 0.09993 (5) 0.37098 (17) 0.16385 (7) 0.0553 (4)
C22 0.11628 (6) 0.2786 (2) 0.22436 (8) 0.0694 (4)
H22 0.1170 0.3176 0.2697 0.083*
C23 0.13134 (7) 0.1289 (2) 0.21644 (10) 0.0774 (5)
H23 0.1429 0.0670 0.2567 0.093*
C24 0.12937 (7) 0.07014 (19) 0.14925 (10) 0.0768 (5)
H24 0.1392 −0.0317 0.1446 0.092*
C25 0.11283 (6) 0.16108 (17) 0.08828 (8) 0.0661 (4)
H25 0.1109 0.1196 0.0430 0.079*
C26 0.09925 (5) 0.31399 (16) 0.09538 (7) 0.0519 (3)
C27 0.13491 (5) 0.35210 (15) −0.04660 (7) 0.0525 (3)
H27A 0.1531 0.2773 −0.0121 0.063*
H27B 0.1043 0.3022 −0.0742 0.063*
C28 0.16785 (6) 0.39514 (15) −0.09723 (7) 0.0558 (4)
H28A 0.1501 0.4721 −0.1310 0.067*
H28B 0.1990 0.4421 −0.0695 0.067*
C29 0.18128 (7) 0.26016 (17) −0.13865 (8) 0.0685 (4)
H29A 0.1503 0.2082 −0.1635 0.082*
H29B 0.2014 0.1869 −0.1052 0.082*
C30 0.21068 (8) 0.3067 (2) −0.19310 (9) 0.0881 (6)
H30A 0.1908 0.3783 −0.2269 0.132*
H30B 0.2177 0.2164 −0.2181 0.132*
H30C 0.2420 0.3550 −0.1688 0.132*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0415 (7) 0.0482 (7) 0.0460 (7) −0.0060 (6) 0.0142 (5) −0.0020 (6)
C2 0.0433 (7) 0.0593 (8) 0.0459 (7) −0.0001 (6) 0.0186 (6) 0.0001 (6)
C3 0.0508 (9) 0.0868 (11) 0.0499 (8) 0.0004 (8) 0.0139 (7) 0.0039 (8)
C4 0.0623 (11) 0.1144 (15) 0.0535 (9) 0.0212 (10) 0.0157 (8) 0.0162 (10)
C5 0.0905 (14) 0.0866 (12) 0.0679 (10) 0.0336 (11) 0.0358 (10) 0.0248 (10)
C6 0.0836 (12) 0.0559 (8) 0.0704 (10) 0.0098 (8) 0.0365 (9) 0.0072 (8)
C7 0.0529 (8) 0.0493 (8) 0.0549 (8) 0.0031 (6) 0.0260 (6) 0.0012 (6)
C8 0.0473 (8) 0.0491 (7) 0.0567 (8) −0.0060 (6) 0.0232 (6) −0.0071 (6)
C9 0.0626 (10) 0.0559 (8) 0.0801 (10) −0.0169 (7) 0.0258 (8) −0.0134 (8)
C10 0.0554 (10) 0.0829 (12) 0.0798 (11) −0.0220 (8) 0.0146 (9) −0.0215 (9)
C11 0.0441 (9) 0.0922 (12) 0.0640 (9) −0.0055 (8) 0.0068 (7) −0.0079 (9)
C12 0.0448 (8) 0.0635 (8) 0.0600 (8) −0.0021 (7) 0.0123 (6) 0.0001 (7)
C13 0.0383 (7) 0.0513 (7) 0.0494 (7) −0.0032 (6) 0.0169 (6) −0.0062 (6)
C14 0.0437 (7) 0.0556 (7) 0.0470 (7) −0.0109 (6) 0.0148 (6) −0.0044 (6)
C15 0.0368 (7) 0.0645 (8) 0.0575 (8) −0.0096 (6) 0.0182 (6) −0.0080 (7)
C16 0.0473 (8) 0.0704 (9) 0.0729 (9) −0.0019 (7) 0.0254 (7) −0.0040 (8)
C17 0.0625 (11) 0.0751 (11) 0.0997 (13) 0.0026 (8) 0.0394 (9) −0.0123 (10)
C18 0.0761 (12) 0.0938 (13) 0.0885 (13) −0.0032 (10) 0.0390 (10) −0.0320 (11)
C19 0.0682 (11) 0.0985 (13) 0.0610 (9) −0.0059 (10) 0.0248 (8) −0.0185 (9)
C20 0.0422 (8) 0.0766 (10) 0.0537 (8) −0.0100 (7) 0.0172 (6) −0.0111 (7)
C21 0.0441 (8) 0.0723 (9) 0.0510 (8) −0.0129 (7) 0.0146 (6) −0.0014 (7)
C22 0.0606 (10) 0.0949 (12) 0.0529 (8) −0.0117 (9) 0.0147 (7) 0.0030 (9)
C23 0.0701 (11) 0.0909 (12) 0.0723 (11) −0.0040 (9) 0.0199 (9) 0.0229 (10)
C24 0.0811 (12) 0.0638 (10) 0.0934 (13) −0.0049 (9) 0.0365 (10) 0.0171 (10)
C25 0.0790 (11) 0.0602 (9) 0.0667 (9) −0.0149 (8) 0.0325 (8) 0.0007 (8)
C26 0.0475 (8) 0.0594 (8) 0.0524 (8) −0.0146 (6) 0.0191 (6) −0.0021 (7)
C27 0.0569 (9) 0.0514 (7) 0.0531 (7) −0.0082 (6) 0.0208 (6) −0.0051 (6)
C28 0.0611 (9) 0.0551 (8) 0.0562 (8) −0.0035 (7) 0.0242 (7) −0.0029 (7)
C29 0.0848 (12) 0.0617 (9) 0.0693 (10) 0.0068 (8) 0.0389 (9) −0.0003 (8)
C30 0.1143 (16) 0.0845 (12) 0.0849 (12) 0.0179 (11) 0.0617 (11) 0.0060 (10)

Geometric parameters (Å, °)

C1—C2 1.5183 (18) C16—H16 0.9300
C1—C13 1.5203 (17) C17—C18 1.380 (2)
C1—C27 1.5481 (18) C17—H17 0.9300
C1—C14 1.5728 (18) C18—C19 1.374 (2)
C2—C3 1.386 (2) C18—H18 0.9300
C2—C7 1.3963 (18) C19—C20 1.393 (2)
C3—C4 1.386 (2) C19—H19 0.9300
C3—H3 0.9300 C20—C21 1.466 (2)
C4—C5 1.381 (2) C21—C22 1.390 (2)
C4—H4 0.9300 C21—C26 1.4018 (18)
C5—C6 1.379 (3) C22—C23 1.376 (2)
C5—H5 0.9300 C22—H22 0.9300
C6—C7 1.3884 (19) C23—C24 1.377 (2)
C6—H6 0.9300 C23—H23 0.9300
C7—C8 1.470 (2) C24—C25 1.391 (2)
C8—C9 1.3897 (19) C24—H24 0.9300
C8—C13 1.3989 (18) C25—C26 1.387 (2)
C9—C10 1.381 (2) C25—H25 0.9300
C9—H9 0.9300 C27—C28 1.5222 (19)
C10—C11 1.376 (2) C27—H27A 0.9700
C10—H10 0.9300 C27—H27B 0.9700
C11—C12 1.387 (2) C28—C29 1.5067 (19)
C11—H11 0.9300 C28—H28A 0.9700
C12—C13 1.3833 (19) C28—H28B 0.9700
C12—H12 0.9300 C29—C30 1.520 (2)
C14—C26 1.5217 (19) C29—H29A 0.9700
C14—C15 1.5237 (18) C29—H29B 0.9700
C14—H14 0.9800 C30—H30A 0.9600
C15—C16 1.389 (2) C30—H30B 0.9600
C15—C20 1.3997 (19) C30—H30C 0.9600
C16—C17 1.385 (2)
C2—C1—C13 101.43 (10) C18—C17—C16 120.85 (17)
C2—C1—C27 110.77 (10) C18—C17—H17 119.6
C13—C1—C27 111.68 (11) C16—C17—H17 119.6
C2—C1—C14 109.53 (10) C19—C18—C17 120.85 (16)
C13—C1—C14 111.83 (10) C19—C18—H18 119.6
C27—C1—C14 111.19 (10) C17—C18—H18 119.6
C3—C2—C7 120.28 (13) C18—C19—C20 118.94 (16)
C3—C2—C1 128.70 (13) C18—C19—H19 120.5
C7—C2—C1 110.96 (11) C20—C19—H19 120.5
C2—C3—C4 118.83 (15) C19—C20—C15 120.53 (15)
C2—C3—H3 120.6 C19—C20—C21 130.31 (14)
C4—C3—H3 120.6 C15—C20—C21 109.04 (12)
C5—C4—C3 120.68 (16) C22—C21—C26 120.82 (15)
C5—C4—H4 119.7 C22—C21—C20 130.58 (14)
C3—C4—H4 119.7 C26—C21—C20 108.50 (12)
C6—C5—C4 120.98 (15) C23—C22—C21 119.27 (15)
C6—C5—H5 119.5 C23—C22—H22 120.4
C4—C5—H5 119.5 C21—C22—H22 120.4
C5—C6—C7 118.81 (16) C22—C23—C24 120.43 (16)
C5—C6—H6 120.6 C22—C23—H23 119.8
C7—C6—H6 120.6 C24—C23—H23 119.8
C6—C7—C2 120.40 (14) C23—C24—C25 120.85 (17)
C6—C7—C8 131.13 (13) C23—C24—H24 119.6
C2—C7—C8 108.42 (11) C25—C24—H24 119.6
C9—C8—C13 120.53 (13) C26—C25—C24 119.55 (15)
C9—C8—C7 131.11 (13) C26—C25—H25 120.2
C13—C8—C7 108.36 (11) C24—C25—H25 120.2
C10—C9—C8 118.67 (14) C25—C26—C21 118.99 (13)
C10—C9—H9 120.7 C25—C26—C14 130.76 (12)
C8—C9—H9 120.7 C21—C26—C14 110.21 (12)
C11—C10—C9 120.90 (14) C28—C27—C1 114.59 (11)
C11—C10—H10 119.5 C28—C27—H27A 108.6
C9—C10—H10 119.5 C1—C27—H27A 108.6
C10—C11—C12 120.93 (15) C28—C27—H27B 108.6
C10—C11—H11 119.5 C1—C27—H27B 108.6
C12—C11—H11 119.5 H27A—C27—H27B 107.6
C13—C12—C11 118.90 (14) C29—C28—C27 113.98 (11)
C13—C12—H12 120.6 C29—C28—H28A 108.8
C11—C12—H12 120.6 C27—C28—H28A 108.8
C12—C13—C8 120.06 (12) C29—C28—H28B 108.8
C12—C13—C1 129.12 (12) C27—C28—H28B 108.8
C8—C13—C1 110.82 (11) H28A—C28—H28B 107.7
C26—C14—C15 102.04 (10) C28—C29—C30 113.36 (13)
C26—C14—C1 116.10 (11) C28—C29—H29A 108.9
C15—C14—C1 113.28 (10) C30—C29—H29A 108.9
C26—C14—H14 108.3 C28—C29—H29B 108.9
C15—C14—H14 108.3 C30—C29—H29B 108.9
C1—C14—H14 108.3 H29A—C29—H29B 107.7
C16—C15—C20 119.68 (13) C29—C30—H30A 109.5
C16—C15—C14 130.33 (13) C29—C30—H30B 109.5
C20—C15—C14 109.96 (12) H30A—C30—H30B 109.5
C17—C16—C15 119.15 (15) C29—C30—H30C 109.5
C17—C16—H16 120.4 H30A—C30—H30C 109.5
C15—C16—H16 120.4 H30B—C30—H30C 109.5
C13—C1—C2—C3 −176.43 (13) C13—C1—C14—C15 51.64 (14)
C27—C1—C2—C3 64.89 (18) C27—C1—C14—C15 177.25 (11)
C14—C1—C2—C3 −58.12 (17) C26—C14—C15—C16 −173.67 (13)
C13—C1—C2—C7 1.02 (13) C1—C14—C15—C16 60.77 (18)
C27—C1—C2—C7 −117.65 (12) C26—C14—C15—C20 4.01 (14)
C14—C1—C2—C7 119.34 (11) C1—C14—C15—C20 −121.55 (12)
C7—C2—C3—C4 −0.8 (2) C20—C15—C16—C17 0.5 (2)
C1—C2—C3—C4 176.49 (13) C14—C15—C16—C17 177.98 (14)
C2—C3—C4—C5 1.4 (2) C15—C16—C17—C18 −0.5 (2)
C3—C4—C5—C6 −0.6 (3) C16—C17—C18—C19 0.0 (3)
C4—C5—C6—C7 −0.7 (2) C17—C18—C19—C20 0.4 (3)
C5—C6—C7—C2 1.3 (2) C18—C19—C20—C15 −0.3 (2)
C5—C6—C7—C8 −175.78 (14) C18—C19—C20—C21 −175.94 (15)
C3—C2—C7—C6 −0.6 (2) C16—C15—C20—C19 −0.1 (2)
C1—C2—C7—C6 −178.28 (12) C14—C15—C20—C19 −178.06 (13)
C3—C2—C7—C8 177.11 (12) C16—C15—C20—C21 176.36 (12)
C1—C2—C7—C8 −0.59 (15) C14—C15—C20—C21 −1.60 (15)
C6—C7—C8—C9 −2.2 (3) C19—C20—C21—C22 −1.9 (3)
C2—C7—C8—C9 −179.55 (14) C15—C20—C21—C22 −177.95 (15)
C6—C7—C8—C13 177.20 (14) C19—C20—C21—C26 174.22 (15)
C2—C7—C8—C13 −0.16 (15) C15—C20—C21—C26 −1.79 (15)
C13—C8—C9—C10 −0.6 (2) C26—C21—C22—C23 −0.8 (2)
C7—C8—C9—C10 178.69 (14) C20—C21—C22—C23 174.97 (15)
C8—C9—C10—C11 0.5 (2) C21—C22—C23—C24 −1.2 (3)
C9—C10—C11—C12 0.3 (3) C22—C23—C24—C25 0.9 (3)
C10—C11—C12—C13 −0.9 (2) C23—C24—C25—C26 1.5 (3)
C11—C12—C13—C8 0.8 (2) C24—C25—C26—C21 −3.4 (2)
C11—C12—C13—C1 −179.59 (13) C24—C25—C26—C14 179.11 (14)
C9—C8—C13—C12 0.0 (2) C22—C21—C26—C25 3.1 (2)
C7—C8—C13—C12 −179.46 (12) C20—C21—C26—C25 −173.51 (13)
C9—C8—C13—C1 −179.69 (12) C22—C21—C26—C14 −178.93 (13)
C7—C8—C13—C1 0.84 (14) C20—C21—C26—C14 4.46 (15)
C2—C1—C13—C12 179.22 (13) C15—C14—C26—C25 172.52 (14)
C27—C1—C13—C12 −62.77 (17) C1—C14—C26—C25 −63.80 (19)
C14—C1—C13—C12 62.57 (17) C15—C14—C26—C21 −5.13 (14)
C2—C1—C13—C8 −1.12 (13) C1—C14—C26—C21 118.54 (12)
C27—C1—C13—C8 116.89 (12) C2—C1—C27—C28 51.73 (15)
C14—C1—C13—C8 −117.77 (12) C13—C1—C27—C28 −60.53 (15)
C2—C1—C14—C26 −177.61 (10) C14—C1—C27—C28 173.78 (11)
C13—C1—C14—C26 −65.98 (14) C1—C27—C28—C29 −178.29 (13)
C27—C1—C14—C26 59.63 (14) C27—C28—C29—C30 175.53 (14)
C2—C1—C14—C15 −59.99 (13)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU2394).

References

  1. Bruker (2001). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Muller, C. D., Falcou, A., Reckefuss, N., Rojahn, M., Wiederhirn, V., Rudati, P., Frohne, H., Nuyken, O., Becker, H. & Meerholz, K. (2003). Nature (London), 421, 829–833. [DOI] [PubMed]
  3. Murahashi, S. & Moritani, I. (1967). Tetrahedron, 23, 3631–3643.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Westrip, S. P. (2008). publCIF In preparation.

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/S1600536808001517/xu2394sup1.cif

e-64-0o490-sup1.cif (23.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808001517/xu2394Isup2.hkl

e-64-0o490-Isup2.hkl (243.5KB, hkl)

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


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