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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Feb 13;64(Pt 3):o588. doi: 10.1107/S1600536808003644

2,6-Di-tert-butyl-4-(methoxy­meth­yl)phenol

Tao Zeng a,*, Ju-Feng Sun b
PMCID: PMC2960792  PMID: 21201926

Abstract

The title compound, C16H26O2, was easily obtained in high yield when 4-bromo­methyl-2,6-di-tert-butyl­phenol was reacted with methanol. There are two independent mol­ecules in the asymmetric unit. The meth­oxy group in each of the independent mol­ecules was found to be disordered, with site-occupation factors of 0.8728 (18)/0.1272 (18) and 0.8781 (17)/0.1219 (17).

Related literature

For related literature, see: Rieker et al. (1968); Yamazaki & Seguchi (1997); Zeng et al. (2005).graphic file with name e-64-0o588-scheme1.jpg

Experimental

Crystal data

  • C16H26O2

  • M r = 250.37

  • Monoclinic, Inline graphic

  • a = 14.240 (3) Å

  • b = 18.012 (3) Å

  • c = 13.677 (3) Å

  • β = 118.603 (3)°

  • V = 3079.7 (10) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.07 mm−1

  • T = 294 (2) K

  • 0.26 × 0.24 × 0.20 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2002) T min = 0.982, T max = 0.986

  • 15799 measured reflections

  • 5428 independent reflections

  • 2928 reflections with I > 2σ(I)

  • R int = 0.046

Refinement

  • R[F 2 > 2σ(F 2)] = 0.060

  • wR(F 2) = 0.189

  • S = 1.04

  • 5428 reflections

  • 378 parameters

  • 108 restraints

  • H-atom parameters constrained

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808003644/er2048sup1.cif

e-64-0o588-sup1.cif (28.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808003644/er2048Isup2.hkl

e-64-0o588-Isup2.hkl (265.8KB, hkl)

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

Acknowledgments

The authors gratefully acknowledge financial support from the Start Foundation for Doctors (HY071314) of Yantai University.

supplementary crystallographic information

Comment

Hindered phenol antioxidants are widely used in polymers and lubricants. It could protect polymers by increasing both their process stability and long-term stability against oxidative degradation (Yamazaki & Seguchi, 1997). In former papers, we have reported the reaction of 4-bromomethyl-20,6-di-tet-butyl-phenol with amines (Zeng et al., 2005) and it was showed that the 4-bromomethyl-2,6-di-tet-butyl-phenol was highly reactive. The title compound, C16H26O2,(1),has been easily synthesied when we tried to dissolve the 4-bromomethyl-2,6-di-tert-butyl-phenol in methanol. It was found that there are two independent molecules in the asymmetric units. The phenolic hydroxyl are hindered by the adjacent tert-butyl groups. And both of the methoxyl groups in the two molecules were found disordered with with site occupation fators 0.8728 (18)/0.1272 (18) and 0.8781 (17)/0.1219 (17).

Experimental

The 4-bromomethyl-2,6-di-tert-butyl-phenol (7.15 g) was synthesized from 2,6-di-tert-butyl-4-methylphenol (5.5 g, 0.025 mol) and equivalent NBS (Rieker et al., 1968) in a yield of 96%. Then 40 ml me thanol was added and stirred for 5 min the produt (5.85 g, 0.023 mol) was obtained in a yield of 97.3%. Suitable crystals were obtained by slow evaporation of a mixture of ethyl acetate and ethanol.

Refinement

The H atoms of O—H were initially located in a difference Fourier Map and restrained on their parent atoms with O—H restrained 0.82 Å. In absence of significant anomalous dispersion effects, Friedel-pair reflections were merged prior to refinement. All H other atoms were positioned geometrically and refined using a riding model, in the range of 0.93–0.97 Å, with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(Cmethyl).

Figures

Fig. 1.

Fig. 1.

The two independent molecules in the structure of (I). Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii.

Crystal data

C16H26O2 F000 = 1104
Mr = 250.37 Dx = 1.080 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
a = 14.240 (3) Å Cell parameters from 2933 reflections
b = 18.012 (3) Å θ = 2.8–25.4º
c = 13.677 (3) Å µ = 0.07 mm1
β = 118.603 (3)º T = 294 (2) K
V = 3079.7 (10) Å3 Block, colourless
Z = 8 0.26 × 0.24 × 0.20 mm

Data collection

Bruker SMART CCD area-detector diffractometer 5428 independent reflections
Radiation source: fine-focus sealed tube 2928 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.046
T = 294(2) K θmax = 25.0º
φ and ω scans θmin = 1.6º
Absorption correction: multi-scan(SADABS; Sheldrick, 2002) h = −13→16
Tmin = 0.982, Tmax = 0.986 k = −20→21
15799 measured reflections l = −16→10

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.060 H-atom parameters constrained
wR(F2) = 0.189   w = 1/[σ2(Fo2) + (0.0751P)2 + 1.0963P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.002
5428 reflections Δρmax = 0.31 e Å3
378 parameters Δρmin = −0.26 e Å3
108 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0102 (7)

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 Occ. (<1)
O1 0.29438 (11) 0.73376 (8) 0.66027 (11) 0.0698 (5)
H1 0.2550 0.7700 0.6367 0.105*
O3 0.20663 (10) 0.25936 (8) 0.37111 (12) 0.0701 (4)
H3 0.2381 0.2196 0.3821 0.105*
C1 0.35866 (12) 0.74063 (10) 0.77320 (14) 0.0425 (5)
C2 0.39601 (12) 0.67334 (9) 0.83200 (14) 0.0410 (5)
C3 0.46179 (12) 0.67844 (10) 0.94611 (14) 0.0448 (5)
H3A 0.4869 0.6349 0.9871 0.054*
C4 0.49145 (12) 0.74549 (10) 1.00116 (14) 0.0453 (5)
C5 0.45463 (13) 0.80952 (10) 0.94014 (15) 0.0501 (5)
H5 0.4756 0.8548 0.9771 0.060*
C6 0.38758 (12) 0.80988 (10) 0.82580 (15) 0.0450 (5)
C7 0.34673 (15) 0.88356 (11) 0.76197 (18) 0.0626 (6)
C8 0.22446 (17) 0.88849 (13) 0.7136 (2) 0.0880 (9)
H8A 0.1995 0.9353 0.6763 0.132*
H8B 0.2067 0.8845 0.7728 0.132*
H8C 0.1910 0.8488 0.6614 0.132*
C9 0.3953 (2) 0.95088 (12) 0.8398 (2) 0.0973 (10)
H9A 0.4714 0.9513 0.8684 0.146*
H9B 0.3796 0.9474 0.9006 0.146*
H9C 0.3651 0.9958 0.7990 0.146*
C10 0.37776 (19) 0.89054 (13) 0.6695 (2) 0.0911 (8)
H10A 0.3479 0.9354 0.6282 0.137*
H10B 0.3506 0.8486 0.6205 0.137*
H10C 0.4543 0.8920 0.7020 0.137*
C11 0.36507 (14) 0.59799 (10) 0.77160 (16) 0.0528 (6)
C12 0.40573 (18) 0.59247 (12) 0.68675 (19) 0.0808 (8)
H12A 0.3708 0.6292 0.6298 0.121*
H12B 0.3904 0.5439 0.6537 0.121*
H12C 0.4816 0.6008 0.7234 0.121*
C13 0.41538 (18) 0.53359 (11) 0.8551 (2) 0.0815 (9)
H13A 0.3971 0.4872 0.8157 0.122*
H13B 0.3886 0.5343 0.9076 0.122*
H13C 0.4917 0.5392 0.8940 0.122*
C14 0.24411 (16) 0.58545 (12) 0.7145 (2) 0.0785 (8)
H14A 0.2089 0.6230 0.6588 0.118*
H14B 0.2197 0.5881 0.7688 0.118*
H14C 0.2277 0.5374 0.6800 0.118*
C17 0.14067 (12) 0.25795 (10) 0.41872 (14) 0.0428 (5)
C18 0.11153 (12) 0.19114 (9) 0.44964 (14) 0.0424 (5)
C19 0.04478 (13) 0.19708 (10) 0.49784 (14) 0.0473 (5)
H19 0.0243 0.1539 0.5200 0.057*
C20 0.00815 (12) 0.26412 (10) 0.51383 (14) 0.0463 (5)
C21 0.03681 (13) 0.32793 (10) 0.47987 (14) 0.0469 (5)
H21 0.0107 0.3731 0.4894 0.056*
C22 0.10338 (13) 0.32747 (10) 0.43179 (14) 0.0435 (5)
C23 0.13593 (15) 0.40024 (10) 0.39658 (16) 0.0565 (6)
C24 0.25658 (16) 0.41172 (13) 0.4620 (2) 0.0821 (8)
H24A 0.2748 0.4583 0.4412 0.123*
H24B 0.2920 0.3721 0.4456 0.123*
H24C 0.2789 0.4120 0.5402 0.123*
C25 0.0990 (2) 0.39898 (13) 0.27121 (18) 0.0843 (8)
H25A 0.1168 0.4453 0.2495 0.126*
H25B 0.0230 0.3916 0.2308 0.126*
H25C 0.1342 0.3592 0.2549 0.126*
C26 0.08391 (18) 0.46798 (11) 0.4192 (2) 0.0839 (8)
H26A 0.1046 0.4700 0.4971 0.126*
H26B 0.0075 0.4639 0.3766 0.126*
H26C 0.1071 0.5124 0.3982 0.126*
C27 0.15203 (15) 0.11556 (11) 0.43482 (17) 0.0591 (6)
C28 0.12020 (19) 0.10122 (12) 0.3133 (2) 0.0873 (8)
H28A 0.0437 0.1021 0.2696 0.131*
H28B 0.1465 0.0535 0.3064 0.131*
H28C 0.1503 0.1390 0.2872 0.131*
C29 0.10241 (17) 0.05158 (11) 0.4707 (2) 0.0827 (8)
H29A 0.1247 0.0559 0.5487 0.124*
H29B 0.1260 0.0048 0.4566 0.124*
H29C 0.0258 0.0544 0.4290 0.124*
C30 0.27315 (16) 0.11003 (13) 0.5082 (2) 0.0907 (9)
H30A 0.3074 0.1487 0.4885 0.136*
H30B 0.2974 0.0626 0.4973 0.136*
H30C 0.2907 0.1153 0.5849 0.136*
C15 0.55793 (15) 0.75095 (12) 1.12630 (15) 0.0648 (6) 0.8728 (18)
H15A 0.5955 0.7980 1.1459 0.078* 0.8728 (18)
H15B 0.5114 0.7492 1.1598 0.078* 0.8728 (18)
O2 0.63105 (11) 0.69353 (9) 1.16775 (11) 0.0614 (5) 0.8728 (18)
C16 0.6887 (2) 0.69504 (18) 1.28628 (18) 0.0875 (10) 0.8728 (18)
H16A 0.7390 0.6548 1.3127 0.131* 0.8728 (18)
H16B 0.6397 0.6901 1.3155 0.131* 0.8728 (18)
H16C 0.7264 0.7413 1.3106 0.131* 0.8728 (18)
C15' 0.5580 (8) 0.7510 (7) 1.1264 (5) 0.0648 (6) 0.1272 (18)
H15C 0.5102 0.7640 1.1557 0.078* 0.1272 (18)
H15D 0.5856 0.7018 1.1541 0.078* 0.1272 (18)
O2' 0.6430 (6) 0.7997 (6) 1.1711 (6) 0.105 (6) 0.1272 (18)
C16' 0.6844 (13) 0.7853 (10) 1.2889 (7) 0.073 (5) 0.1272 (18)
H16D 0.7463 0.8156 1.3310 0.110* 0.1272 (18)
H16E 0.7037 0.7339 1.3040 0.110* 0.1272 (18)
H16F 0.6306 0.7969 1.3097 0.110* 0.1272 (18)
C31 −0.0573 (9) 0.2684 (4) 0.5737 (4) 0.0646 (6) 0.8781 (17)
H31A −0.0098 0.2663 0.6533 0.078* 0.8781 (17)
H31B −0.0948 0.3154 0.5568 0.078* 0.8781 (17)
O4 −0.13064 (10) 0.21107 (9) 0.54314 (11) 0.0608 (5) 0.8781 (17)
C32 −0.18536 (18) 0.21175 (19) 0.6076 (2) 0.0943 (11) 0.8781 (17)
H32A −0.2358 0.1716 0.5845 0.141* 0.8781 (17)
H32B −0.2226 0.2580 0.5966 0.141* 0.8781 (17)
H32C −0.1345 0.2061 0.6850 0.141* 0.8781 (17)
C31' −0.0573 (9) 0.2684 (4) 0.5737 (4) 0.0646 (6) 0.1219 (17)
H31C −0.0839 0.2190 0.5752 0.078* 0.1219 (17)
H31D −0.0106 0.2831 0.6501 0.078* 0.1219 (17)
O4' −0.1426 (5) 0.3164 (5) 0.5280 (6) 0.071 (3) 0.1219 (17)
C32' −0.1973 (8) 0.3038 (9) 0.5923 (9) 0.060 (4) 0.1219 (17)
H32D −0.2571 0.3371 0.5676 0.089* 0.1219 (17)
H32E −0.1489 0.3125 0.6697 0.089* 0.1219 (17)
H32F −0.2224 0.2535 0.5823 0.089* 0.1219 (17)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0750 (9) 0.0690 (9) 0.0423 (8) 0.0148 (7) 0.0095 (7) 0.0070 (7)
O3 0.0796 (7) 0.0652 (9) 0.0971 (8) 0.0051 (7) 0.0677 (6) 0.0076 (7)
C1 0.0349 (8) 0.0530 (10) 0.0384 (9) 0.0040 (8) 0.0167 (7) 0.0026 (8)
C2 0.0342 (8) 0.0445 (10) 0.0426 (9) 0.0019 (7) 0.0171 (7) 0.0041 (8)
C3 0.0345 (8) 0.0532 (10) 0.0451 (9) 0.0028 (8) 0.0178 (7) 0.0099 (8)
C4 0.0330 (8) 0.0600 (11) 0.0424 (9) −0.0013 (8) 0.0177 (7) −0.0034 (9)
C5 0.0427 (8) 0.0513 (11) 0.0595 (10) −0.0009 (8) 0.0272 (8) −0.0114 (9)
C6 0.0379 (8) 0.0463 (10) 0.0548 (10) 0.0044 (8) 0.0255 (7) 0.0010 (8)
C7 0.0625 (11) 0.0460 (11) 0.0771 (13) 0.0114 (9) 0.0318 (10) 0.0058 (10)
C8 0.0754 (13) 0.0737 (15) 0.1056 (18) 0.0319 (12) 0.0358 (13) 0.0151 (13)
C9 0.1047 (17) 0.0478 (13) 0.126 (2) 0.0059 (13) 0.0441 (15) −0.0020 (14)
C10 0.1118 (16) 0.0688 (14) 0.1058 (16) 0.0121 (13) 0.0626 (13) 0.0317 (13)
C11 0.0470 (9) 0.0475 (11) 0.0550 (11) −0.0020 (8) 0.0172 (8) 0.0005 (9)
C12 0.0961 (14) 0.0655 (14) 0.0892 (15) −0.0035 (12) 0.0511 (12) −0.0236 (12)
C13 0.0829 (15) 0.0466 (12) 0.0873 (17) −0.0029 (11) 0.0184 (13) 0.0079 (12)
C14 0.0588 (12) 0.0702 (14) 0.0853 (16) −0.0185 (11) 0.0174 (12) −0.0097 (12)
C17 0.0356 (7) 0.0538 (11) 0.0412 (9) −0.0024 (8) 0.0201 (7) 0.0017 (8)
C18 0.0352 (8) 0.0455 (10) 0.0433 (9) 0.0007 (8) 0.0163 (7) 0.0050 (8)
C19 0.0380 (8) 0.0542 (11) 0.0494 (10) −0.0012 (8) 0.0206 (7) 0.0113 (9)
C20 0.0346 (8) 0.0618 (11) 0.0409 (9) 0.0026 (8) 0.0167 (7) 0.0020 (9)
C21 0.0399 (8) 0.0511 (10) 0.0457 (10) 0.0012 (8) 0.0172 (7) −0.0046 (9)
C22 0.0393 (8) 0.0464 (10) 0.0408 (9) −0.0026 (8) 0.0158 (7) 0.0003 (8)
C23 0.0612 (10) 0.0472 (11) 0.0587 (11) −0.0110 (9) 0.0269 (9) −0.0012 (9)
C24 0.0755 (12) 0.0713 (14) 0.0990 (16) −0.0283 (11) 0.0415 (12) −0.0053 (13)
C25 0.1207 (16) 0.0698 (14) 0.0628 (13) −0.0133 (13) 0.0443 (12) 0.0119 (11)
C26 0.1037 (15) 0.0477 (12) 0.1044 (17) −0.0043 (12) 0.0532 (13) −0.0026 (12)
C27 0.0565 (9) 0.0487 (11) 0.0801 (12) 0.0080 (9) 0.0392 (9) 0.0096 (10)
C28 0.1188 (16) 0.0573 (13) 0.0998 (16) 0.0070 (13) 0.0637 (13) −0.0119 (12)
C29 0.0912 (13) 0.0477 (12) 0.1248 (17) 0.0076 (11) 0.0643 (12) 0.0154 (12)
C30 0.0632 (12) 0.0791 (15) 0.133 (2) 0.0299 (11) 0.0492 (12) 0.0286 (14)
C15 0.0585 (10) 0.0878 (15) 0.0508 (10) 0.0038 (10) 0.0283 (8) −0.0017 (10)
O2 0.0523 (8) 0.0869 (11) 0.0372 (8) 0.0066 (8) 0.0153 (6) 0.0022 (8)
C16 0.0718 (16) 0.142 (3) 0.0366 (13) 0.0054 (17) 0.0159 (12) 0.0100 (15)
C15' 0.0585 (10) 0.0878 (15) 0.0508 (10) 0.0038 (10) 0.0283 (8) −0.0017 (10)
O2' 0.043 (6) 0.204 (15) 0.049 (7) 0.037 (8) 0.006 (5) −0.019 (8)
C16' 0.069 (6) 0.087 (7) 0.061 (6) −0.005 (6) 0.029 (5) −0.002 (6)
C31 0.0554 (9) 0.0890 (14) 0.0601 (10) −0.0009 (10) 0.0362 (8) 0.0004 (10)
O4 0.0464 (7) 0.0904 (11) 0.0556 (8) −0.0017 (8) 0.0326 (6) 0.0079 (8)
C32 0.0657 (12) 0.163 (3) 0.0771 (15) −0.0018 (17) 0.0522 (11) 0.0131 (17)
C31' 0.0554 (9) 0.0890 (14) 0.0601 (10) −0.0009 (10) 0.0362 (8) 0.0004 (10)
O4' 0.065 (4) 0.091 (4) 0.065 (4) 0.001 (3) 0.038 (3) −0.001 (4)
C32' 0.061 (6) 0.073 (7) 0.066 (6) 0.012 (5) 0.048 (4) 0.001 (5)

Geometric parameters (Å, °)

O1—C1 1.373 (2) C21—H21 0.9300
O1—H1 0.8200 C22—C23 1.542 (3)
O3—C17 1.376 (2) C23—C24 1.524 (3)
O3—H3 0.8200 C23—C26 1.534 (3)
C1—C6 1.400 (2) C23—C25 1.534 (3)
C1—C2 1.410 (2) C24—H24A 0.9600
C2—C3 1.386 (2) C24—H24B 0.9600
C2—C11 1.539 (2) C24—H24C 0.9600
C3—C4 1.378 (2) C25—H25A 0.9600
C3—H3A 0.9300 C25—H25B 0.9600
C4—C5 1.372 (2) C25—H25C 0.9600
C4—C15 1.511 (2) C26—H26A 0.9600
C5—C6 1.388 (2) C26—H26B 0.9600
C5—H5 0.9300 C26—H26C 0.9600
C6—C7 1.541 (3) C27—C28 1.521 (3)
C7—C10 1.531 (4) C27—C30 1.528 (3)
C7—C8 1.541 (3) C27—C29 1.549 (3)
C7—C9 1.542 (3) C28—H28A 0.9600
C8—H8A 0.9600 C28—H28B 0.9600
C8—H8B 0.9600 C28—H28C 0.9600
C8—H8C 0.9600 C29—H29A 0.9600
C9—H9A 0.9600 C29—H29B 0.9600
C9—H9B 0.9600 C29—H29C 0.9600
C9—H9C 0.9600 C30—H30A 0.9600
C10—H10A 0.9600 C30—H30B 0.9600
C10—H10B 0.9600 C30—H30C 0.9600
C10—H10C 0.9600 C15—O2 1.382 (2)
C11—C12 1.528 (3) C15—H15A 0.9700
C11—C14 1.530 (3) C15—H15B 0.9700
C11—C13 1.543 (3) O2—C16 1.424 (3)
C12—H12A 0.9600 C16—H16A 0.9600
C12—H12B 0.9600 C16—H16B 0.9600
C12—H12C 0.9600 C16—H16C 0.9600
C13—H13A 0.9600 O2'—C16' 1.449 (8)
C13—H13B 0.9600 C16'—H16D 0.9600
C13—H13C 0.9600 C16'—H16E 0.9600
C14—H14A 0.9600 C16'—H16F 0.9600
C14—H14B 0.9600 C31—O4 1.383 (2)
C14—H14C 0.9600 C31—H31A 0.9700
C17—C18 1.403 (2) C31—H31B 0.9700
C17—C22 1.404 (2) O4—C32 1.429 (3)
C18—C19 1.396 (3) C32—H32A 0.9600
C18—C27 1.529 (3) C32—H32B 0.9600
C19—C20 1.374 (3) C32—H32C 0.9600
C19—H19 0.9300 O4'—C32' 1.445 (9)
C20—C21 1.373 (3) C32'—H32D 0.9600
C20—C31 1.507 (3) C32'—H32E 0.9600
C21—C22 1.389 (3) C32'—H32F 0.9600
C1—O1—H1 109.5 C24—C23—C26 106.94 (17)
C17—O3—H3 109.5 C24—C23—C25 110.1 (2)
O1—C1—C6 122.15 (15) C26—C23—C25 107.30 (17)
O1—C1—C2 115.50 (15) C24—C23—C22 110.80 (15)
C6—C1—C2 122.33 (15) C26—C23—C22 111.50 (19)
C3—C2—C1 116.88 (16) C25—C23—C22 110.07 (15)
C3—C2—C11 121.88 (15) C23—C24—H24A 109.5
C1—C2—C11 121.24 (15) C23—C24—H24B 109.5
C4—C3—C2 122.57 (16) H24A—C24—H24B 109.5
C4—C3—H3A 118.7 C23—C24—H24C 109.5
C2—C3—H3A 118.7 H24A—C24—H24C 109.5
C5—C4—C3 118.45 (15) H24B—C24—H24C 109.5
C5—C4—C15 118.95 (17) C23—C25—H25A 109.5
C3—C4—C15 122.52 (17) C23—C25—H25B 109.5
C4—C5—C6 123.06 (17) H25A—C25—H25B 109.5
C4—C5—H5 118.5 C23—C25—H25C 109.5
C6—C5—H5 118.5 H25A—C25—H25C 109.5
C5—C6—C1 116.70 (16) H25B—C25—H25C 109.5
C5—C6—C7 120.77 (16) C23—C26—H26A 109.5
C1—C6—C7 122.53 (16) C23—C26—H26B 109.5
C10—C7—C8 110.73 (19) H26A—C26—H26B 109.5
C10—C7—C6 111.01 (18) C23—C26—H26C 109.5
C8—C7—C6 109.59 (17) H26A—C26—H26C 109.5
C10—C7—C9 107.1 (2) H26B—C26—H26C 109.5
C8—C7—C9 107.01 (19) C28—C27—C30 111.0 (2)
C6—C7—C9 111.29 (17) C28—C27—C18 111.22 (16)
C7—C8—H8A 109.5 C30—C27—C18 110.47 (16)
C7—C8—H8B 109.5 C28—C27—C29 106.11 (18)
H8A—C8—H8B 109.5 C30—C27—C29 106.62 (17)
C7—C8—H8C 109.5 C18—C27—C29 111.22 (18)
H8A—C8—H8C 109.5 C27—C28—H28A 109.5
H8B—C8—H8C 109.5 C27—C28—H28B 109.5
C7—C9—H9A 109.5 H28A—C28—H28B 109.5
C7—C9—H9B 109.5 C27—C28—H28C 109.5
H9A—C9—H9B 109.5 H28A—C28—H28C 109.5
C7—C9—H9C 109.5 H28B—C28—H28C 109.5
H9A—C9—H9C 109.5 C27—C29—H29A 109.5
H9B—C9—H9C 109.5 C27—C29—H29B 109.5
C7—C10—H10A 109.5 H29A—C29—H29B 109.5
C7—C10—H10B 109.5 C27—C29—H29C 109.5
H10A—C10—H10B 109.5 H29A—C29—H29C 109.5
C7—C10—H10C 109.5 H29B—C29—H29C 109.5
H10A—C10—H10C 109.5 C27—C30—H30A 109.5
H10B—C10—H10C 109.5 C27—C30—H30B 109.5
C12—C11—C14 110.25 (18) H30A—C30—H30B 109.5
C12—C11—C2 110.47 (17) C27—C30—H30C 109.5
C14—C11—C2 111.54 (16) H30A—C30—H30C 109.5
C12—C11—C13 107.62 (18) H30B—C30—H30C 109.5
C14—C11—C13 106.10 (17) O2—C15—C4 110.88 (17)
C2—C11—C13 110.70 (15) O2—C15—H15A 109.5
C11—C12—H12A 109.5 C4—C15—H15A 109.5
C11—C12—H12B 109.5 O2—C15—H15B 109.5
H12A—C12—H12B 109.5 C4—C15—H15B 109.5
C11—C12—H12C 109.5 H15A—C15—H15B 108.1
H12A—C12—H12C 109.5 C15—O2—C16 111.31 (19)
H12B—C12—H12C 109.5 O2—C16—H16A 109.5
C11—C13—H13A 109.5 O2—C16—H16B 109.5
C11—C13—H13B 109.5 H16A—C16—H16B 109.5
H13A—C13—H13B 109.5 O2—C16—H16C 109.5
C11—C13—H13C 109.5 H16A—C16—H16C 109.5
H13A—C13—H13C 109.5 H16B—C16—H16C 109.5
H13B—C13—H13C 109.5 O2'—C16'—H16D 109.5
C11—C14—H14A 109.5 O2'—C16'—H16E 109.5
C11—C14—H14B 109.5 H16D—C16'—H16E 109.5
H14A—C14—H14B 109.5 O2'—C16'—H16F 109.5
C11—C14—H14C 109.5 H16D—C16'—H16F 109.5
H14A—C14—H14C 109.5 H16E—C16'—H16F 109.5
H14B—C14—H14C 109.5 O4—C31—C20 111.93 (17)
O3—C17—C18 121.74 (16) O4—C31—H31A 109.2
O3—C17—C22 115.43 (16) C20—C31—H31A 109.2
C18—C17—C22 122.82 (18) O4—C31—H31B 109.2
C19—C18—C17 116.31 (16) C20—C31—H31B 109.2
C19—C18—C27 121.06 (17) H31A—C31—H31B 107.9
C17—C18—C27 122.61 (18) C31—O4—C32 111.38 (19)
C20—C19—C18 122.59 (17) O4—C32—H32A 109.5
C20—C19—H19 118.7 O4—C32—H32B 109.5
C18—C19—H19 118.7 H32A—C32—H32B 109.5
C21—C20—C19 119.02 (18) O4—C32—H32C 109.5
C21—C20—C31 120.16 (18) H32A—C32—H32C 109.5
C19—C20—C31 120.73 (18) H32B—C32—H32C 109.5
C20—C21—C22 122.41 (17) O4'—C32'—H32D 109.5
C20—C21—H21 118.8 O4'—C32'—H32E 109.5
C22—C21—H21 118.8 H32D—C32'—H32E 109.5
C21—C22—C17 116.82 (17) O4'—C32'—H32F 109.5
C21—C22—C23 121.21 (17) H32D—C32'—H32F 109.5
C17—C22—C23 121.97 (18) H32E—C32'—H32F 109.5
O1—C1—C2—C3 179.52 (16) C22—C17—C18—C27 179.76 (15)
C6—C1—C2—C3 1.3 (3) C17—C18—C19—C20 0.5 (2)
O1—C1—C2—C11 −0.3 (3) C27—C18—C19—C20 179.07 (15)
C6—C1—C2—C11 −178.52 (18) C18—C19—C20—C21 0.9 (2)
C1—C2—C3—C4 −0.8 (3) C18—C19—C20—C31 −175.59 (15)
C11—C2—C3—C4 179.05 (18) C19—C20—C21—C22 −1.3 (2)
C2—C3—C4—C5 −0.3 (3) C31—C20—C21—C22 175.23 (15)
C2—C3—C4—C15 176.40 (18) C20—C21—C22—C17 0.2 (2)
C3—C4—C5—C6 1.0 (3) C20—C21—C22—C23 −178.79 (15)
C15—C4—C5—C6 −175.84 (18) O3—C17—C22—C21 −179.85 (14)
C4—C5—C6—C1 −0.5 (3) C18—C17—C22—C21 1.4 (2)
C4—C5—C6—C7 178.64 (19) O3—C17—C22—C23 −0.9 (2)
O1—C1—C6—C5 −178.78 (17) C18—C17—C22—C23 −179.64 (15)
C2—C1—C6—C5 −0.7 (3) C21—C22—C23—C24 117.6 (2)
O1—C1—C6—C7 2.1 (3) C17—C22—C23—C24 −61.3 (2)
C2—C1—C6—C7 −179.83 (18) C21—C22—C23—C26 −1.4 (2)
C5—C6—C7—C10 122.6 (2) C17—C22—C23—C26 179.73 (15)
C1—C6—C7—C10 −58.3 (2) C21—C22—C23—C25 −120.32 (19)
C5—C6—C7—C8 −114.8 (2) C17—C22—C23—C25 60.8 (2)
C1—C6—C7—C8 64.4 (3) C19—C18—C27—C28 122.42 (19)
C5—C6—C7—C9 3.4 (3) C17—C18—C27—C28 −59.2 (2)
C1—C6—C7—C9 −177.5 (2) C19—C18—C27—C30 −113.8 (2)
C3—C2—C11—C12 −118.3 (2) C17—C18—C27—C30 64.6 (2)
C1—C2—C11—C12 61.5 (2) C19—C18—C27—C29 4.4 (2)
C3—C2—C11—C14 118.7 (2) C17—C18—C27—C29 −177.19 (16)
C1—C2—C11—C14 −61.5 (3) C5—C4—C15—O2 −148.81 (18)
C3—C2—C11—C13 0.8 (3) C3—C4—C15—O2 34.4 (3)
C1—C2—C11—C13 −179.37 (19) C4—C15—O2—C16 −175.74 (19)
O3—C17—C18—C19 179.58 (14) C21—C20—C31—O4 142.81 (16)
C22—C17—C18—C19 −1.7 (2) C19—C20—C31—O4 −40.7 (2)
O3—C17—C18—C27 1.1 (2) C20—C31—O4—C32 174.72 (17)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ER2048).

References

  1. Bruker (1997). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Rieker, A., Kaufmann, D., Brück, R., Workman, R. & Müller, E. (1968). Tetrahedron, 24, 103–115.
  3. Sheldrick, G. M. (2002). SADABS University of Göttingen, Germany.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Yamazaki, T. & Seguchi, T. (1997). J. Polym. Sci. A: Polym. Chem.35, 2431–2439.
  6. Zeng, T., Dong, C.-M. & Shu, X.-G. (2005). Acta Cryst. E61, o2334–o2335.

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/S1600536808003644/er2048sup1.cif

e-64-0o588-sup1.cif (28.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808003644/er2048Isup2.hkl

e-64-0o588-Isup2.hkl (265.8KB, hkl)

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


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