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A new non-centrosymmetric monoclinic modification of 9,10-di­hydro­anthracene-9,10-α,β-succinic acid anhydride (sys­tem­atic name: 5,6:7,8-dibenzobi­cyclo­[2.2.2]­octa-5,7-diene-2,3-di­carboxyl­ic acid anhydride), C18H12O3, was obtained by reacting maleic anhydride and anthracene in xyl­ene, followed by recrystallization from ethyl acetate. The structure consists of chains of mol­ecules along the c axis and is held together solely through van der Waals interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802005767/bt6131sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802005767/bt6131Isup2.hkl
Contains datablock I

CCDC reference: 185775

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.036
  • wR factor = 0.084
  • Data-to-parameter ratio = 8.1

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
REFLT_03 From the CIF: _diffrn_reflns_theta_max 28.31 From the CIF: _reflns_number_total 1543 TEST2: Reflns within _diffrn_reflns_theta_max Count of symmetry unique reflns 1653 Completeness (_total/calc) 93.35% Alert C: < 95% complete General Notes
REFLT_03 From the CIF: _diffrn_reflns_theta_max 28.31 From the CIF: _reflns_number_total 1543 Count of symmetry unique reflns 1653 Completeness (_total/calc) 93.35% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

As part of a project on Diels–Alder reactions in an undergraduate organic chemistry laboratory, 9,10-dihydroanthracene-9,10-α,β-succinic acid anhydride, (I), was synthesized. The compound had been previously prepared (Bulgarovskii et al., 1979) and the crystal data and coordinates are reported in the Cambridge Structural Database (refcode BCOCAN; Allen & Kennard, 1993). Bulgarovskii et al. used benzene as the reaction and crystallization solvent, while in the present study, xylene was used for the reaction and the material was recrystallized from ethyl acetate. The reported unit-cell parameters for BCOCAN are a = 11.229 (3), b = 12.874 (3), c = 9.468 (4) Å and γ = 103.51 (2)° (space group P21/b). The cell in (I) and the cell obtained by Bulgarovskii et al., (II), are related, approximately, by the transformation aII = [001/101/010]aI. The frames collected were re-indexed in cell (II) and attempts were made to solve the structure in this cell but without success. Therefore, it was considered appropriate to describe the material under investigation as a new polymorph.

In the structure of BCOCAN, pairs of molecules related by the 21 axis face each other in an antiparallel fashion and have the planes of the anhydride rings parallel to the b axis. The central O atom of these rings points approximately in the +c and -c directions.

In contrast, as shown in Fig. 2, in the Cc polymorph, the molecules pack in chains along the c axis, with the planes of the anhydride rings approximately parallel to the b axis. The central O atoms of the anhydride rings point in the [11] and [110] directions.

In both cases, van der Waals interactions are responsible of the interactions between the molecules.

Experimental top

The title compound was prepared by mixing maleic anhydride (dienophile) and anthracene (diene) in xylene in a 1:1 molar ratio. The mixture was refluxed at 403–413 K for 35 min. The resulting solution was allowed to cool to room temperature and was then placed in a water–ice bath. The yellow crystals formed were removed by filtration and washed with ethyl acetate. They were recrystallized from hot ethyl acetate, using activated charcoal to remove impurities. Colourless crystals formed upon cooling the ethyl acetate solution. The IR spectra were recorded from KBr discs, using a PE-1600 FTIR spectrometer with IRDM software. IR (cm-1): ν(δb C—H asymmetric) 3075, ν(C—H symmetric) 3026, ν(C—H) 2968, ν(CO asymmetric) 1862, ν(CO symmetric) 1782, ν(CC) 1463, ν(C—O asymmetric) 1229, ν(C—O symmetric) 1069. The 1H and 13C NMR spectra were obtained on a Bruker Advance 400 equipment. 1H NMR (400 MHz, CDCl3, M4Si; δH, p.p.m.): 3.55 (2H, s), 4.87 (2H, s), 7.34 (4H, m), 7.41 (4H, m). 13C NMR: (400 MHz, CDCl3, M4Si, δH, p.p.m.): 170.42 (C1, C2), 140.62 (C7, C12), 138.09 (C13, C18), 127.75 (C8, C11), 127.14 (C9,C10), 125.20 (C14,C17), 125.20 (C15,C16), 47.98 (C3, C4), 45.41 (C5, C6).

Refinement top

611 Friedel pairs merged since absolute configuration could not be determined reliably [Flack x parameter = -0.8 (12)]. H atoms were included in geometrically calculated positions and refined using a riding model. Their isotropic displacement parameters were set to 1.2 times the equivalent displacement parameters of their parent C atoms.

Computing details top

Data collection: SMART (Bruker, 1997-1998); cell refinement: SAINT (Bruker, 1997-1998; data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 1998); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 1990).

Figures top
[Figure 1] Fig. 1. PLEASE SUPPLY CAPTION
[Figure 2] Fig. 2. PLEASE SUPPLY CAPTION
5,6:7,8-dibenzobicyclo[2.2.2]octa-5,7-diene-2,3-dicarboxylic acid anhydride top
Crystal data top
C18H12O3F(000) = 576
Mr = 276.28Dx = 1.381 Mg m3
Monoclinic, CcMelting point: 261.3(1)° K
Hall symbol: C -2ycMo Kα radiation, λ = 0.71073 Å
a = 15.410 (2) ÅCell parameters from 1961 reflections
b = 9.4020 (12) Åθ = 2.7–28.3°
c = 11.0939 (15) ŵ = 0.09 mm1
β = 124.235 (10)°T = 293 K
V = 1328.8 (3) Å3Prism, colorless
Z = 40.6 × 0.4 × 0.32 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1289 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.035
Graphite monochromatorθmax = 28.3°, θmin = 2.7°
Detector resolution: 0.75 pixels mm-1h = 1918
ϕ and ω scansk = 712
8380 measured reflectionsl = 1414
1543 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.036Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.084H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0507P)2]
where P = (Fo2 + 2Fc2)/3
1543 reflections(Δ/σ)max < 0.001
190 parametersΔρmax = 0.12 e Å3
2 restraintsΔρmin = 0.16 e Å3
Crystal data top
C18H12O3V = 1328.8 (3) Å3
Mr = 276.28Z = 4
Monoclinic, CcMo Kα radiation
a = 15.410 (2) ŵ = 0.09 mm1
b = 9.4020 (12) ÅT = 293 K
c = 11.0939 (15) Å0.6 × 0.4 × 0.32 mm
β = 124.235 (10)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
1289 reflections with I > 2σ(I)
8380 measured reflectionsRint = 0.035
1543 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0362 restraints
wR(F2) = 0.084H-atom parameters constrained
S = 1.03Δρmax = 0.12 e Å3
1543 reflectionsΔρmin = 0.16 e Å3
190 parameters
Special details top

Experimental. Siemens SMART CCD diffractometer equipped with a normal focus, 2.4 kW sealed tube X-ray source (Mo Kα radiation, λ = 0.71073 Å) operating at 40 kV and 35 mA. The data collection covered about 1.3 hemisphere of reciprocal space by a combination of three sets of exposures; each set had a different ϕ angle (0, 90, 180 °) for the crystal and each exposure of 10 s covered 0.3° in ω to give a total of 1321 frames. The crystal-to-detector distance was 5.029 cm and the detector swing angle was -30°. Coverage of the unique set was over 99% complete. Crystal decay was monitored by repeating fifty frames from the initial set at the end of the data collection. The analysis of the duplicate reflections indicated that crystal decay was negligible.

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All e.s.d.'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) top
xyzUiso*/Ueq
O10.39685 (17)0.8228 (2)0.6917 (2)0.0847 (7)
O20.27881 (16)0.66074 (19)0.5445 (2)0.0694 (7)
O30.1388 (2)0.5462 (2)0.3630 (3)0.0962 (9)
C10.3132 (2)0.7995 (3)0.5837 (3)0.0573 (9)
C20.1805 (2)0.6570 (3)0.4147 (3)0.0623 (10)
C30.23194 (17)0.9012 (2)0.4725 (2)0.0436 (6)
C40.14307 (17)0.8055 (2)0.3580 (2)0.0459 (7)
C50.27666 (15)0.9919 (2)0.4012 (2)0.0401 (6)
C60.12639 (15)0.8282 (2)0.2075 (2)0.0431 (6)
C70.31173 (15)0.8876 (2)0.33241 (19)0.0392 (6)
C80.41146 (17)0.8754 (3)0.3617 (2)0.0501 (7)
C90.43059 (19)0.7741 (3)0.2895 (3)0.0590 (8)
C100.3514 (2)0.6849 (3)0.1888 (3)0.0593 (9)
C110.25095 (19)0.6967 (3)0.1576 (2)0.0522 (8)
C120.23125 (15)0.7989 (2)0.2291 (2)0.0402 (6)
C130.10372 (15)0.9854 (2)0.1736 (2)0.0435 (6)
C140.01505 (17)1.0439 (3)0.0520 (2)0.0557 (8)
C150.0080 (2)1.1911 (3)0.0349 (3)0.0650 (9)
C160.0876 (2)1.2770 (3)0.1383 (3)0.0626 (9)
C170.1758 (2)1.2195 (2)0.2607 (3)0.0524 (8)
C180.18434 (15)1.0732 (2)0.2781 (2)0.0417 (6)
H30.206700.963400.517500.0520*
H40.078100.825900.351300.0550*
H50.333601.055000.471600.0480*
H60.070100.768200.131300.0520*
H80.465100.935000.429600.0600*
H90.497400.765800.308700.0710*
H100.365400.616500.141400.0710*
H110.197600.636700.089700.0630*
H140.039100.985700.017300.0670*
H150.050901.231500.047000.0780*
H160.081901.375200.125700.0750*
H170.228901.278500.330800.0630*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0800 (13)0.0934 (15)0.0498 (10)0.0190 (11)0.0177 (10)0.0147 (10)
O20.0925 (14)0.0524 (11)0.0678 (11)0.0178 (9)0.0479 (11)0.0179 (8)
O30.130 (2)0.0477 (11)0.1142 (17)0.0140 (11)0.0707 (16)0.0004 (11)
C10.0703 (16)0.0626 (16)0.0434 (12)0.0130 (12)0.0347 (13)0.0105 (10)
C20.0875 (19)0.0466 (14)0.0715 (17)0.0001 (13)0.0560 (16)0.0044 (12)
C30.0536 (11)0.0447 (11)0.0366 (9)0.0073 (10)0.0279 (9)0.0003 (9)
C40.0526 (12)0.0453 (11)0.0497 (12)0.0003 (9)0.0347 (10)0.0010 (9)
C50.0443 (10)0.0359 (10)0.0355 (9)0.0015 (8)0.0196 (8)0.0023 (8)
C60.0427 (10)0.0460 (12)0.0397 (10)0.0072 (8)0.0226 (9)0.0069 (8)
C70.0445 (10)0.0384 (10)0.0375 (10)0.0033 (8)0.0248 (9)0.0046 (8)
C80.0459 (12)0.0535 (13)0.0504 (12)0.0005 (9)0.0268 (10)0.0038 (10)
C90.0562 (13)0.0707 (16)0.0650 (14)0.0140 (12)0.0432 (12)0.0104 (13)
C100.0754 (17)0.0605 (15)0.0610 (15)0.0125 (12)0.0500 (14)0.0015 (11)
C110.0677 (15)0.0497 (13)0.0472 (12)0.0026 (10)0.0372 (12)0.0065 (10)
C120.0455 (11)0.0428 (10)0.0371 (10)0.0003 (8)0.0261 (9)0.0004 (8)
C130.0442 (10)0.0536 (12)0.0383 (9)0.0042 (9)0.0266 (9)0.0024 (9)
C140.0444 (12)0.0843 (18)0.0382 (11)0.0133 (11)0.0231 (10)0.0045 (11)
C150.0684 (16)0.0870 (19)0.0488 (13)0.0391 (14)0.0386 (13)0.0258 (13)
C160.0810 (18)0.0569 (15)0.0664 (15)0.0268 (13)0.0515 (15)0.0199 (13)
C170.0674 (14)0.0434 (12)0.0584 (13)0.0092 (11)0.0427 (12)0.0053 (11)
C180.0479 (11)0.0445 (11)0.0405 (10)0.0057 (9)0.0296 (9)0.0036 (9)
Geometric parameters (Å, º) top
O1—C11.186 (4)C13—C141.384 (3)
O2—C11.383 (3)C13—C181.396 (3)
O2—C21.384 (4)C14—C151.393 (4)
O3—C21.188 (4)C15—C161.375 (4)
C1—C31.505 (4)C16—C171.381 (4)
C2—C41.506 (3)C17—C181.385 (3)
C3—C41.530 (3)C3—H30.9803
C3—C51.562 (3)C4—H40.9803
C4—C61.554 (3)C5—H50.9802
C5—C71.517 (3)C6—H60.9799
C5—C181.512 (3)C8—H80.9296
C6—C121.519 (4)C9—H90.9299
C6—C131.517 (3)C10—H100.9297
C7—C81.385 (4)C11—H110.9299
C7—C121.396 (3)C14—H140.9300
C8—C91.379 (4)C15—H150.9304
C9—C101.381 (4)C16—H160.9305
C10—C111.388 (5)C17—H170.9306
C11—C121.384 (3)
O1···C8i3.344 (3)C16···O3ix3.321 (4)
O1···C15ii3.410 (3)C8···H6iii2.9185
O1···C4iii3.373 (4)C13···H3vii2.9734
O2···C73.418 (3)C14···H10x3.0563
O2···C123.403 (3)C15···H4vii2.7959
O3···C16iv3.321 (4)C16···H9x2.9109
O1···H4iii2.7067H3···C13i2.9734
O1···H15ii2.6762H4···C15i2.7959
O2···H10v2.8490H4···O1vi2.7067
O3···H16iv2.7725H5···H82.5805
O3···H11v2.7458H5···H172.5735
C1···C123.388 (3)H6···H112.5734
C2···C73.421 (4)H6···H142.5710
C2···C113.597 (4)H6···C8vi2.9185
C2···C16i3.547 (5)H8···H52.5805
C4···C15i3.575 (4)H8···H16xi2.5983
C4···O1vi3.373 (4)H9···C16xii2.9109
C7···O23.418 (3)H10···O2xiii2.8490
C7···C23.421 (4)H10···C14xii3.0563
C8···O1vii3.344 (3)H11···H62.5734
C11···C23.597 (4)H11···O3xiii2.7458
C12···C13.388 (3)H14···H62.5710
C12···O23.403 (3)H15···O1viii2.6762
C15···C4vii3.575 (4)H16···O3ix2.7725
C15···O1viii3.410 (3)H16···H8xiv2.5983
C16···C2vii3.547 (5)H17···H52.5735
C1—O2—C2110.6 (2)C15—C16—C17120.9 (3)
O1—C1—O2119.9 (3)C16—C17—C18119.3 (2)
O1—C1—C3129.8 (3)C5—C18—C13113.37 (16)
O2—C1—C3110.3 (2)C5—C18—C17126.5 (2)
O2—C2—O3120.2 (3)C13—C18—C17120.1 (2)
O2—C2—C4110.4 (2)C1—C3—H3110.31
O3—C2—C4129.4 (3)C4—C3—H3110.32
C1—C3—C4104.49 (17)C5—C3—H3110.28
C1—C3—C5111.2 (2)C2—C4—H4110.35
C4—C3—C5110.14 (16)C3—C4—H4110.29
C2—C4—C3104.17 (18)C6—C4—H4110.31
C2—C4—C6111.64 (19)C3—C5—H5112.27
C3—C4—C6109.93 (19)C7—C5—H5112.31
C3—C5—C7106.58 (16)C18—C5—H5112.29
C3—C5—C18105.9 (2)C4—C6—H6112.26
C7—C5—C18107.03 (15)C12—C6—H6112.23
C4—C6—C12106.69 (17)C13—C6—H6112.24
C4—C6—C13106.02 (16)C7—C8—H8120.24
C12—C6—C13106.98 (19)C9—C8—H8120.26
C5—C7—C8126.72 (19)C8—C9—H9119.73
C5—C7—C12113.3 (2)C10—C9—H9119.67
C8—C7—C12119.9 (2)C9—C10—H10119.81
C7—C8—C9119.5 (2)C11—C10—H10119.70
C8—C9—C10120.6 (3)C10—C11—H11120.49
C9—C10—C11120.5 (3)C12—C11—H11120.42
C10—C11—C12119.1 (2)C13—C14—H14120.44
C6—C12—C7113.33 (18)C15—C14—H14120.47
C6—C12—C11126.3 (2)C14—C15—H15119.81
C7—C12—C11120.4 (2)C16—C15—H15119.82
C6—C13—C14126.3 (2)C15—C16—H16119.54
C6—C13—C18113.40 (17)C17—C16—H16119.58
C14—C13—C18120.26 (19)C16—C17—H17120.31
C13—C14—C15119.1 (2)C18—C17—H17120.37
C14—C15—C16120.4 (3)
C2—O2—C1—O1179.1 (3)C7—C5—C18—C17124.1 (3)
C2—O2—C1—C30.3 (4)C4—C6—C12—C759.4 (2)
C1—O2—C2—O3179.1 (3)C4—C6—C12—C11120.6 (2)
C1—O2—C2—C40.2 (4)C13—C6—C12—C753.7 (2)
O1—C1—C3—C4178.7 (4)C13—C6—C12—C11126.3 (2)
O1—C1—C3—C559.9 (4)C4—C6—C13—C14122.3 (3)
O2—C1—C3—C40.7 (3)C4—C6—C13—C1859.1 (3)
O2—C1—C3—C5119.5 (2)C12—C6—C13—C14124.1 (3)
O2—C2—C4—C30.6 (3)C12—C6—C13—C1854.4 (2)
O2—C2—C4—C6117.9 (3)C5—C7—C8—C9179.8 (2)
O3—C2—C4—C3179.4 (4)C12—C7—C8—C90.8 (3)
O3—C2—C4—C660.8 (5)C5—C7—C12—C60.8 (2)
C1—C3—C4—C20.8 (3)C5—C7—C12—C11179.30 (18)
C1—C3—C4—C6119.0 (2)C8—C7—C12—C6178.68 (18)
C5—C3—C4—C2120.3 (2)C8—C7—C12—C111.3 (3)
C5—C3—C4—C60.5 (3)C7—C8—C9—C100.1 (4)
C1—C3—C5—C758.3 (2)C8—C9—C10—C110.6 (4)
C1—C3—C5—C18172.10 (17)C9—C10—C11—C120.2 (4)
C4—C3—C5—C757.0 (2)C10—C11—C12—C6179.2 (2)
C4—C3—C5—C1856.8 (2)C10—C11—C12—C70.8 (3)
C2—C4—C6—C1258.7 (3)C6—C13—C14—C15177.8 (3)
C2—C4—C6—C13172.4 (2)C18—C13—C14—C150.6 (4)
C3—C4—C6—C1256.4 (2)C6—C13—C18—C50.4 (3)
C3—C4—C6—C1357.3 (2)C6—C13—C18—C17178.8 (2)
C3—C5—C7—C8122.5 (2)C14—C13—C18—C5178.2 (2)
C3—C5—C7—C1258.1 (2)C14—C13—C18—C170.2 (4)
C18—C5—C7—C8124.5 (2)C13—C14—C15—C160.7 (5)
C18—C5—C7—C1254.9 (2)C14—C15—C16—C170.0 (5)
C3—C5—C18—C1359.3 (2)C15—C16—C17—C180.8 (5)
C3—C5—C18—C17122.5 (3)C16—C17—C18—C5177.3 (3)
C7—C5—C18—C1354.2 (3)C16—C17—C18—C130.9 (4)
Symmetry codes: (i) x, y+2, z+1/2; (ii) x+1/2, y1/2, z+1; (iii) x+1/2, y+3/2, z+1/2; (iv) x, y1, z; (v) x, y+1, z+1/2; (vi) x1/2, y+3/2, z1/2; (vii) x, y+2, z1/2; (viii) x1/2, y+1/2, z1; (ix) x, y+1, z; (x) x1/2, y+1/2, z; (xi) x+1/2, y+5/2, z+1/2; (xii) x+1/2, y1/2, z; (xiii) x, y+1, z1/2; (xiv) x1/2, y+5/2, z1/2.

Experimental details

Crystal data
Chemical formulaC18H12O3
Mr276.28
Crystal system, space groupMonoclinic, Cc
Temperature (K)293
a, b, c (Å)15.410 (2), 9.4020 (12), 11.0939 (15)
β (°) 124.235 (10)
V3)1328.8 (3)
Z4
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.6 × 0.4 × 0.32
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
8380, 1543, 1289
Rint0.035
(sin θ/λ)max1)0.667
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.036, 0.084, 1.03
No. of reflections1543
No. of parameters190
No. of restraints2
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.12, 0.16

Computer programs: SMART (Bruker, 1997-1998), SAINT (Bruker, 1997-1998, SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg, 1998), SHELXL97 and PLATON (Spek, 1990).

Selected geometric parameters (Å, º) top
O1—C11.186 (4)C7—C81.385 (4)
O2—C11.383 (3)C7—C121.396 (3)
O2—C21.384 (4)C8—C91.379 (4)
O3—C21.188 (4)C9—C101.381 (4)
C1—C31.505 (4)C10—C111.388 (5)
C2—C41.506 (3)C11—C121.384 (3)
C3—C41.530 (3)C13—C141.384 (3)
C3—C51.562 (3)C13—C181.396 (3)
C4—C61.554 (3)C14—C151.393 (4)
C5—C71.517 (3)C15—C161.375 (4)
C5—C181.512 (3)C16—C171.381 (4)
C6—C121.519 (4)C17—C181.385 (3)
C6—C131.517 (3)
C1—O2—C2110.6 (2)C5—C7—C12113.3 (2)
O1—C1—O2119.9 (3)C8—C7—C12119.9 (2)
O1—C1—C3129.8 (3)C7—C8—C9119.5 (2)
O2—C1—C3110.3 (2)C8—C9—C10120.6 (3)
O2—C2—O3120.2 (3)C9—C10—C11120.5 (3)
O2—C2—C4110.4 (2)C10—C11—C12119.1 (2)
O3—C2—C4129.4 (3)C6—C12—C7113.33 (18)
C1—C3—C4104.49 (17)C6—C12—C11126.3 (2)
C1—C3—C5111.2 (2)C7—C12—C11120.4 (2)
C4—C3—C5110.14 (16)C6—C13—C14126.3 (2)
C2—C4—C3104.17 (18)C6—C13—C18113.40 (17)
C2—C4—C6111.64 (19)C14—C13—C18120.26 (19)
C3—C4—C6109.93 (19)C13—C14—C15119.1 (2)
C3—C5—C7106.58 (16)C14—C15—C16120.4 (3)
C3—C5—C18105.9 (2)C15—C16—C17120.9 (3)
C7—C5—C18107.03 (15)C16—C17—C18119.3 (2)
C4—C6—C12106.69 (17)C5—C18—C13113.37 (16)
C4—C6—C13106.02 (16)C5—C18—C17126.5 (2)
C12—C6—C13106.98 (19)C13—C18—C17120.1 (2)
C5—C7—C8126.72 (19)
 

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