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The title compound, 1,1',8,8'-tetra­methoxy-9,9'-bianthracene-10,10'(9H,9'H)-dione, C32H26O6, was obtained by the reduction of 1,8-di­methoxy­anthra­quinone with sodium borohydride and tri­fluoro­acetic acid. In the anthrone dimers, the methoxy and carbonyl groups are attached to opposite sides of the anthracene rings. In the solid state, the mol­ecule has a crystallographically imposed centre of symmetry located at the mid-point of the C-C bond linking the two anthracene systems.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804028168/cv6407sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804028168/cv6407Isup2.hkl
Contains datablock I

CCDC reference: 238534

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.059
  • wR factor = 0.115
  • Data-to-parameter ratio = 13.8

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SMART; data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

1,1',8,8'-tetramethoxy-9,9'-bianthracene-10,10'(9H,9'H)-dione top
Crystal data top
C32H26O6Z = 1
Mr = 506.53F(000) = 266
Triclinic, P1Dx = 1.387 Mg m3
Hall symbol: -P 1Melting point = 232–234 K
a = 7.585 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.443 (2) ÅCell parameters from 523 reflections
c = 10.631 (3) Åθ = 2.6–25.9°
α = 67.801 (4)°µ = 0.10 mm1
β = 74.187 (4)°T = 293 K
γ = 85.328 (5)°Block, white
V = 606.3 (3) Å30.32 × 0.26 × 0.24 mm
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2392 independent reflections
Radiation source: sealed tube1381 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.048
φ and ω scansθmax = 26.0°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 89
Tmin = 0.97, Tmax = 0.98k = 910
4784 measured reflectionsl = 1113
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.059H-atom parameters constrained
wR(F2) = 0.115 w = 1/[σ2(Fo2) + (0.04P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.038
2392 reflectionsΔρmax = 0.19 e Å3
173 parametersΔρmin = 0.19 e Å3
0 restraintsExtinction correction: SHELXTL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.027 (4)
Special details top

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) top
xyzUiso*/Ueq
O10.3711 (3)0.1898 (2)0.71932 (18)0.0679 (5)
O30.0207 (2)0.39447 (16)0.86225 (15)0.0494 (4)
O40.17835 (19)0.02600 (18)1.23353 (13)0.0483 (4)
C10.2722 (2)0.1191 (2)1.15674 (18)0.0371 (4)
C20.3197 (3)0.1023 (2)0.7915 (2)0.0435 (5)
C30.0320 (4)0.5676 (3)0.8113 (3)0.0654 (7)
H3A0.09480.59970.88930.098*
H3B0.11200.58040.75210.098*
H3C0.07510.63980.75800.098*
C40.3386 (2)0.1581 (2)0.93691 (19)0.0378 (4)
C60.2385 (2)0.0762 (2)1.02504 (17)0.0320 (4)
C70.3934 (3)0.2462 (2)1.2007 (2)0.0483 (5)
H7A0.41240.27611.28960.058*
C80.1539 (2)0.1518 (2)0.82388 (17)0.0328 (4)
C100.1113 (2)0.3233 (2)0.7672 (2)0.0408 (4)
C130.0951 (2)0.04904 (19)0.97971 (16)0.0295 (3)
H13A0.07860.12791.02980.035*
C140.4608 (3)0.2847 (2)0.9817 (2)0.0502 (5)
H14A0.52540.33960.92260.060*
C170.2534 (2)0.0732 (2)0.73307 (18)0.0393 (4)
C180.4860 (3)0.3285 (3)1.1136 (3)0.0537 (5)
H18A0.56640.41471.14430.064*
C210.2608 (3)0.3308 (3)0.5345 (2)0.0640 (6)
H21A0.29500.39100.43780.077*
C230.1979 (4)0.0634 (4)1.3697 (2)0.0661 (7)
H23A0.12390.01211.41000.099*
H23B0.32410.04811.36450.099*
H23C0.15910.17981.42750.099*
C290.3045 (3)0.1649 (3)0.5872 (2)0.0512 (5)
H29A0.36850.11130.52690.061*
C310.1653 (3)0.4128 (3)0.6233 (2)0.0597 (6)
H31A0.13780.52780.58600.072*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0795 (11)0.0700 (11)0.0599 (10)0.0020 (8)0.0029 (8)0.0449 (8)
O30.0604 (9)0.0333 (7)0.0491 (8)0.0056 (6)0.0112 (7)0.0122 (5)
O40.0558 (9)0.0574 (9)0.0365 (7)0.0072 (6)0.0156 (6)0.0216 (6)
C10.0350 (9)0.0354 (8)0.0408 (9)0.0068 (7)0.0086 (7)0.0135 (7)
C20.0380 (9)0.0494 (11)0.0452 (10)0.0081 (8)0.0032 (8)0.0277 (9)
C30.0799 (16)0.0333 (10)0.0829 (17)0.0113 (10)0.0308 (14)0.0169 (11)
C40.0297 (8)0.0343 (9)0.0467 (10)0.0037 (6)0.0029 (7)0.0162 (7)
C60.0299 (8)0.0284 (8)0.0338 (8)0.0059 (6)0.0030 (6)0.0097 (6)
C70.0500 (11)0.0404 (10)0.0544 (12)0.0033 (8)0.0268 (9)0.0076 (9)
C80.0291 (8)0.0365 (8)0.0306 (8)0.0082 (6)0.0036 (6)0.0112 (6)
C100.0371 (9)0.0388 (9)0.0430 (10)0.0049 (7)0.0111 (8)0.0098 (8)
C130.0329 (8)0.0279 (7)0.0279 (8)0.0001 (6)0.0068 (6)0.0112 (6)
C140.0401 (10)0.0360 (9)0.0758 (14)0.0026 (7)0.0092 (10)0.0266 (9)
C170.0313 (8)0.0521 (11)0.0342 (9)0.0105 (8)0.0026 (7)0.0174 (8)
C180.0457 (11)0.0370 (10)0.0813 (15)0.0085 (8)0.0297 (11)0.0175 (10)
C210.0675 (14)0.0776 (16)0.0296 (10)0.0153 (12)0.0089 (10)0.0000 (10)
C230.0670 (15)0.0970 (19)0.0402 (11)0.0031 (13)0.0174 (10)0.0298 (12)
C290.0465 (11)0.0751 (14)0.0320 (9)0.0120 (10)0.0041 (8)0.0215 (9)
C310.0663 (14)0.0504 (12)0.0466 (12)0.0052 (10)0.0184 (10)0.0031 (9)
Geometric parameters (Å, º) top
O1—C21.227 (2)C8—C171.396 (2)
O3—C101.367 (2)C8—C131.507 (2)
O3—C31.419 (2)C10—C311.383 (3)
O4—C11.367 (2)C13—C13i1.594 (3)
O4—C231.407 (2)C13—H13A0.9800
C1—C71.382 (3)C14—C181.372 (3)
C1—C61.397 (2)C14—H14A0.9300
C2—C171.479 (3)C17—C291.403 (3)
C2—C41.480 (3)C18—H18A0.9300
C3—H3A0.9600C21—C291.348 (3)
C3—H3B0.9600C21—C311.391 (4)
C3—H3C0.9600C21—H21A0.9300
C4—C141.387 (3)C23—H23A0.9600
C4—C61.396 (2)C23—H23B0.9600
C6—C131.499 (2)C23—H23C0.9600
C7—C181.373 (3)C29—H29A0.9300
C7—H7A0.9300C31—H31A0.9300
C8—C101.391 (3)
C10—O3—C3118.67 (17)C6—C13—C13i110.09 (15)
C1—O4—C23119.26 (17)C8—C13—C13i110.61 (15)
O4—C1—C7124.64 (17)C6—C13—H13A108.4
O4—C1—C6114.85 (15)C8—C13—H13A108.4
C7—C1—C6120.50 (17)C13i—C13—H13A108.4
O1—C2—C17121.71 (19)C18—C14—C4119.7 (2)
O1—C2—C4122.1 (2)C18—C14—H14A120.2
C17—C2—C4115.85 (15)C4—C14—H14A120.2
O3—C3—H3A109.5C8—C17—C29120.30 (18)
O3—C3—H3B109.5C8—C17—C2119.77 (16)
H3A—C3—H3B109.5C29—C17—C2119.69 (18)
O3—C3—H3C109.5C14—C18—C7120.58 (19)
H3A—C3—H3C109.5C14—C18—H18A119.7
H3B—C3—H3C109.5C7—C18—H18A119.7
C14—C4—C6120.91 (18)C29—C21—C31120.75 (19)
C14—C4—C2119.94 (18)C29—C21—H21A119.6
C6—C4—C2119.08 (16)C31—C21—H21A119.6
C4—C6—C1118.03 (16)O4—C23—H23A109.5
C4—C6—C13120.09 (15)O4—C23—H23B109.5
C1—C6—C13121.84 (15)H23A—C23—H23B109.5
C1—C7—C18120.22 (19)O4—C23—H23C109.5
C1—C7—H7A119.9H23A—C23—H23C109.5
C18—C7—H7A119.9H23B—C23—H23C109.5
C10—C8—C17118.72 (16)C21—C29—C17119.9 (2)
C10—C8—C13121.95 (15)C21—C29—H29A120.0
C17—C8—C13119.33 (15)C17—C29—H29A120.0
O3—C10—C31123.91 (19)C21—C31—C10120.0 (2)
O3—C10—C8115.76 (16)C21—C31—H31A120.0
C31—C10—C8120.29 (19)C10—C31—H31A120.0
C6—C13—C8110.88 (13)
Symmetry code: (i) x, y, z+2.
 

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