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In the crystals of the title lignin model compound, C20H26O8, the mol­ecules adopt a conformation in which the bulky 2,6-di­methoxy­phenoxy and 3,4,5-tri­methoxy­phenyl groups are distant from each other. The O(phenoxy)-C-C-C(phenyl) torsion angle between these groups is 178.58 (7)°. The hydrogen-bonding pattern is discussed in terms of graph-set theory.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536801019390/ob6090sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536801019390/ob6090Isup2.hkl
Contains datablock I

CCDC reference: 177226

Key indicators

  • Single-crystal X-ray study
  • T = 183 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.044
  • wR factor = 0.124
  • Data-to-parameter ratio = 25.9

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Computing details top

Data collection: SMART (Siemens, 1995); cell refinement: SAINT (Siemens, 1995); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 1997); program(s) used to refine structure: SHELXTL; molecular graphics: DIAMOND (Brandenburg, 2000); software used to prepare material for publication: SHELXTL.

(I) top
Crystal data top
C20H26O8Dx = 1.268 Mg m3
Mr = 394.41Melting point: 105°C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 11.7627 (2) ÅCell parameters from 8192 reflections
b = 9.6220 (2) Åθ = 1.8–32.9°
c = 18.7387 (3) ŵ = 0.10 mm1
β = 103.034 (1)°T = 183 K
V = 2066.22 (6) Å3Irregular shape, colorless
Z = 40.65 × 0.30 × 0.20 mm
F(000) = 840
Data collection top
Siemens SMART CCD
diffractometer
7394 independent reflections
Radiation source: fine-focus sealed tube5861 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.032
ω scansθmax = 32.9°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS, Sheldrick, 2001)
h = 1717
Tmin = 0.939, Tmax = 0.981k = 1414
33473 measured reflectionsl = 2727
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)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.125H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0586P)2 + 0.5426P]
where P = (Fo2 + 2Fc2)/3
7394 reflections(Δ/σ)max < 0.001
286 parametersΔρmax = 0.41 e Å3
0 restraintsΔρmin = 0.21 e Å3
Special details top

Experimental. Data were collected at 183 K using a Siemens SMART CCD diffractometer equipped with a Siemens LT-2 A low temperature device. A full sphere of reciprocal space was scanned by 0.3° steps in ω with a crystal–to–detector distance of 3.97 cm, 15 s per frame. Preliminary orientation matrix was obtained from the first 100 frames using SMART (Siemens, 1995). The collected frames were integrated using the preliminary orientation matrix which was updated every 100 frames. Final cell parameters were obtained by refinement on the position of 8192 reflections with I>10σ(I) after integration of all the frames data using SAINT (Siemens, 1995). The data were empirically corrected for absorption and other effects using SADABS (Sheldrick, 2001) based on the method of Blessing (1995).

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. The structure was solved by direct methods and refined by full-matrix least squares on all F2 data using SHELXTL (Bruker, 1997). All non-H atoms were refined anisotropically.

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
O10.00372 (7)0.26496 (8)0.25618 (4)0.02953 (17)
O20.10719 (7)0.15028 (7)0.38367 (4)0.02695 (15)
O30.29718 (7)0.27099 (8)0.46848 (4)0.03178 (17)
O40.38019 (7)0.69798 (8)0.33437 (4)0.02838 (16)
H40.40480.77080.31830.053 (5)*
O50.48713 (9)0.44577 (10)0.16854 (5)0.0444 (2)
H50.47200.50750.13610.062 (5)*
O60.39378 (6)0.71484 (7)0.18345 (4)0.02091 (13)
O70.27690 (7)0.93525 (8)0.21872 (5)0.03244 (18)
O80.36330 (8)0.62600 (9)0.04555 (4)0.03223 (18)
C10.24515 (8)0.50809 (9)0.30875 (5)0.02041 (17)
C20.14171 (8)0.45040 (10)0.26748 (5)0.02254 (18)
H20.10360.49150.22230.034 (4)*
C30.09503 (8)0.33186 (10)0.29329 (5)0.02154 (17)
C40.14994 (8)0.27274 (9)0.36096 (5)0.02125 (17)
C50.25209 (8)0.33381 (10)0.40260 (5)0.02236 (17)
C60.30055 (8)0.45055 (10)0.37606 (5)0.02256 (18)
H60.37070.49040.40370.036 (4)*
C70.04562 (11)0.30136 (15)0.18097 (6)0.0378 (3)
H7A0.07610.39650.17760.049 (4)*
H7B0.10800.23720.15820.055 (5)*
H7C0.01850.29540.15560.040 (4)*
C80.40235 (10)0.32813 (14)0.51333 (7)0.0365 (3)
H8A0.46490.32430.48660.049 (4)*
H8B0.42510.27400.55860.045 (4)*
H8C0.38870.42490.52530.049 (4)*
C90.29599 (8)0.63374 (10)0.27772 (5)0.02065 (17)
H90.23160.70170.25970.028 (3)*
C100.34869 (8)0.59131 (9)0.21281 (5)0.02028 (17)
H100.28650.54820.17380.025 (3)*
C110.45136 (10)0.49227 (12)0.23274 (6)0.0319 (2)
H11A0.51740.53970.26590.040 (4)*
H11B0.42910.41110.25910.042 (4)*
C120.31469 (8)0.78403 (10)0.12923 (5)0.02170 (17)
C130.25505 (9)0.90160 (11)0.14603 (6)0.0267 (2)
C140.17973 (11)0.97455 (13)0.08976 (7)0.0376 (3)
H140.13881.05400.10070.058 (5)*
C150.16578 (11)0.92945 (15)0.01808 (8)0.0422 (3)
H150.11470.97900.01990.059 (5)*
C160.22431 (11)0.81390 (14)0.00036 (6)0.0375 (3)
H160.21360.78500.04920.047 (4)*
C170.29933 (9)0.74021 (11)0.05620 (5)0.02623 (19)
C180.23050 (16)1.06279 (15)0.23917 (10)0.0539 (4)
H18A0.25741.14020.21320.058 (5)*
H18B0.25731.07670.29210.069 (6)*
H18C0.14511.05890.22620.058 (5)*
C190.33984 (14)0.56785 (14)0.02728 (6)0.0432 (3)
H19A0.25710.54280.04230.053 (5)*
H19B0.38780.48470.02750.061 (5)*
H19C0.35860.63660.06150.045 (4)*
C200.02895 (14)0.16976 (15)0.43106 (9)0.0464 (3)
H20A0.07020.21560.47620.076 (6)*
H20B0.00020.07930.44300.055 (5)*
H20C0.03680.22780.40650.075 (6)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0262 (3)0.0334 (4)0.0260 (3)0.0101 (3)0.0004 (3)0.0032 (3)
O20.0318 (4)0.0198 (3)0.0305 (4)0.0029 (3)0.0095 (3)0.0032 (3)
O30.0352 (4)0.0289 (4)0.0261 (4)0.0035 (3)0.0039 (3)0.0079 (3)
O40.0394 (4)0.0256 (4)0.0211 (3)0.0129 (3)0.0089 (3)0.0042 (3)
O50.0630 (6)0.0457 (5)0.0288 (4)0.0324 (5)0.0192 (4)0.0047 (4)
O60.0193 (3)0.0236 (3)0.0192 (3)0.0003 (2)0.0030 (2)0.0013 (2)
O70.0367 (4)0.0259 (4)0.0369 (4)0.0050 (3)0.0129 (3)0.0039 (3)
O80.0465 (5)0.0305 (4)0.0194 (3)0.0002 (3)0.0067 (3)0.0021 (3)
C10.0222 (4)0.0177 (4)0.0218 (4)0.0004 (3)0.0060 (3)0.0005 (3)
C20.0228 (4)0.0216 (4)0.0222 (4)0.0001 (3)0.0031 (3)0.0026 (3)
C30.0200 (4)0.0216 (4)0.0223 (4)0.0010 (3)0.0034 (3)0.0014 (3)
C40.0243 (4)0.0172 (4)0.0227 (4)0.0001 (3)0.0064 (3)0.0009 (3)
C50.0245 (4)0.0200 (4)0.0213 (4)0.0016 (3)0.0026 (3)0.0013 (3)
C60.0230 (4)0.0206 (4)0.0230 (4)0.0009 (3)0.0028 (3)0.0010 (3)
C70.0338 (6)0.0487 (7)0.0263 (5)0.0139 (5)0.0026 (4)0.0055 (5)
C80.0318 (5)0.0404 (6)0.0309 (5)0.0001 (5)0.0063 (4)0.0056 (5)
C90.0231 (4)0.0183 (4)0.0212 (4)0.0005 (3)0.0063 (3)0.0008 (3)
C100.0236 (4)0.0182 (4)0.0185 (4)0.0020 (3)0.0038 (3)0.0003 (3)
C110.0393 (6)0.0346 (5)0.0233 (5)0.0182 (5)0.0100 (4)0.0041 (4)
C120.0209 (4)0.0215 (4)0.0221 (4)0.0014 (3)0.0036 (3)0.0037 (3)
C130.0242 (4)0.0237 (4)0.0330 (5)0.0000 (3)0.0079 (4)0.0045 (4)
C140.0321 (5)0.0310 (5)0.0499 (7)0.0070 (4)0.0095 (5)0.0164 (5)
C150.0344 (6)0.0453 (7)0.0428 (7)0.0015 (5)0.0002 (5)0.0237 (6)
C160.0410 (6)0.0424 (6)0.0246 (5)0.0060 (5)0.0020 (4)0.0112 (5)
C170.0297 (5)0.0265 (5)0.0216 (4)0.0051 (4)0.0040 (3)0.0040 (3)
C180.0686 (10)0.0365 (7)0.0635 (10)0.0178 (7)0.0295 (8)0.0059 (6)
C190.0679 (9)0.0379 (6)0.0231 (5)0.0128 (6)0.0093 (5)0.0082 (5)
C200.0544 (8)0.0394 (7)0.0555 (8)0.0057 (6)0.0334 (7)0.0052 (6)
Geometric parameters (Å, º) top
O1—C31.3722 (11)C8—H8A0.9800
O1—C71.4278 (13)C8—H8B0.9800
O2—C41.3852 (11)C8—H8C0.9800
O2—C201.4281 (15)C9—C101.5396 (13)
O3—C51.3695 (12)C9—H91.0000
O3—C81.4388 (14)C10—C111.5175 (13)
O4—C91.4198 (11)C10—H101.0000
O4—H40.8400C11—H11A0.9900
O5—C111.4326 (13)C11—H11B0.9900
O5—H50.8400C12—C171.4040 (14)
O6—C121.3837 (11)C12—C131.4039 (14)
O6—C101.4589 (11)C13—C141.4028 (15)
O7—C131.3668 (14)C14—C151.386 (2)
O7—C181.4301 (15)C14—H140.9500
O8—C171.3717 (14)C15—C161.387 (2)
O8—C191.4430 (13)C15—H150.9500
C1—C61.3969 (13)C16—C171.4000 (15)
C1—C21.4007 (13)C16—H160.9500
C1—C91.5213 (13)C18—H18A0.9800
C2—C31.3986 (13)C18—H18B0.9800
C2—H20.9500C18—H18C0.9800
C3—C41.4068 (13)C19—H19A0.9800
C4—C51.4053 (13)C19—H19B0.9800
C5—C61.4007 (13)C19—H19C0.9800
C6—H60.9500C20—H20A0.9800
C7—H7A0.9800C20—H20B0.9800
C7—H7B0.9800C20—H20C0.9800
C7—H7C0.9800
C3—O1—C7116.71 (8)C11—C10—C9114.34 (8)
C4—O2—C20114.14 (9)O6—C10—H10109.2
C5—O3—C8117.72 (9)C11—C10—H10109.2
C9—O4—H4109.5C9—C10—H10109.2
C11—O5—H5109.5O5—C11—C10110.96 (8)
C12—O6—C10115.31 (7)O5—C11—H11A109.4
C13—O7—C18118.23 (10)C10—C11—H11A109.4
C17—O8—C19117.01 (9)O5—C11—H11B109.4
C6—C1—C2120.78 (9)C10—C11—H11B109.4
C6—C1—C9121.10 (8)H11A—C11—H11B108.0
C2—C1—C9118.12 (8)O6—C12—C17119.24 (9)
C1—C2—C3119.48 (9)O6—C12—C13120.69 (9)
C1—C2—H2120.3C17—C12—C13119.97 (9)
C3—C2—H2120.3O7—C13—C12115.03 (9)
O1—C3—C2124.11 (9)O7—C13—C14125.13 (10)
O1—C3—C4115.55 (8)C12—C13—C14119.83 (10)
C2—C3—C4120.34 (8)C13—C14—C15119.25 (11)
O2—C4—C3119.74 (8)C13—C14—H14120.4
O2—C4—C5120.62 (8)C15—C14—H14120.4
C3—C4—C5119.51 (9)C16—C15—C14121.77 (11)
O3—C5—C6124.62 (9)C16—C15—H15119.1
O3—C5—C4115.14 (8)C14—C15—H15119.1
C6—C5—C4120.25 (9)C15—C16—C17119.36 (11)
C1—C6—C5119.60 (9)C15—C16—H16120.3
C1—C6—H6120.2C17—C16—H16120.3
C5—C6—H6120.2O8—C17—C12115.35 (9)
O1—C7—H7A109.5O8—C17—C16124.82 (10)
O1—C7—H7B109.5C12—C17—C16119.82 (11)
H7A—C7—H7B109.5O7—C18—H18A109.5
O1—C7—H7C109.5O7—C18—H18B109.5
H7A—C7—H7C109.5H18A—C18—H18B109.5
H7B—C7—H7C109.5O7—C18—H18C109.5
O3—C8—H8A109.5H18A—C18—H18C109.5
O3—C8—H8B109.5H18B—C18—H18C109.5
H8A—C8—H8B109.5O8—C19—H19A109.5
O3—C8—H8C109.5O8—C19—H19B109.5
H8A—C8—H8C109.5H19A—C19—H19B109.5
H8B—C8—H8C109.5O8—C19—H19C109.5
O4—C9—C1109.16 (7)H19A—C19—H19C109.5
O4—C9—C10111.65 (8)H19B—C19—H19C109.5
C1—C9—C10110.75 (7)O2—C20—H20A109.5
O4—C9—H9108.4O2—C20—H20B109.5
C1—C9—H9108.4H20A—C20—H20B109.5
C10—C9—H9108.4O2—C20—H20C109.5
O6—C10—C11105.52 (8)H20A—C20—H20C109.5
O6—C10—C9109.11 (7)H20B—C20—H20C109.5
C6—C1—C2—C31.51 (14)C12—O6—C10—C989.24 (9)
C9—C1—C2—C3177.73 (8)O4—C9—C10—O659.56 (9)
C7—O1—C3—C213.75 (15)C1—C9—C10—O6178.58 (7)
C7—O1—C3—C4165.75 (10)O4—C9—C10—C1158.31 (11)
C1—C2—C3—O1178.02 (9)C1—C9—C10—C1163.55 (11)
C1—C2—C3—C41.46 (14)O6—C10—C11—O566.51 (11)
C20—O2—C4—C395.46 (12)C9—C10—C11—O5173.58 (9)
C20—O2—C4—C588.67 (12)C10—O6—C12—C1785.36 (10)
O1—C3—C4—O23.71 (13)C10—O6—C12—C1398.22 (10)
C2—C3—C4—O2175.81 (9)C18—O7—C13—C12172.64 (11)
O1—C3—C4—C5179.62 (9)C18—O7—C13—C147.40 (17)
C2—C3—C4—C50.10 (14)O6—C12—C13—O73.30 (13)
C8—O3—C5—C60.60 (15)C17—C12—C13—O7179.69 (9)
C8—O3—C5—C4179.48 (10)O6—C12—C13—C14176.73 (9)
O2—C4—C5—O35.83 (13)C17—C12—C13—C140.34 (15)
C3—C4—C5—O3178.29 (9)O7—C13—C14—C15179.74 (11)
O2—C4—C5—C6174.24 (8)C12—C13—C14—C150.29 (17)
C3—C4—C5—C61.63 (14)C13—C14—C15—C160.02 (19)
C2—C1—C6—C50.00 (14)C14—C15—C16—C170.21 (19)
C9—C1—C6—C5179.23 (8)C19—O8—C17—C12172.90 (10)
O3—C5—C6—C1178.33 (9)C19—O8—C17—C168.29 (16)
C4—C5—C6—C11.58 (14)O6—C12—C17—O82.31 (13)
C6—C1—C9—O416.15 (12)C13—C12—C17—O8178.76 (9)
C2—C1—C9—O4164.61 (8)O6—C12—C17—C16176.56 (9)
C6—C1—C9—C10107.16 (10)C13—C12—C17—C160.11 (15)
C2—C1—C9—C1072.08 (10)C15—C16—C17—O8178.91 (10)
C12—O6—C10—C11147.47 (8)C15—C16—C17—C120.16 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O4—H4···O5i0.842.092.8569 (11)152
O4—H4···O60.842.562.8731 (10)104
O4—H4···O70.842.643.1934 (12)125
O5—H5···O60.842.452.8504 (11)110
O5—H5···O80.842.202.9876 (12)157
C6—H6···O40.952.402.7360 (12)101
C9—H9···O71.002.473.0947 (12)120
C11—H11A···O7ii0.992.583.1676 (14)118
C19—H19C···O4iii0.982.583.5465 (15)171
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+1, y1/2, z+1/2; (iii) x, y+3/2, z1/2.
 

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