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In the crystal structure of the title compound, C19H22O5, intermolecular hydrogen bonding gives rise to centrosymmetric dimers. The conformations of the title compound and its benzene solvate are compared.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804008578/lh6198sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804008578/lh6198Isup2.hkl
Contains datablock I

CCDC reference: 239257

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.034
  • wR factor = 0.107
  • Data-to-parameter ratio = 12.2

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT027_ALERT_3_B _diffrn_reflns_theta_full (too) Low ............ 24.98 Deg.
Alert level C PLAT155_ALERT_4_C The Triclinic Unitcell is NOT Reduced .......... ? PLAT156_ALERT_4_C Axial System Input Cell not Standard ........... ? PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.26 Ratio PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 1 C19 H22 O5
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: TEXRAY (Molecular Structure Corporation, 1985); cell refinement: TEXRAY; data reduction: TEXRAY; program(s) used to solve structure: MITHRIL (Gilmore, 1984); program(s) used to refine structure: SHELXTL (Bruker, 2001); molecular graphics: DIAMOND (Brandenburg, 2001); software used to prepare material for publication: SHELXTL.

(Z)-2,3-bis(3,4-dimethoxyphenyl)-2-propen-1-ol top
Crystal data top
C19H22O5Z = 2
Mr = 330.37F(000) = 352
Triclinic, P1Dx = 1.288 Mg m3
Hall symbol: -P 1Melting point = 403–404 K
a = 10.097 (2) ÅMo Kα radiation, λ = 0.71069 Å
b = 10.358 (2) ÅCell parameters from 25 reflections
c = 8.665 (2) Åθ = 7.0–22.9°
α = 103.08 (2)°µ = 0.09 mm1
β = 101.93 (2)°T = 295 K
γ = 78.10 (2)°Prism, colourless
V = 851.5 (3) Å30.34 × 0.23 × 0.18 mm
Data collection top
Rigaku AFC6
diffractometer
Rint = 0.025
Radiation source: normal-focus rotating anodeθmax = 25.0°, θmin = 2.1°
Graphite monochromatorh = 011
2θω scansk = 1212
3180 measured reflectionsl = 1010
2993 independent reflections3 standard reflections every 150 reflections
1665 reflections with I > 2σ(I) intensity decay: none
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)] = 0.034H-atom parameters constrained
wR(F2) = 0.107 w = 1/[σ2(Fo2) + (0.0356P)2 + 0.1258P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
2993 reflectionsΔρmax = 0.16 e Å3
245 parametersΔρmin = 0.15 e Å3
0 restraintsExtinction correction: SHELXTL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.013 (3)
Special details top

Experimental. Data were collected at room temperature using a Rigaku AFC6R diffractometer. The data were collected using 2θ-ω-scan. Scans of (1.26 + 0.30tanθ) were made at a speed of 4.0ο/min in ω. The weak reflections (I<10.0σI) were rescanned (maximum 3 rescans) and the counts were accumulated to assure good counting statistics. Stationary bacground counts were recored on each side of the reflection·The ratio of peak counting time to backgroud counting time was 2:1. The crystal–to–detector distance was 400 mm.

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
C10.9087 (2)0.4994 (2)0.7537 (2)0.0353 (5)
C20.8311 (2)0.5249 (2)0.8571 (2)0.0373 (5)
H20.75390.46330.88230.038 (6)*
C30.8674 (2)0.6397 (2)0.9222 (2)0.0365 (5)
C40.9853 (2)0.7318 (2)0.8870 (2)0.0368 (5)
C51.0628 (2)0.7060 (2)0.7879 (2)0.0400 (5)
H51.14110.76650.76430.041 (6)*
C61.0252 (2)0.5907 (2)0.7231 (2)0.0396 (5)
H61.07970.57440.65750.045 (6)*
C70.8712 (2)0.3798 (2)0.6796 (2)0.0386 (5)
H70.94470.34390.66740.041 (6)*
C80.7468 (2)0.3148 (2)0.6271 (2)0.0379 (5)
C90.6743 (2)0.5822 (3)1.0555 (3)0.0573 (7)
H9A0.69620.49671.11400.062 (8)*
H9B0.62860.61901.11810.067 (8)*
H9C0.61520.57080.95570.059 (7)*
C101.1345 (3)0.9351 (3)0.9281 (4)0.0639 (8)
H10A1.13150.96670.81460.077 (9)*
H10B1.14191.00990.97940.072 (8)*
H10C1.21250.89070.97150.083 (10)*
C110.7345 (2)0.1897 (2)0.5624 (2)0.0360 (5)
C120.6366 (2)0.1632 (2)0.4271 (2)0.0377 (5)
H120.57620.22310.37870.042 (6)*
C130.6288 (2)0.0499 (2)0.3652 (2)0.0367 (5)
C140.7168 (2)0.0425 (2)0.4392 (2)0.0387 (5)
C150.8126 (2)0.0182 (2)0.5723 (3)0.0451 (6)
H150.87170.07910.62180.047 (6)*
C160.8209 (2)0.0976 (2)0.6328 (2)0.0426 (6)
H160.88610.11300.72260.043 (6)*
C170.4600 (3)0.1159 (3)0.1388 (3)0.0578 (7)
H17A0.51950.19940.10960.070 (8)*
H17B0.40930.08570.04330.067 (7)*
H17C0.39730.12890.20130.079 (9)*
C180.7894 (3)0.2468 (3)0.4374 (4)0.0682 (8)
H18A0.77710.28510.54630.116 (13)*
H18B0.76960.31680.37580.083 (9)*
H18C0.88250.20210.43590.095 (11)*
C190.6162 (2)0.3603 (2)0.6334 (3)0.0513 (6)
H19A0.54830.34030.54120.047 (6)*
H19B0.63380.45690.62620.054 (7)*
O10.79704 (15)0.67112 (15)1.02396 (19)0.0504 (4)
O21.01262 (15)0.84333 (15)0.95593 (18)0.0488 (4)
O30.54010 (16)0.01772 (15)0.23126 (18)0.0493 (4)
O40.69887 (16)0.15257 (15)0.36958 (18)0.0488 (4)
O50.56207 (18)0.2974 (2)0.7766 (2)0.0692 (6)
H5A0.51260.22590.76360.124 (14)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0381 (12)0.0357 (12)0.0340 (11)0.0066 (10)0.0080 (9)0.0087 (9)
C20.0361 (12)0.0375 (12)0.0397 (12)0.0010 (10)0.0106 (10)0.0111 (10)
C30.0376 (12)0.0421 (13)0.0333 (11)0.0078 (10)0.0093 (9)0.0103 (10)
C40.0397 (12)0.0357 (12)0.0361 (11)0.0037 (10)0.0064 (10)0.0117 (10)
C50.0355 (12)0.0446 (13)0.0389 (12)0.0038 (10)0.0121 (10)0.0104 (10)
C60.0379 (12)0.0480 (13)0.0361 (12)0.0057 (11)0.0103 (10)0.0122 (10)
C70.0410 (13)0.0408 (13)0.0384 (12)0.0088 (10)0.0108 (10)0.0111 (10)
C80.0401 (13)0.0410 (12)0.0343 (11)0.0063 (10)0.0097 (9)0.0077 (10)
C90.0435 (14)0.0715 (19)0.0662 (17)0.0016 (13)0.0253 (13)0.0249 (15)
C100.0635 (19)0.0565 (16)0.077 (2)0.0169 (15)0.0253 (15)0.0349 (15)
C110.0375 (12)0.0364 (12)0.0362 (11)0.0013 (10)0.0121 (10)0.0104 (10)
C120.0343 (12)0.0392 (13)0.0404 (12)0.0066 (10)0.0074 (10)0.0081 (10)
C130.0327 (12)0.0384 (12)0.0378 (12)0.0032 (10)0.0064 (9)0.0128 (10)
C140.0407 (13)0.0345 (12)0.0419 (12)0.0007 (10)0.0115 (10)0.0116 (10)
C150.0478 (14)0.0418 (13)0.0449 (13)0.0104 (12)0.0019 (11)0.0092 (11)
C160.0463 (13)0.0460 (13)0.0351 (12)0.0052 (11)0.0020 (11)0.0137 (10)
C170.0500 (15)0.0646 (18)0.0564 (15)0.0124 (14)0.0102 (13)0.0217 (14)
C180.079 (2)0.0488 (15)0.081 (2)0.0245 (16)0.0101 (16)0.0293 (15)
C190.0438 (14)0.0571 (16)0.0621 (16)0.0098 (12)0.0041 (12)0.0328 (13)
O10.0462 (9)0.0563 (10)0.0599 (10)0.0015 (8)0.0244 (8)0.0289 (8)
O20.0485 (10)0.0454 (9)0.0570 (10)0.0063 (8)0.0172 (8)0.0244 (8)
O30.0479 (9)0.0502 (10)0.0486 (9)0.0075 (8)0.0070 (8)0.0214 (8)
O40.0530 (10)0.0377 (9)0.0576 (10)0.0078 (8)0.0006 (8)0.0208 (8)
O50.0539 (11)0.0836 (14)0.0872 (14)0.0157 (11)0.0366 (10)0.0532 (12)
Geometric parameters (Å, º) top
C1—C61.381 (3)C11—C161.380 (3)
C1—C21.403 (3)C11—C121.408 (3)
C1—C71.468 (3)C12—C131.379 (3)
C2—C31.380 (3)C12—H120.9300
C2—H20.9300C13—O31.372 (2)
C3—O11.368 (2)C13—C141.398 (3)
C3—C41.404 (3)C14—O41.371 (2)
C4—O21.371 (2)C14—C151.378 (3)
C4—C51.374 (3)C15—C161.395 (3)
C5—C61.383 (3)C15—H150.9300
C5—H50.9300C16—H160.9300
C6—H60.9300C17—O31.426 (3)
C7—C81.338 (3)C17—H17A0.9600
C7—H70.9300C17—H17B0.9600
C8—C111.497 (3)C17—H17C0.9600
C8—C191.504 (3)C18—O41.421 (3)
C9—O11.419 (3)C18—H18A0.9600
C9—H9A0.9600C18—H18B0.9600
C9—H9B0.9600C18—H18C0.9600
C9—H9C0.9600C19—O51.425 (3)
C10—O21.418 (3)C19—H19A0.9700
C10—H10A0.9600C19—H19B0.9700
C10—H10B0.9600O5—H5A0.8200
C10—H10C0.9600
C6—C1—C2117.84 (18)C13—C12—C11121.1 (2)
C6—C1—C7119.59 (19)C13—C12—H12119.5
C2—C1—C7122.57 (19)C11—C12—H12119.5
C3—C2—C1121.24 (19)O3—C13—C12125.3 (2)
C3—C2—H2119.4O3—C13—C14114.73 (17)
C1—C2—H2119.4C12—C13—C14120.00 (19)
O1—C3—C2124.51 (19)O4—C14—C15125.2 (2)
O1—C3—C4115.85 (17)O4—C14—C13115.22 (18)
C2—C3—C4119.63 (19)C15—C14—C13119.58 (19)
O2—C4—C5125.15 (19)C14—C15—C16120.0 (2)
O2—C4—C3115.56 (18)C14—C15—H15120.0
C5—C4—C3119.29 (18)C16—C15—H15120.0
C4—C5—C6120.5 (2)C11—C16—C15121.4 (2)
C4—C5—H5119.7C11—C16—H16119.3
C6—C5—H5119.7C15—C16—H16119.3
C1—C6—C5121.4 (2)O3—C17—H17A109.5
C1—C6—H6119.3O3—C17—H17B109.5
C5—C6—H6119.3H17A—C17—H17B109.5
C8—C7—C1129.5 (2)O3—C17—H17C109.5
C8—C7—H7115.2H17A—C17—H17C109.5
C1—C7—H7115.2H17B—C17—H17C109.5
C7—C8—C11119.7 (2)O4—C18—H18A109.5
C7—C8—C19122.69 (19)O4—C18—H18B109.5
C11—C8—C19117.62 (19)H18A—C18—H18B109.5
O1—C9—H9A109.5O4—C18—H18C109.5
O1—C9—H9B109.5H18A—C18—H18C109.5
H9A—C9—H9B109.5H18B—C18—H18C109.5
O1—C9—H9C109.5O5—C19—C8112.7 (2)
H9A—C9—H9C109.5O5—C19—H19A109.1
H9B—C9—H9C109.5C8—C19—H19A109.1
O2—C10—H10A109.5O5—C19—H19B109.1
O2—C10—H10B109.5C8—C19—H19B109.1
H10A—C10—H10B109.5H19A—C19—H19B107.8
O2—C10—H10C109.5C3—O1—C9116.66 (17)
H10A—C10—H10C109.5C4—O2—C10116.69 (17)
H10B—C10—H10C109.5C13—O3—C17117.32 (16)
C16—C11—C12117.89 (19)C14—O4—C18117.16 (18)
C16—C11—C8120.67 (18)C19—O5—H5A109.5
C12—C11—C8121.4 (2)
C6—C1—C2—C32.1 (3)C8—C11—C12—C13177.90 (19)
C7—C1—C2—C3178.6 (2)C11—C12—C13—O3177.86 (19)
C1—C2—C3—O1179.9 (2)C11—C12—C13—C141.6 (3)
C1—C2—C3—C41.2 (3)O3—C13—C14—O41.6 (3)
O1—C3—C4—O21.7 (3)C12—C13—C14—O4178.93 (18)
C2—C3—C4—O2179.50 (19)O3—C13—C14—C15178.32 (19)
O1—C3—C4—C5178.86 (19)C12—C13—C14—C151.2 (3)
C2—C3—C4—C50.0 (3)O4—C14—C15—C16179.8 (2)
O2—C4—C5—C6179.3 (2)C13—C14—C15—C160.3 (3)
C3—C4—C5—C60.1 (3)C12—C11—C16—C150.2 (3)
C2—C1—C6—C52.0 (3)C8—C11—C16—C15178.8 (2)
C7—C1—C6—C5178.7 (2)C14—C15—C16—C110.2 (3)
C4—C5—C6—C10.9 (3)C7—C8—C19—O592.6 (3)
C6—C1—C7—C8145.4 (2)C11—C8—C19—O586.0 (2)
C2—C1—C7—C835.3 (3)C2—C3—O1—C93.9 (3)
C1—C7—C8—C11177.1 (2)C4—C3—O1—C9177.4 (2)
C1—C7—C8—C191.5 (4)C5—C4—O2—C103.3 (3)
C7—C8—C11—C1638.7 (3)C3—C4—O2—C10177.3 (2)
C19—C8—C11—C16140.0 (2)C12—C13—O3—C177.2 (3)
C7—C8—C11—C12140.3 (2)C14—C13—O3—C17172.23 (19)
C19—C8—C11—C1241.1 (3)C15—C14—O4—C182.1 (3)
C16—C11—C12—C131.1 (3)C13—C14—O4—C18177.8 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O5—H5A···O3i0.822.463.226 (2)156
O5—H5A···O4i0.822.282.940 (2)138
C2—H2···O50.932.483.277 (3)144
Symmetry code: (i) x+1, y, z+1.
Selected torsion angles (°) in (I) and the benzene solvate of (I) top
compound
Torsion angle(I)Benzene solvate of (I)
C2—C1—C7—C8-35.3 (3)141.1 (3)
C1—C7—C8—C11177.1 (2)-179.2 (3)
C1—C7—C8—C19-1.5 (4)-0.7 (5)
C7—C8—C19—O592.6 (3)88.0 (3)
C12—C11—C8—C7140.3 (2)-45.3 (4)
 

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