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The title compound, C18H16O3, (I), was prepared in the course of studies towards the synthesis of furo­furan ligands and was reported previously [Brown & Hinks (1998). Chem. Commun. pp. 1895-1896]. The compound is a a model system, where both oxy­genated aromatic rings that are present in the natural products have been substituted by a simple phenyl group.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536801008170/cv6025sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536801008170/cv6025Isup2.hkl
Contains datablock I

CCDC reference: 170753

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.051
  • wR factor = 0.109
  • Data-to-parameter ratio = 12.0

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Comment top

NO COMMENT

Experimental top

The furofuranone was recrystallized from Et2O/hexanes as colourless crystals.

Computing details top

Data collection: DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998); cell refinement: DENZO and COLLECT; data reduction: DENZO and COLLECT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 1990).

Figures top
[Figure 1] Fig. 1. The structure of (I) showing 50% probability displacement ellipsoids.
(1S*,4S*,5R*,8R*)-4,8-Diphenyl-3,7-dioxabicyclo[3.3.0]octan-2-one top
Crystal data top
C18H16O3F(000) = 1184
Mr = 280.31Dx = 1.342 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 21.416 (1) ÅCell parameters from 8593 reflections
b = 7.520 (1) Åθ = 2.9–25.2°
c = 19.487 (1) ŵ = 0.09 mm1
β = 117.86 (1)°T = 150 K
V = 2774.7 (3) Å3Block, colourless
Z = 80.30 × 0.20 × 0.15 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
2489 independent reflections
Radiation source: Nonius FR591 rotating anode1822 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.067
ϕ and ω scans to fill Ewald sphereθmax = 25.3°, θmin = 2.9°
Absorption correction: multi-scan
(Blessing, 1997)
h = 2425
Tmin = 0.973, Tmax = 0.987k = 98
7164 measured reflectionsl = 2323
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)] = 0.051H-atom parameters constrained
wR(F2) = 0.109 w = 1/[σ2(Fo2) + (0.0009P)2 + 5.P]
where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max = 0.003
2489 reflectionsΔρmax = 0.25 e Å3
207 parametersΔρmin = 0.22 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0062 (5)
Crystal data top
C18H16O3V = 2774.7 (3) Å3
Mr = 280.31Z = 8
Monoclinic, C2/cMo Kα radiation
a = 21.416 (1) ŵ = 0.09 mm1
b = 7.520 (1) ÅT = 150 K
c = 19.487 (1) Å0.30 × 0.20 × 0.15 mm
β = 117.86 (1)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
2489 independent reflections
Absorption correction: multi-scan
(Blessing, 1997)
1822 reflections with I > 2σ(I)
Tmin = 0.973, Tmax = 0.987Rint = 0.067
7164 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0510 restraints
wR(F2) = 0.109H-atom parameters constrained
S = 0.97Δρmax = 0.25 e Å3
2489 reflectionsΔρmin = 0.22 e Å3
207 parameters
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
O10.07450 (7)0.2916 (2)0.34285 (9)0.0348 (4)
O20.22067 (7)0.0174 (2)0.46476 (9)0.0354 (4)
O30.00184 (7)0.0704 (2)0.33285 (9)0.0382 (4)
C10.05818 (11)0.1159 (3)0.33989 (12)0.0302 (5)
C20.11744 (11)0.0022 (3)0.34348 (13)0.0315 (5)
H20.09980.08230.29870.046 (7)*
C30.17074 (10)0.1339 (3)0.33991 (13)0.0312 (5)
H30.17200.12870.28930.037 (6)*
C40.14588 (10)0.3167 (3)0.35418 (13)0.0302 (5)
H40.17670.35110.40950.023 (5)*
C50.16173 (10)0.0976 (3)0.42139 (13)0.0315 (5)
H50.18050.20860.40940.028 (5)*
C60.24032 (11)0.0813 (3)0.40766 (14)0.0371 (6)
H6A0.26370.01330.39260.044 (7)*
H6B0.27250.18470.42760.040 (6)*
C70.08997 (11)0.5192 (3)0.23582 (13)0.0350 (6)
H70.04520.46610.22100.042 (6)*
C80.09694 (12)0.6527 (3)0.19024 (14)0.0409 (6)
H80.05670.69210.14480.044 (7)*
C90.16205 (12)0.7277 (3)0.21082 (15)0.0410 (6)
H90.16660.81670.17880.042 (6)*
C100.22031 (12)0.6746 (3)0.27718 (15)0.0396 (6)
H100.26510.72690.29130.042 (6)*
C110.21346 (11)0.5436 (3)0.32364 (14)0.0360 (6)
H110.25360.50820.37010.034 (6)*
C120.14846 (11)0.4642 (3)0.30268 (13)0.0299 (5)
C130.11114 (11)0.3256 (3)0.47345 (15)0.0408 (6)
H130.12170.41130.44450.050 (7)*
C140.08009 (13)0.3801 (3)0.51884 (17)0.0519 (7)
H140.06990.50220.52120.076 (9)*
C150.06434 (12)0.2559 (3)0.56027 (15)0.0451 (6)
H150.04350.29230.59160.063 (8)*
C160.07874 (11)0.0796 (3)0.55638 (13)0.0392 (6)
H160.06740.00570.58480.065 (8)*
C170.10979 (11)0.0244 (3)0.51127 (13)0.0337 (5)
H170.11940.09810.50870.038 (6)*
C180.12677 (10)0.1495 (3)0.46991 (12)0.0296 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0270 (8)0.0444 (9)0.0465 (10)0.0046 (7)0.0283 (8)0.0013 (7)
O20.0220 (8)0.0508 (10)0.0411 (10)0.0004 (7)0.0212 (7)0.0031 (7)
O30.0243 (8)0.0625 (11)0.0359 (9)0.0014 (7)0.0207 (7)0.0014 (8)
C10.0246 (11)0.0493 (14)0.0230 (12)0.0006 (10)0.0163 (10)0.0008 (10)
C20.0278 (11)0.0422 (13)0.0348 (13)0.0013 (9)0.0234 (10)0.0050 (10)
C30.0285 (12)0.0399 (12)0.0387 (13)0.0015 (9)0.0269 (11)0.0023 (10)
C40.0228 (11)0.0424 (13)0.0327 (13)0.0013 (9)0.0192 (10)0.0041 (10)
C50.0238 (11)0.0390 (13)0.0409 (13)0.0017 (9)0.0227 (10)0.0020 (10)
C60.0279 (12)0.0450 (14)0.0533 (16)0.0044 (10)0.0313 (12)0.0052 (11)
C70.0278 (12)0.0402 (13)0.0419 (14)0.0050 (10)0.0203 (11)0.0033 (10)
C80.0367 (14)0.0466 (14)0.0395 (15)0.0004 (11)0.0179 (12)0.0020 (11)
C90.0439 (15)0.0425 (14)0.0526 (16)0.0018 (11)0.0358 (14)0.0006 (12)
C100.0315 (13)0.0448 (14)0.0566 (17)0.0054 (10)0.0323 (13)0.0075 (12)
C110.0243 (12)0.0481 (14)0.0417 (14)0.0032 (10)0.0205 (11)0.0023 (11)
C120.0271 (11)0.0355 (12)0.0380 (13)0.0002 (9)0.0242 (11)0.0062 (10)
C130.0369 (13)0.0411 (14)0.0598 (17)0.0092 (10)0.0355 (13)0.0052 (11)
C140.0507 (16)0.0444 (16)0.082 (2)0.0097 (12)0.0494 (16)0.0166 (14)
C150.0364 (14)0.0622 (17)0.0509 (16)0.0089 (12)0.0324 (13)0.0129 (13)
C160.0245 (12)0.0631 (16)0.0375 (14)0.0006 (11)0.0207 (11)0.0058 (12)
C170.0252 (11)0.0439 (14)0.0385 (14)0.0022 (10)0.0202 (11)0.0053 (10)
C180.0191 (10)0.0397 (13)0.0346 (13)0.0055 (9)0.0163 (10)0.0021 (10)
Geometric parameters (Å, º) top
O1—C11.361 (3)C7—H70.9500
O1—C41.451 (2)C8—C91.379 (3)
O2—C51.435 (2)C8—H80.9500
O2—C61.444 (2)C9—C101.371 (3)
O3—C11.199 (2)C9—H90.9500
C1—C21.505 (3)C10—C111.391 (3)
C2—C31.537 (3)C10—H100.9500
C2—C51.556 (3)C11—C121.389 (3)
C2—H21.0000C11—H110.9500
C3—C61.510 (3)C13—C181.376 (3)
C3—C41.546 (3)C13—C141.394 (3)
C3—H31.0000C13—H130.9500
C4—C121.514 (3)C14—C151.376 (3)
C4—H41.0000C14—H140.9500
C5—C181.506 (3)C15—C161.372 (3)
C5—H51.0000C15—H150.9500
C6—H6A0.9900C16—C171.391 (3)
C6—H6B0.9900C16—H160.9500
C7—C121.383 (3)C17—C181.393 (3)
C7—C81.394 (3)C17—H170.9500
C1—O1—C4111.34 (15)C12—C7—H7120.1
C5—O2—C6103.87 (16)C8—C7—H7120.1
O3—C1—O1120.45 (19)C9—C8—C7120.3 (2)
O3—C1—C2128.7 (2)C9—C8—H8119.9
O1—C1—C2110.84 (16)C7—C8—H8119.9
C1—C2—C3105.06 (17)C10—C9—C8120.4 (2)
C1—C2—C5115.83 (17)C10—C9—H9119.8
C3—C2—C5103.17 (17)C8—C9—H9119.8
C1—C2—H2110.8C9—C10—C11119.6 (2)
C3—C2—H2110.8C9—C10—H10120.2
C5—C2—H2110.8C11—C10—H10120.2
C6—C3—C2104.00 (17)C12—C11—C10120.6 (2)
C6—C3—C4110.95 (18)C12—C11—H11119.7
C2—C3—C4103.84 (15)C10—C11—H11119.7
C6—C3—H3112.5C7—C12—C11119.4 (2)
C2—C3—H3112.5C7—C12—C4123.08 (18)
C4—C3—H3112.5C11—C12—C4117.5 (2)
O1—C4—C12110.89 (16)C18—C13—C14120.9 (2)
O1—C4—C3106.50 (16)C18—C13—H13119.5
C12—C4—C3114.20 (16)C14—C13—H13119.5
O1—C4—H4108.4C15—C14—C13119.6 (2)
C12—C4—H4108.4C15—C14—H14120.2
C3—C4—H4108.4C13—C14—H14120.2
O2—C5—C18110.18 (17)C16—C15—C14120.1 (2)
O2—C5—C2104.57 (16)C16—C15—H15120.0
C18—C5—C2118.83 (16)C14—C15—H15120.0
O2—C5—H5107.6C15—C16—C17120.6 (2)
C18—C5—H5107.6C15—C16—H16119.7
C2—C5—H5107.6C17—C16—H16119.7
O2—C6—C3103.71 (15)C16—C17—C18119.7 (2)
O2—C6—H6A111.0C16—C17—H17120.1
C3—C6—H6A111.0C18—C17—H17120.1
O2—C6—H6B111.0C13—C18—C17119.1 (2)
C3—C6—H6B111.0C13—C18—C5119.00 (19)
H6A—C6—H6B109.0C17—C18—C5121.9 (2)
C12—C7—C8119.7 (2)

Experimental details

Crystal data
Chemical formulaC18H16O3
Mr280.31
Crystal system, space groupMonoclinic, C2/c
Temperature (K)150
a, b, c (Å)21.416 (1), 7.520 (1), 19.487 (1)
β (°) 117.86 (1)
V3)2774.7 (3)
Z8
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.30 × 0.20 × 0.15
Data collection
DiffractometerNonius KappaCCD area-detector
diffractometer
Absorption correctionMulti-scan
(Blessing, 1997)
Tmin, Tmax0.973, 0.987
No. of measured, independent and
observed [I > 2σ(I)] reflections
7164, 2489, 1822
Rint0.067
(sin θ/λ)max1)0.600
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.051, 0.109, 0.97
No. of reflections2489
No. of parameters207
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.25, 0.22

Computer programs: DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998), DENZO and COLLECT, DENZO and COLLECT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 1990).

 

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