supplementary materials


Acta Cryst. (2008). E64, o2161    [ doi:10.1107/S1600536808031644 ]

(E)-3-(2-Furyl)-1-(2-hydroxyphenyl)prop-2-en-1-one

L. Kong and Y. Liu

Abstract top

In the title molecule, C13H10O3, an intramolecular O-H...O hydrogen bond influences the molecular conformation, and the benzene and furan rings form a dihedral angle of 8.35 (7)°. Weak intermolecular C-H...O hydrogen bonds link molecules into sheets parallel to the bc plane.

Comment top

In continuation of our ongoing program directed to the development of environmentally benign methods of chemical synthesis, we describe in this paper a user-friendly, solvent-free protocol for the synthesis of chalcones starting from the fragrant aldehydes and fragrant ketones in the presence of NaOH under solvent-free conditions. Using this method, which can be considered as a a general method for the synthesis of chalcones, we obtained the title compound, (I). We present here its crystal structure.

In (I) (Fig. 1), the bond lengths and angles are normal and comparable to those observed in related compound (Li et al., 1992). The benzene and furan rings form a dihedral angle of 8.35 (7)°. In the crystal, weak intermolecular C—H···O hydrogen bonds (Table 1) link the molecules into sheets parallel to bc plane.

Related literature top

For a related crystal structure, see: Li et al. (1992).

Experimental top

Furan-2-carbaldehyde (0.3 mmol) and 2-hydroxylacetophenone (0.3 mmol), NaOH (0.3 mmol) were mixed in 50 ml flash under sovlent-free conditions After stirring for 5 min at 373 K, the mixture was soilden slowly and afforded the title compound, then recrystallized from ethanol, affording the title compound as a colourless crystalline solid. Elemental analysis: calculated for C13H10O3: C 72.90, H 4.71%; found: C 72.88, H 4.65%.

Refinement top

All H atoms were placed in geometrically idealized positions (O—H 0.85 Å, C—H 0.93 Å) and treated as riding, with Uiso(H) = 1.2 Ueq(C,O).

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) showing the atomic numbering and 40% probability displacement ellipsoids.
(E)-3-(2-Furyl)-1-(2-hydroxyphenyl)prop-2-en-1-one top
Crystal data top
C13H10O3F(000) = 448
Mr = 214.21Dx = 1.367 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 3.8560 (5) ÅCell parameters from 438 reflections
b = 15.6565 (14) Åθ = 2.4–18.4°
c = 17.309 (2) ŵ = 0.10 mm1
β = 95.065 (2)°T = 298 K
V = 1040.9 (2) Å3Block, colourless
Z = 40.27 × 0.25 × 0.07 mm
Data collection top
Siemens SMART CCD area-detector
diffractometer
1848 independent reflections
Radiation source: fine-focus sealed tube668 reflections with I > 2σ(I)
graphiteRint = 0.126
Detector resolution: φ and ω pixels mm-1θmax = 25.0°, θmin = 1.8°
φ and ω scansh = 44
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 718
Tmin = 0.974, Tmax = 0.993l = 2020
5153 measured 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)] = 0.067Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.184H-atom parameters constrained
S = 0.81 w = 1/[σ2(Fo2) + (0.0721P)2]
where P = (Fo2 + 2Fc2)/3
1848 reflections(Δ/σ)max < 0.001
146 parametersΔρmax = 0.22 e Å3
0 restraintsΔρmin = 0.19 e Å3
Crystal data top
C13H10O3V = 1040.9 (2) Å3
Mr = 214.21Z = 4
Monoclinic, P21/cMo Kα radiation
a = 3.8560 (5) ŵ = 0.10 mm1
b = 15.6565 (14) ÅT = 298 K
c = 17.309 (2) Å0.27 × 0.25 × 0.07 mm
β = 95.065 (2)°
Data collection top
Siemens SMART CCD area-detector
diffractometer
1848 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
668 reflections with I > 2σ(I)
Tmin = 0.974, Tmax = 0.993Rint = 0.126
5153 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.067H-atom parameters constrained
wR(F2) = 0.184Δρmax = 0.22 e Å3
S = 0.81Δρmin = 0.19 e Å3
1848 reflectionsAbsolute structure: ?
146 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
O11.0561 (7)0.73465 (16)0.48262 (15)0.0794 (9)
O20.8017 (8)0.83794 (18)0.74522 (15)0.0885 (11)
O30.5477 (10)0.9672 (2)0.80912 (17)0.1030 (12)
H30.65460.92200.80870.154*
C11.1454 (12)0.6735 (3)0.4327 (2)0.0842 (15)
H11.14720.68110.37940.101*
C21.2297 (11)0.6018 (3)0.4699 (3)0.0769 (13)
H21.30180.55100.44850.092*
C31.1887 (11)0.6177 (3)0.5478 (2)0.0748 (13)
H3A1.22710.57880.58820.090*
C41.0842 (10)0.6991 (2)0.5544 (2)0.0584 (10)
C50.9983 (9)0.7493 (2)0.6177 (2)0.0608 (11)
H51.02220.72400.66650.073*
C60.8860 (10)0.8300 (2)0.6137 (2)0.0598 (11)
H60.86760.85780.56610.072*
C70.7918 (10)0.8754 (2)0.6822 (2)0.0600 (11)
C80.6700 (9)0.9648 (2)0.6757 (2)0.0553 (10)
C90.5559 (11)1.0064 (3)0.7399 (2)0.0690 (12)
C100.4467 (12)1.0901 (3)0.7358 (3)0.0835 (14)
H100.36971.11700.77900.100*
C110.4529 (13)1.1329 (3)0.6679 (3)0.0930 (16)
H110.37691.18930.66490.112*
C120.5685 (12)1.0951 (3)0.6033 (3)0.0839 (14)
H120.57471.12560.55730.101*
C130.6745 (11)1.0117 (3)0.6079 (2)0.0702 (12)
H130.75180.98580.56420.084*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.111 (3)0.0632 (19)0.0648 (18)0.0106 (16)0.0132 (16)0.0022 (16)
O20.138 (3)0.067 (2)0.0625 (18)0.0095 (18)0.0190 (18)0.0029 (15)
O30.150 (4)0.087 (3)0.076 (2)0.010 (2)0.033 (2)0.0105 (18)
C10.112 (4)0.076 (3)0.065 (3)0.008 (3)0.015 (3)0.014 (3)
C20.080 (4)0.057 (3)0.095 (3)0.008 (2)0.012 (3)0.016 (3)
C30.086 (4)0.061 (3)0.078 (3)0.008 (2)0.011 (2)0.004 (2)
C40.065 (3)0.053 (2)0.058 (2)0.002 (2)0.010 (2)0.001 (2)
C50.063 (3)0.059 (2)0.061 (2)0.001 (2)0.010 (2)0.004 (2)
C60.067 (3)0.058 (2)0.054 (2)0.002 (2)0.005 (2)0.003 (2)
C70.064 (3)0.057 (3)0.059 (2)0.005 (2)0.004 (2)0.001 (2)
C80.055 (3)0.053 (2)0.058 (2)0.0020 (19)0.006 (2)0.001 (2)
C90.071 (3)0.069 (3)0.068 (3)0.001 (2)0.009 (2)0.009 (2)
C100.080 (4)0.073 (3)0.095 (4)0.008 (3)0.001 (3)0.023 (3)
C110.093 (4)0.061 (3)0.122 (4)0.014 (3)0.014 (3)0.013 (3)
C120.099 (4)0.063 (3)0.086 (3)0.000 (3)0.008 (3)0.007 (3)
C130.078 (3)0.056 (3)0.076 (3)0.004 (2)0.007 (2)0.005 (2)
Geometric parameters (Å, °) top
O1—C11.354 (4)C6—C71.455 (5)
O1—C41.357 (4)C6—H60.9300
O2—C71.237 (4)C7—C81.476 (5)
O3—C91.349 (4)C8—C131.386 (5)
O3—H30.8200C8—C91.393 (5)
C1—C21.321 (5)C9—C101.377 (6)
C1—H10.9300C10—C111.354 (5)
C2—C31.394 (5)C10—H100.9300
C2—H20.9300C11—C121.374 (6)
C3—C41.343 (5)C11—H110.9300
C3—H3A0.9300C12—C131.368 (5)
C4—C51.413 (5)C12—H120.9300
C5—C61.335 (5)C13—H130.9300
C5—H50.9300
C1—O1—C4106.9 (3)O2—C7—C8120.1 (4)
C9—O3—H3109.5C6—C7—C8120.1 (3)
C2—C1—O1110.8 (3)C13—C8—C9117.1 (4)
C2—C1—H1124.6C13—C8—C7122.6 (3)
O1—C1—H1124.6C9—C8—C7120.3 (4)
C1—C2—C3106.0 (4)O3—C9—C10116.6 (4)
C1—C2—H2127.0O3—C9—C8122.0 (4)
C3—C2—H2127.0C10—C9—C8121.4 (4)
C4—C3—C2108.2 (4)C11—C10—C9119.2 (4)
C4—C3—H3A125.9C11—C10—H10120.4
C2—C3—H3A125.9C9—C10—H10120.4
C3—C4—O1108.2 (3)C10—C11—C12121.6 (4)
C3—C4—C5133.3 (4)C10—C11—H11119.2
O1—C4—C5118.5 (3)C12—C11—H11119.2
C6—C5—C4125.7 (3)C13—C12—C11118.8 (4)
C6—C5—H5117.1C13—C12—H12120.6
C4—C5—H5117.1C11—C12—H12120.6
C5—C6—C7121.6 (3)C12—C13—C8122.0 (4)
C5—C6—H6119.2C12—C13—H13119.0
C7—C6—H6119.2C8—C13—H13119.0
O2—C7—C6119.7 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O3—H3···O20.821.842.544 (4)144
C1—H1···O2i0.932.593.400 (5)146
C3—H3A···O3ii0.932.593.504 (5)169
Symmetry codes: (i) x, −y+3/2, z−1/2; (ii) −x+2, y−1/2, −z+3/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O3—H3···O20.821.842.544 (4)144
C1—H1···O2i0.932.593.400 (5)146
C3—H3A···O3ii0.932.593.504 (5)169
Symmetry codes: (i) x, −y+3/2, z−1/2; (ii) −x+2, y−1/2, −z+3/2.
Acknowledgements top

This project was supported by the Foundation of Dongchang College, Liaocheng University (grant No. LG0801).

references
References top

Li, Z.-D., Huang, L.-Z., Su, G.-B. & Wang, H.-Y. (1992). Chin. J. Struct. Chem. 11, 1–4.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Siemens (1996). SMART and SAINT. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.