Abstract
In the title compound, C15H12O2, the dihedral angle between the aromatic ring systems is 16.67 (6)°. The methyl C atom is almost coplanar with its attached benzene ring [displacement = 0.020 (2) Å]. In the crystal, the molecules are connected by weak C—H⋯O bonds and face-to-edge C—H⋯π interactions between the 2-methoxyphenyl rings.
Related literature
For the biological activity of related compounds, see: Akgul & Anil (2003 ▶); Aslam et al. (2006 ▶); Galal et al. (2009 ▶); Khan et al. (2005 ▶); Soekamto et al. (2003 ▶). For the synthesis, see: Takeda et al. (2007 ▶).
Experimental
Crystal data
C15H12O2
M r = 224.25
Orthorhombic,
a = 6.9419 (1) Å
b = 11.4409 (2) Å
c = 14.1703 (3) Å
V = 1125.43 (3) Å3
Z = 4
Cu Kα radiation
μ = 0.70 mm−1
T = 120 K
0.27 × 0.25 × 0.12 mm
Data collection
Oxford Diffraction Xcalibur Atlas Gemini Ultra diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010 ▶) T min = 0.683, T max = 1.000
11347 measured reflections
2006 independent reflections
1955 reflections with I > 2σ(I)
R int = 0.050
Refinement
R[F 2 > 2σ(F 2)] = 0.033
wR(F 2) = 0.088
S = 1.09
2006 reflections
155 parameters
H-atom parameters constrained
Δρmax = 0.20 e Å−3
Δρmin = −0.14 e Å−3
Absolute structure: Flack (1983 ▶), 822 Friedel pairs
Flack parameter: −0.2 (2)
Data collection: CrysAlis PRO (Oxford Diffraction, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811017168/hb5866sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811017168/hb5866Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the C2–C7 ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C1—H1B⋯O2i | 0.96 | 2.57 | 3.272 (2) | 131 |
| C3—H3⋯Cg1ii | 0.93 | 2.78 | 3.604 (2) | 149 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported by the Institutional research plan No. AVOZ10100521 of the Institute of Physics, the project Praemium Academiae of the Academy of Sciences of the Czech Republic and the Czech Ministry of Education, Youth and Sports, project MSM 4977751303.
supplementary crystallographic information
Comment
A wide range of natural products with diverse pharmaceutical properties, such as antifungal, antitumor, antiviral, and antimicrobial (Aslam et al., 2006; Galal et al., 2009; Khan et al., 2005), contain a benzofuran ring (Akgul & Anil, 2003; Soekamto et al., 2003). In this paper, we present a crystal structure of the title compound, (I).
The benzofuran unit is essentially planar, with a mean deviation of 0.019 (2)Å from the least-square plane defined by the nine atoms in benzofuran ring. The methoxy group forms intermolecular hydrogen bond to the oxygen in benzofuran ring (Table 1). Another weak interactions found in the crystal is the C—H···π interaction between the 2-methoxyphenyl rings [C3—H3···Cg1 (C2 → C7)] which is responsible for their edge-to-face orientation (Fig. 2).
Experimental
2-(2'-methoxyphenyl]-benzo[b]furan was synthesized by the method described by Takeda (Takeda et al., 2007). Crystals were prepared by slow evaporation from acetonitrile.
Refinement
The hydrogen atoms were localized from the difference Fourier map. Despite of that, all hydrogen atoms connected to C were constrained to ideal positions. The isotropic temperature parameters of hydrogen atoms were calculated as 1.2*Ueq of the parent atom.
Figures
Fig. 1.
View of (I) with displacement ellipsoids shown at the 50% probability level.
Fig. 2.
Projection along the b axis with highlighted face-to-edge CH-π interactions between methoxyphenyl rings.
Crystal data
| C15H12O2 | F(000) = 472 |
| Mr = 224.25 | Dx = 1.323 Mg m−3 |
| Orthorhombic, P212121 | Cu Kα radiation, λ = 1.5418 Å |
| Hall symbol: P 2ab 2ac | Cell parameters from 7843 reflections |
| a = 6.9419 (1) Å | θ = 3.1–66.9° |
| b = 11.4409 (2) Å | µ = 0.70 mm−1 |
| c = 14.1703 (3) Å | T = 120 K |
| V = 1125.43 (3) Å3 | Plate, colourless |
| Z = 4 | 0.27 × 0.25 × 0.12 mm |
Data collection
| Oxford Diffraction Xcalibur Atlas Gemini ultra diffractometer | 2006 independent reflections |
| Radiation source: Enhance Ultra (Cu) X-ray Source | 1955 reflections with I > 2σ(I) |
| mirror | Rint = 0.050 |
| Detector resolution: 10.3748 pixels mm-1 | θmax = 67.1°, θmin = 5.0° |
| Rotation method data acquisition using ω scans | h = −8→7 |
| Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) | k = −13→13 |
| Tmin = 0.683, Tmax = 1.000 | l = −16→14 |
| 11347 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.033 | H-atom parameters constrained |
| wR(F2) = 0.088 | w = 1/[σ2(Fo2) + (0.0543P)2 + 0.153P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.09 | (Δ/σ)max < 0.001 |
| 2006 reflections | Δρmax = 0.20 e Å−3 |
| 155 parameters | Δρmin = −0.14 e Å−3 |
| 0 restraints | Absolute structure: Flack (1983), 822 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: −0.2 (2) |
Special details
| 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. The hydrogen atoms were localized from the difference Fourier map. Despite of that,all hydrogen atoms connected to C were constrained to ideal positions. The isotropic temperature parameters of hydrogen atoms were calculated as 1.2*Ueq of the parent atom. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| O1 | 1.06771 (15) | 0.13587 (9) | 0.33592 (7) | 0.0323 (3) | |
| O2 | 0.61359 (14) | 0.36286 (9) | 0.28934 (7) | 0.0293 (3) | |
| C2 | 1.0779 (2) | 0.24444 (13) | 0.37522 (10) | 0.0282 (3) | |
| C11 | 0.4903 (2) | 0.32298 (13) | 0.22083 (10) | 0.0281 (3) | |
| C6 | 0.9320 (2) | 0.43475 (13) | 0.38967 (10) | 0.0301 (3) | |
| H6 | 0.8355 | 0.4875 | 0.3737 | 0.036* | |
| C7 | 0.9277 (2) | 0.32219 (13) | 0.35139 (10) | 0.0275 (3) | |
| C3 | 1.2221 (2) | 0.27897 (14) | 0.43667 (11) | 0.0319 (3) | |
| H3 | 1.3202 | 0.2272 | 0.4525 | 0.038* | |
| C15 | 0.4610 (2) | 0.17104 (13) | 0.10446 (11) | 0.0322 (3) | |
| H15 | 0.5069 | 0.1044 | 0.0743 | 0.039* | |
| C9 | 0.7486 (2) | 0.20323 (12) | 0.22207 (11) | 0.0295 (3) | |
| H9 | 0.8343 | 0.1430 | 0.2087 | 0.035* | |
| C14 | 0.2874 (2) | 0.22039 (14) | 0.07865 (11) | 0.0344 (4) | |
| H14 | 0.2165 | 0.1869 | 0.0300 | 0.041* | |
| C5 | 1.0769 (2) | 0.46960 (13) | 0.45085 (11) | 0.0333 (3) | |
| H5 | 1.0774 | 0.5449 | 0.4755 | 0.040* | |
| C10 | 0.5664 (2) | 0.22374 (13) | 0.17718 (10) | 0.0283 (3) | |
| C8 | 0.7723 (2) | 0.28854 (12) | 0.28798 (10) | 0.0268 (3) | |
| C13 | 0.2159 (2) | 0.31977 (14) | 0.12430 (11) | 0.0346 (4) | |
| H13 | 0.0980 | 0.3505 | 0.1055 | 0.041* | |
| C12 | 0.3160 (2) | 0.37352 (14) | 0.19675 (11) | 0.0333 (3) | |
| H12 | 0.2690 | 0.4395 | 0.2274 | 0.040* | |
| C1 | 1.2147 (3) | 0.05403 (14) | 0.36035 (12) | 0.0382 (4) | |
| H1A | 1.3373 | 0.0828 | 0.3394 | 0.046* | |
| H1B | 1.1884 | −0.0196 | 0.3305 | 0.046* | |
| H1C | 1.2171 | 0.0438 | 0.4276 | 0.046* | |
| C4 | 1.2206 (2) | 0.39125 (14) | 0.47490 (11) | 0.0352 (4) | |
| H4 | 1.3168 | 0.4136 | 0.5168 | 0.042* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0364 (5) | 0.0258 (5) | 0.0348 (5) | 0.0044 (5) | −0.0035 (5) | −0.0030 (4) |
| O2 | 0.0288 (5) | 0.0280 (5) | 0.0311 (5) | 0.0011 (4) | 0.0007 (4) | −0.0013 (4) |
| C2 | 0.0321 (7) | 0.0253 (7) | 0.0272 (7) | −0.0002 (6) | 0.0043 (6) | 0.0028 (5) |
| C11 | 0.0276 (6) | 0.0282 (7) | 0.0284 (7) | −0.0049 (6) | 0.0025 (6) | 0.0041 (6) |
| C6 | 0.0328 (8) | 0.0259 (7) | 0.0317 (7) | 0.0009 (6) | 0.0005 (6) | 0.0025 (6) |
| C7 | 0.0300 (7) | 0.0253 (7) | 0.0271 (7) | −0.0013 (6) | 0.0031 (6) | 0.0029 (6) |
| C3 | 0.0322 (7) | 0.0303 (7) | 0.0331 (8) | 0.0005 (7) | −0.0021 (6) | 0.0049 (6) |
| C15 | 0.0370 (8) | 0.0273 (7) | 0.0324 (7) | −0.0031 (6) | −0.0008 (6) | 0.0006 (6) |
| C9 | 0.0320 (7) | 0.0251 (7) | 0.0314 (8) | 0.0011 (6) | 0.0007 (6) | −0.0008 (6) |
| C14 | 0.0351 (8) | 0.0332 (8) | 0.0349 (8) | −0.0076 (7) | −0.0039 (7) | 0.0039 (6) |
| C5 | 0.0388 (8) | 0.0257 (7) | 0.0352 (8) | −0.0034 (7) | −0.0023 (7) | −0.0010 (6) |
| C10 | 0.0307 (7) | 0.0251 (7) | 0.0291 (7) | −0.0032 (6) | 0.0026 (6) | 0.0033 (6) |
| C8 | 0.0279 (6) | 0.0235 (7) | 0.0289 (7) | 0.0008 (6) | 0.0030 (6) | 0.0033 (6) |
| C13 | 0.0276 (7) | 0.0372 (8) | 0.0389 (8) | −0.0024 (7) | −0.0013 (6) | 0.0072 (7) |
| C12 | 0.0318 (7) | 0.0309 (8) | 0.0373 (8) | 0.0014 (7) | 0.0046 (6) | 0.0029 (6) |
| C1 | 0.0394 (8) | 0.0316 (8) | 0.0437 (9) | 0.0092 (7) | −0.0027 (7) | −0.0036 (7) |
| C4 | 0.0382 (8) | 0.0326 (8) | 0.0348 (8) | −0.0048 (7) | −0.0059 (7) | 0.0015 (6) |
Geometric parameters (Å, °)
| O1—C2 | 1.3630 (18) | C15—H15 | 0.9300 |
| O1—C1 | 1.4273 (18) | C9—C8 | 1.361 (2) |
| O2—C11 | 1.3723 (18) | C9—C10 | 1.435 (2) |
| O2—C8 | 1.3921 (17) | C9—H9 | 0.9300 |
| C2—C3 | 1.384 (2) | C14—C13 | 1.399 (2) |
| C2—C7 | 1.411 (2) | C14—H14 | 0.9300 |
| C11—C12 | 1.384 (2) | C5—C4 | 1.384 (2) |
| C11—C10 | 1.397 (2) | C5—H5 | 0.9300 |
| C6—C5 | 1.386 (2) | C13—C12 | 1.384 (2) |
| C6—C7 | 1.398 (2) | C13—H13 | 0.9300 |
| C6—H6 | 0.9300 | C12—H12 | 0.9300 |
| C7—C8 | 1.456 (2) | C1—H1A | 0.9600 |
| C3—C4 | 1.394 (2) | C1—H1B | 0.9600 |
| C3—H3 | 0.9300 | C1—H1C | 0.9600 |
| C15—C14 | 1.380 (2) | C4—H4 | 0.9300 |
| C15—C10 | 1.400 (2) | ||
| C2—O1—C1 | 117.50 (12) | C13—C14—H14 | 119.3 |
| C11—O2—C8 | 106.31 (11) | C4—C5—C6 | 119.38 (14) |
| O1—C2—C3 | 123.68 (14) | C4—C5—H5 | 120.3 |
| O1—C2—C7 | 116.00 (14) | C6—C5—H5 | 120.3 |
| C3—C2—C7 | 120.31 (13) | C11—C10—C15 | 118.58 (14) |
| O2—C11—C12 | 125.51 (14) | C11—C10—C9 | 105.67 (13) |
| O2—C11—C10 | 110.34 (13) | C15—C10—C9 | 135.74 (15) |
| C12—C11—C10 | 124.14 (14) | C9—C8—O2 | 110.60 (12) |
| C5—C6—C7 | 121.56 (14) | C9—C8—C7 | 134.67 (14) |
| C5—C6—H6 | 119.2 | O2—C8—C7 | 114.61 (11) |
| C7—C6—H6 | 119.2 | C12—C13—C14 | 121.74 (15) |
| C6—C7—C2 | 118.17 (14) | C12—C13—H13 | 119.1 |
| C6—C7—C8 | 119.94 (13) | C14—C13—H13 | 119.1 |
| C2—C7—C8 | 121.89 (13) | C11—C12—C13 | 115.87 (15) |
| C2—C3—C4 | 120.13 (15) | C11—C12—H12 | 122.1 |
| C2—C3—H3 | 119.9 | C13—C12—H12 | 122.1 |
| C4—C3—H3 | 119.9 | O1—C1—H1A | 109.5 |
| C14—C15—C10 | 118.36 (15) | O1—C1—H1B | 109.5 |
| C14—C15—H15 | 120.8 | H1A—C1—H1B | 109.5 |
| C10—C15—H15 | 120.8 | O1—C1—H1C | 109.5 |
| C8—C9—C10 | 107.07 (13) | H1A—C1—H1C | 109.5 |
| C8—C9—H9 | 126.5 | H1B—C1—H1C | 109.5 |
| C10—C9—H9 | 126.5 | C5—C4—C3 | 120.42 (15) |
| C15—C14—C13 | 121.31 (15) | C5—C4—H4 | 119.8 |
| C15—C14—H14 | 119.3 | C3—C4—H4 | 119.8 |
Hydrogen-bond geometry (°)
| Cg1 is the centroid of the C2–C7 ring. |
| D—H···A |
| —··· |
| —··· |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB5866).
References
- Akgul, Y. Y. & Anil, H. (2003). Phytochemistry, 63, 939–943. [DOI] [PubMed]
- Aslam, S. N., Stevenson, P. C., Phythian, S. J., Veitch, N. C. & Hall, D. R. (2006). Tetrahedron, 62, 4214–4226.
- Flack, H. D. (1983). Acta Cryst. A39, 876–881.
- Galal, S. A., Abd El-All, A. S., Abdalah, M. M. & El-Diwani, H. I. (2009). Bioorg. Med. Chem. Lett. 19, 2420–2428. [DOI] [PubMed]
- Khan, M. W., Alam, M. J., Rashid, M. A. & Chowdhury, R. (2005). Bioorg. Med. Chem. 13, 4796–4805. [DOI] [PubMed]
- Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
- Oxford Diffraction (2010). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Soekamto, N. H., Achmad, S. A., Ghisalberti, E. L., Hakim, E. H. & Syah, Y. M. (2003). Phytochemistry, 64, 831–834. [DOI] [PubMed]
- Takeda, N., Miyata, O. & Naito, T. (2007). Eur. J. Org. Chem 9, 1491–1509.
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811017168/hb5866sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811017168/hb5866Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


