organic compounds
3-Methyl-4H-chromen-4-one
aShandong Provincial Key Laboratory of Microbial Engineering, Shandong Institute of Light Industry, Jinan 250353, People's Republic of China
*Correspondence e-mail: lujianghao001@yahoo.com.cn
In the title chromenone derivative, C10H8O2, the two fused six-membered rings are coplanar, with a mean deviation of 0.0261 (1) Å from the plane through the non-H atoms of the rings. The carbonyl and methyl substituents of the pyran ring also lie close to that plane, with the O and C atoms deviating by 0.0557 (1) and 0.1405 (1) Å, respectively. In the crystal, weak C—H⋯O contacts form chains along the a axis.
Related literature
For the pharmaceutical applications of chromanone compounds, see: Shi et al. (2004). For related structures, see: Takikawa & Suzuki (2007); Patonay et al. (2002); Alaniz & Rovis, (2005).
Experimental
Crystal data
|
Refinement
|
Data collection: APEX2 (Bruker, 2004); cell SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus; 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.
Supporting information
10.1107/S1600536810020453/sj5009sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810020453/sj5009Isup2.hkl
3-methyl-4H-chromen-4-one powder (10 mmoL, 1.60 g) was purchased from Jinan Henghua Science & Technology Co. Ltd., dissolved in 20 ml ethanol and evaporated in an open flask at room temperature. One week later, colorless block like crystals of the title compound suitable for the X-ray analysis were obained. Anal. C10H8O2: C, 74.93; H, 5.00%. Found: C, 74.86; H, 4.89%.
Hydrogen atoms were placed in geometrically calculated positions (C—H 0.95 Å for aromatic and formyl, 0.99 Å for methylene and 0.98 Å for methyl) and included in the
in a riding motion approximation with Uiso(H) = 1.2Ueq(C) [for methyl groups Uiso(H) = 1.5Ueq(C)].Data collection: APEX2 (Bruker, 2004); cell
SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus (Bruker, 2001); 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).C10H8O2 | Z = 2 |
Mr = 160.16 | F(000) = 168 |
Triclinic, P1 | Dx = 1.336 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 6.5284 (13) Å | Cell parameters from 1573 reflections |
b = 7.2210 (14) Å | θ = 2.4–28.4° |
c = 8.9834 (18) Å | µ = 0.09 mm−1 |
α = 75.137 (2)° | T = 296 K |
β = 78.169 (2)° | Block, colorless |
γ = 80.895 (2)° | 0.12 × 0.10 × 0.08 mm |
V = 398.12 (14) Å3 |
Bruker APEXII CCD diffractometer | 1394 independent reflections |
Radiation source: fine-focus sealed tube | 1143 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.014 |
ϕ and ω scans | θmax = 25.0°, θmin = 2.4° |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −7→7 |
Tmin = 0.989, Tmax = 0.993 | k = −8→8 |
2771 measured reflections | l = −10→10 |
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)] = 0.039 | H-atom parameters constrained |
wR(F2) = 0.116 | w = 1/[σ2(Fo2) + (0.065P)2 + 0.067P] where P = (Fo2 + 2Fc2)/3 |
S = 1.00 | (Δ/σ)max < 0.001 |
1394 reflections | Δρmax = 0.18 e Å−3 |
111 parameters | Δρmin = −0.14 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.032 (10) |
C10H8O2 | γ = 80.895 (2)° |
Mr = 160.16 | V = 398.12 (14) Å3 |
Triclinic, P1 | Z = 2 |
a = 6.5284 (13) Å | Mo Kα radiation |
b = 7.2210 (14) Å | µ = 0.09 mm−1 |
c = 8.9834 (18) Å | T = 296 K |
α = 75.137 (2)° | 0.12 × 0.10 × 0.08 mm |
β = 78.169 (2)° |
Bruker APEXII CCD diffractometer | 1394 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | 1143 reflections with I > 2σ(I) |
Tmin = 0.989, Tmax = 0.993 | Rint = 0.014 |
2771 measured reflections |
R[F2 > 2σ(F2)] = 0.039 | 0 restraints |
wR(F2) = 0.116 | H-atom parameters constrained |
S = 1.00 | Δρmax = 0.18 e Å−3 |
1394 reflections | Δρmin = −0.14 e Å−3 |
111 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.5883 (2) | 0.71757 (18) | 1.05339 (16) | 0.0417 (3) | |
C2 | 0.4277 (2) | 0.76708 (17) | 0.96592 (15) | 0.0390 (3) | |
C3 | 0.4728 (2) | 0.76636 (18) | 0.79936 (15) | 0.0427 (4) | |
C4 | 0.6928 (2) | 0.71855 (19) | 0.73797 (16) | 0.0455 (4) | |
C5 | 0.8332 (2) | 0.6710 (2) | 0.83389 (17) | 0.0503 (4) | |
H5 | 0.9726 | 0.6398 | 0.7905 | 0.060* | |
C6 | 0.7581 (3) | 0.7246 (3) | 0.56727 (18) | 0.0700 (5) | |
H6A | 0.9074 | 0.6903 | 0.5445 | 0.105* | |
H6B | 0.7222 | 0.8524 | 0.5078 | 0.105* | |
H6C | 0.6864 | 0.6350 | 0.5400 | 0.105* | |
C7 | 0.2263 (2) | 0.8210 (2) | 1.04176 (18) | 0.0506 (4) | |
H7 | 0.1150 | 0.8533 | 0.9864 | 0.061* | |
C8 | 0.1897 (3) | 0.8271 (2) | 1.19601 (19) | 0.0602 (4) | |
H8 | 0.0549 | 0.8646 | 1.2443 | 0.072* | |
C9 | 0.3541 (3) | 0.7771 (2) | 1.28035 (18) | 0.0607 (5) | |
H9 | 0.3291 | 0.7818 | 1.3851 | 0.073* | |
C10 | 0.5524 (3) | 0.7212 (2) | 1.21027 (17) | 0.0554 (4) | |
H10 | 0.6621 | 0.6859 | 1.2671 | 0.066* | |
O1 | 0.33452 (17) | 0.80490 (17) | 0.71782 (12) | 0.0648 (4) | |
O2 | 0.79069 (14) | 0.66418 (15) | 0.98916 (11) | 0.0522 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0424 (7) | 0.0398 (7) | 0.0441 (7) | −0.0053 (5) | −0.0089 (6) | −0.0103 (5) |
C2 | 0.0379 (7) | 0.0336 (6) | 0.0444 (7) | −0.0056 (5) | −0.0078 (5) | −0.0057 (5) |
C3 | 0.0444 (8) | 0.0392 (7) | 0.0440 (7) | −0.0064 (6) | −0.0133 (6) | −0.0031 (5) |
C4 | 0.0487 (8) | 0.0439 (7) | 0.0421 (7) | −0.0055 (6) | −0.0062 (6) | −0.0080 (6) |
C5 | 0.0397 (8) | 0.0574 (9) | 0.0522 (8) | −0.0016 (6) | −0.0028 (6) | −0.0162 (7) |
C6 | 0.0782 (12) | 0.0787 (12) | 0.0445 (9) | −0.0009 (9) | −0.0016 (8) | −0.0108 (8) |
C7 | 0.0418 (8) | 0.0482 (8) | 0.0594 (9) | −0.0046 (6) | −0.0063 (6) | −0.0106 (6) |
C8 | 0.0552 (9) | 0.0551 (9) | 0.0635 (10) | −0.0085 (7) | 0.0104 (7) | −0.0168 (7) |
C9 | 0.0803 (12) | 0.0573 (9) | 0.0437 (8) | −0.0141 (8) | 0.0018 (8) | −0.0164 (7) |
C10 | 0.0673 (10) | 0.0573 (9) | 0.0461 (8) | −0.0084 (7) | −0.0180 (7) | −0.0129 (7) |
O1 | 0.0559 (7) | 0.0849 (8) | 0.0544 (7) | −0.0039 (6) | −0.0253 (5) | −0.0076 (5) |
O2 | 0.0403 (6) | 0.0681 (7) | 0.0517 (6) | 0.0017 (5) | −0.0162 (4) | −0.0184 (5) |
C1—O2 | 1.3668 (17) | C6—H6A | 0.9600 |
C1—C2 | 1.3854 (19) | C6—H6B | 0.9600 |
C1—C10 | 1.387 (2) | C6—H6C | 0.9600 |
C2—C7 | 1.3967 (19) | C7—C8 | 1.368 (2) |
C2—C3 | 1.4657 (19) | C7—H7 | 0.9300 |
C3—O1 | 1.2312 (16) | C8—C9 | 1.388 (2) |
C3—C4 | 1.450 (2) | C8—H8 | 0.9300 |
C4—C5 | 1.332 (2) | C9—C10 | 1.366 (2) |
C4—C6 | 1.4961 (19) | C9—H9 | 0.9300 |
C5—O2 | 1.3548 (17) | C10—H10 | 0.9300 |
C5—H5 | 0.9300 | ||
O2—C1—C2 | 121.70 (12) | H6A—C6—H6B | 109.5 |
O2—C1—C10 | 116.53 (12) | C4—C6—H6C | 109.5 |
C2—C1—C10 | 121.77 (14) | H6A—C6—H6C | 109.5 |
C1—C2—C7 | 117.46 (13) | H6B—C6—H6C | 109.5 |
C1—C2—C3 | 120.18 (13) | C8—C7—C2 | 121.23 (14) |
C7—C2—C3 | 122.34 (13) | C8—C7—H7 | 119.4 |
O1—C3—C4 | 122.69 (13) | C2—C7—H7 | 119.4 |
O1—C3—C2 | 122.50 (13) | C7—C8—C9 | 119.91 (15) |
C4—C3—C2 | 114.81 (11) | C7—C8—H8 | 120.0 |
C5—C4—C3 | 119.62 (13) | C9—C8—H8 | 120.0 |
C5—C4—C6 | 121.16 (14) | C10—C9—C8 | 120.34 (14) |
C3—C4—C6 | 119.22 (13) | C10—C9—H9 | 119.8 |
C4—C5—O2 | 125.65 (13) | C8—C9—H9 | 119.8 |
C4—C5—H5 | 117.2 | C9—C10—C1 | 119.28 (14) |
O2—C5—H5 | 117.2 | C9—C10—H10 | 120.4 |
C4—C6—H6A | 109.5 | C1—C10—H10 | 120.4 |
C4—C6—H6B | 109.5 | C5—O2—C1 | 117.89 (11) |
D—H···A | D—H | H···A | D···A | D—H···A |
C5—H5···O1i | 0.93 | 2.70 | 3.4374 (19) | 137 |
C7—H7···O2ii | 0.93 | 2.69 | 3.3820 (19) | 132 |
Symmetry codes: (i) x+1, y, z; (ii) x−1, y, z. |
Experimental details
Crystal data | |
Chemical formula | C10H8O2 |
Mr | 160.16 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 296 |
a, b, c (Å) | 6.5284 (13), 7.2210 (14), 8.9834 (18) |
α, β, γ (°) | 75.137 (2), 78.169 (2), 80.895 (2) |
V (Å3) | 398.12 (14) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.12 × 0.10 × 0.08 |
Data collection | |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2001) |
Tmin, Tmax | 0.989, 0.993 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2771, 1394, 1143 |
Rint | 0.014 |
(sin θ/λ)max (Å−1) | 0.594 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.039, 0.116, 1.00 |
No. of reflections | 1394 |
No. of parameters | 111 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.18, −0.14 |
Computer programs: APEX2 (Bruker, 2004), SAINT-Plus (Bruker, 2001), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C5—H5···O1i | 0.93 | 2.70 | 3.4374 (19) | 136.8 |
C7—H7···O2ii | 0.93 | 2.69 | 3.3820 (19) | 132.0 |
Symmetry codes: (i) x+1, y, z; (ii) x−1, y, z. |
Acknowledgements
Financial support from the International Cooperation Program for Excellent Lectures of 2008 by Shandong Provincial Education Department is gratefully acknowledged.
References
Alaniz, J. R. de & Rovis, T. (2005). J. Am. Chem. Soc. 127, 6284—6289. Google Scholar
Bruker (2001). SAINT-Plus and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Bruker (2004). APEX2. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Patonay, T., Juhász-Tóth, É. & Bényei, A. (2002). Eur. J. Org. Chem. pp. 285—295. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Shi, G. F., Lu, R. H., Yang, Y. S., Li, C. L., Yang, A. M. & Cai, L. X. (2004). Chin. J. Struct. Chem. 23, 1164–1169. CAS Google Scholar
Takikawa, H. & Suzuki, K. (2007). Org. Lett. 9, 2713—2716. Web of Science CSD CrossRef Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The synthesis of chromanone derivatives has attracted continuous research interest due to their applications as vasodilator, anti-hypertensive, bronchodilator, heptaprotective, anti-tumor, anti-mutagenic, geroprotective and anti-diabetic agents (Shi et al., 2004). Here, we describe the cystallization and structural characterization of the title compound.
As shown in Fig 1. the two fused six membered rings are coplanar with a mean deviation of 0.0261 (1) Å from the plane through the non-hydrogen atoms of the rings. The carbonyl and methyl substituents of the pyran ring also lie close to that plane with deviations of 0.0557 (1) and 0.1405 (1) Å, respectively. The C=O and C—O bond distances, 1.367 (2) and 1.231 (2)—1.355 (2) Å, respectively, are in the normal range compared to reported chromanone derivatives (Takikawa & Suzuki, 2007; Patonay et al., 2002; Alaniz & Rovis, 2005). In the crystal structure, chains along the a axis are formed via the weak C—H···O contacts.