organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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(3E)-3-[(2E)-3-(4-Meth­­oxy­phen­yl)prop-2-enyl­­idene]-2,3-di­hydro-4H-chromen-4-one

aDepartment of Physics, Bharathi Women's College, Chennai-108, Tamilnadu, India, bDepartment of Chemistry, Madras Christian College, Chennai-59, Tamilnadu, India, and cPG and Research Department of Physics, Queen Mary's College, Chennai-4, Tamilnadu, India
*Correspondence e-mail: guqmc@yahoo.com

Edited by W. T. A. Harrison, University of Aberdeen, Scotland (Received 29 May 2018; accepted 5 June 2018; online 8 June 2018)

In the title compound, C19H16O3, the dihedral angle between the chromanone moiety and the meth­oxy phenyl ring is 16.47 (1)°. In the crystal, the mol­ecules are linked by pairs of C—H⋯O hydrogen bonds, generating R22(14) inversion dimers; further C—H⋯O hydrogen bonds connect the dimers into [100] double chains.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

A large number of naturally occurring chalcones are polyhy­droxy­lated in the aryl rings (Jasinski et al., 2010[Jasinski, J. P., Pek, A. E., Narayana, B., Kamath, P. K. & Yathirajan, H. S. (2010). Acta Cryst. E66, o1995.]). The radical quenching properties of the phenolic groups present in many chalcones have raised inter­est in using these compounds or chalcone-rich plant extracts as drugs or food preservatives (Dhar, 1981[Dhar, D. N. (1981). The Chemistry of Chalcones and Related Compounds. New York: John Wiley.]). As part of our studies in this area, we now describe the synthesis and structure of the title compound (Fig. 1[link]).

[Figure 1]
Figure 1
The mol­ecular structure of the title compound, with displacement ellipsoids drawn at the 30% probability level.

The tetra­hydro-4H-pyran-4-one ring adopts a sofa conformation with the methyl­ene group (atom C12) displaced from the other atoms. The C—O and C=O distances in the chromanone moiety are typical of those in previously reported structures (Gopaul et al., 2012[Gopaul, K., Shaikh, M. M., Koorbanally, N. A., Ramjugernath, D. & Omondi, B. (2012). Acta Cryst. E68, o1972.]). The dihedral angle between the the meth­oxy phenyl ring and chromanone ring system (all atoms) is 16.47 (1)°.

In the crystal, the mol­ecules are linked by C—H⋯O hydrogen bonds (Table 1[link]). Inversion dimers featuring [R_{2}^{2}] (14) loops arise from the very weak C8—H8⋯O2 bonds and the dimers are linked into [100] double chains by the C17—H17⋯O3 bonds (Figs. 2[link] and 3[link]).

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C8—H8⋯O2i 0.93 2.59 3.362 (5) 141
C17—H17⋯O3ii 0.93 2.53 3.342 (5) 146
Symmetry codes: (i) -x+2, -y, -z+1; (ii) x+1, y, z.
[Figure 2]
Figure 2
The packing of the mol­ecules in the crystal structure. The dashed lines indicate hydrogen bonds.
[Figure 3]
Figure 3
A partial view of the packing of the title compound showing the hydrogen bonds as dashed lines.

Synthesis and crystallization

In a 250 ml round-bottomed flask, a mixture of 4-chromanone (1.4 g, 0.010 mol) and meth­oxy cinnamaldehyde (1.5 g, 0.010 mol) was added to absolute alcohol and stirred for five minutes. Then, a solution of NaOH (0.3 g, 10 ml) was added and stirred for 2 h. The mixture was kept overnight at room temperature and then dumped into crushed ice, leading to a precipitate of the title compound, which was isolated by filtration and washed with distilled water several times to remove any trace of NaOH remaining in the product. The crude chalcone derivative was recrystallized twice from ethyl methyl­ketone solution to give colourless blocks of the title compound (yield: 80%; mp: 135°C).

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula C19H16O3
Mr 292.32
Crystal system, space group Triclinic, P[\overline{1}]
Temperature (K) 296
a, b, c (Å) 6.8573 (12), 7.4073 (14), 15.550 (3)
α, β, γ (°) 87.843 (6), 78.892 (5), 72.347 (5)
V3) 738.4 (2)
Z 2
Radiation type Mo Kα
μ (mm−1) 0.09
Crystal size (mm) 0.15 × 0.15 × 0.10
 
Data collection
Diffractometer Bruker APEXIII CMOS
Absorption correction Multi-scan (SADABS)
Tmin, Tmax 0.987, 0.991
No. of measured, independent and observed [I > 2σ(I)] reflections 20521, 2589, 1609
Rint 0.092
(sin θ/λ)max−1) 0.595
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.080, 0.251, 1.12
No. of reflections 2580
No. of parameters 201
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.24, −0.25
Computer programs: APEX3 and SAINT (Bruker, 2016[Bruker (2016). APEX3, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]), SHELXT2014 (Sheldrick, 2015a[Sheldrick, G. M. (2015a). Acta Cryst. A71, 3-8.]), SHELXL2014 (Sheldrick, 2015b[Sheldrick, G. M. (2015b). Acta Cryst. C71, 3-8.]) and ORTEP-3 for Windows (Farrugia, 2012[Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849-854.]).

Structural data


Computing details top

Data collection: APEX3 (Bruker, 2016); cell refinement: SAINT (Bruker, 2016); data reduction: SAINT (Bruker, 2016); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2015b).

(3E)-3-[(2E)-3-(4-Methoxyphenyl)prop-2-enylidene]-2,3-dihydro-4H-chromen-4-one top
Crystal data top
C19H16O3Z = 2
Mr = 292.32F(000) = 308
Triclinic, P1Dx = 1.315 Mg m3
a = 6.8573 (12) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.4073 (14) ÅCell parameters from 7704 reflections
c = 15.550 (3) Åθ = 3.2–26.7°
α = 87.843 (6)°µ = 0.09 mm1
β = 78.892 (5)°T = 296 K
γ = 72.347 (5)°Block, colourless
V = 738.4 (2) Å30.15 × 0.15 × 0.10 mm
Data collection top
Bruker APEXIII CMOS
diffractometer
1609 reflections with I > 2σ(I)
φ and ω scansRint = 0.092
Absorption correction: multi-scan
(SADABS)
θmax = 25.0°, θmin = 2.9°
Tmin = 0.987, Tmax = 0.991h = 88
20521 measured reflectionsk = 88
2589 independent reflectionsl = 1818
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.080 w = 1/[σ2(Fo2) + (0.0879P)2 + 0.7561P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.251(Δ/σ)max < 0.001
S = 1.12Δρmax = 0.24 e Å3
2580 reflectionsΔρmin = 0.25 e Å3
201 parametersExtinction correction: SHELXL2014 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.09 (3)
Primary atom site location: structure-invariant direct methods
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. H atoms were positioned geometrically and treated as riding on their parent atoms and refined with, C—H distance of 0.93–0.97 Å, with Uiso(H)= 1.5 Ueq(c-methyl),and Uiso(H)= 1.2Ueq(C) for other H atom.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.3016 (8)0.3018 (7)0.8572 (3)0.0924 (15)
H1A0.23250.37440.88330.139*
H1B0.24540.17010.86930.139*
H1C0.44810.34400.88140.139*
C20.0725 (6)0.2889 (5)0.7197 (3)0.0597 (10)
C30.0532 (6)0.3314 (5)0.6320 (3)0.0628 (10)
H30.17250.38330.60850.075*
C40.1369 (6)0.2990 (5)0.5794 (3)0.0605 (10)
H40.14510.32910.52050.073*
C50.3203 (6)0.2214 (5)0.6116 (2)0.0539 (9)
C80.5250 (6)0.1928 (5)0.5585 (3)0.0596 (10)
H80.63780.13650.58550.072*
C90.5699 (6)0.2387 (5)0.4746 (3)0.0593 (10)
H90.45940.29370.44620.071*
C100.7755 (6)0.2092 (5)0.4260 (3)0.0567 (10)
H100.88380.15660.45600.068*
C110.8297 (5)0.2488 (5)0.3421 (2)0.0524 (9)
C191.0486 (6)0.2170 (5)0.3014 (3)0.0555 (10)
C181.0927 (5)0.2306 (5)0.2055 (2)0.0537 (9)
C171.2938 (6)0.2108 (6)0.1601 (3)0.0682 (11)
H171.40000.19820.19130.082*
C161.3383 (8)0.2095 (7)0.0702 (3)0.0831 (13)
H161.47310.19760.04050.100*
C151.1807 (9)0.2259 (8)0.0246 (3)0.0949 (16)
H151.21050.22340.03630.114*
C70.1057 (7)0.2083 (5)0.7534 (3)0.0651 (11)
H70.09580.17570.81200.078*
C60.2986 (6)0.1764 (5)0.6996 (3)0.0629 (11)
H60.41770.12300.72300.076*
C140.9823 (8)0.2457 (8)0.0671 (3)0.0875 (14)
H140.87750.25670.03530.105*
C130.9370 (6)0.2496 (6)0.1575 (3)0.0635 (10)
C120.6740 (6)0.3353 (6)0.2856 (3)0.0693 (11)
H12A0.54410.31020.31060.083*
H12B0.64760.47150.28620.083*
O10.2702 (5)0.3267 (5)0.7659 (2)0.0835 (10)
O21.1894 (4)0.1790 (4)0.3435 (2)0.0788 (10)
O30.7373 (4)0.2668 (4)0.19599 (18)0.0742 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.100 (4)0.077 (3)0.083 (3)0.016 (3)0.006 (3)0.005 (3)
C20.061 (2)0.050 (2)0.070 (3)0.0191 (17)0.0130 (19)0.0013 (18)
C30.060 (2)0.055 (2)0.076 (3)0.0138 (17)0.024 (2)0.0037 (19)
C40.063 (2)0.054 (2)0.067 (2)0.0182 (18)0.0183 (19)0.0042 (18)
C50.060 (2)0.0371 (18)0.069 (2)0.0184 (16)0.0165 (18)0.0016 (16)
C80.063 (2)0.044 (2)0.077 (3)0.0185 (17)0.0219 (19)0.0022 (18)
C90.058 (2)0.043 (2)0.079 (3)0.0128 (16)0.0227 (19)0.0006 (18)
C100.056 (2)0.0421 (19)0.074 (3)0.0129 (16)0.0214 (18)0.0018 (17)
C110.055 (2)0.0378 (18)0.068 (2)0.0145 (15)0.0211 (17)0.0020 (16)
C190.054 (2)0.0365 (18)0.082 (3)0.0156 (15)0.0239 (19)0.0010 (16)
C180.056 (2)0.0395 (18)0.071 (2)0.0181 (15)0.0192 (18)0.0013 (16)
C170.068 (3)0.059 (2)0.086 (3)0.0256 (19)0.023 (2)0.004 (2)
C160.078 (3)0.090 (3)0.086 (3)0.037 (3)0.008 (2)0.002 (3)
C150.100 (4)0.120 (4)0.073 (3)0.047 (3)0.014 (3)0.005 (3)
C70.083 (3)0.057 (2)0.062 (2)0.029 (2)0.019 (2)0.0067 (18)
C60.071 (3)0.049 (2)0.075 (3)0.0195 (18)0.028 (2)0.0075 (18)
C140.088 (3)0.112 (4)0.075 (3)0.039 (3)0.029 (3)0.006 (3)
C130.061 (2)0.062 (2)0.074 (3)0.0238 (18)0.020 (2)0.0042 (19)
C120.058 (2)0.070 (3)0.081 (3)0.0162 (19)0.021 (2)0.001 (2)
O10.074 (2)0.090 (2)0.080 (2)0.0201 (16)0.0068 (16)0.0035 (16)
O20.0637 (18)0.090 (2)0.087 (2)0.0200 (15)0.0310 (15)0.0082 (16)
O30.0652 (18)0.092 (2)0.0743 (19)0.0280 (15)0.0279 (14)0.0066 (15)
Geometric parameters (Å, º) top
C1—O11.408 (5)C11—C121.492 (5)
C1—H1A0.9600C19—O21.227 (4)
C1—H1B0.9600C19—C181.469 (5)
C1—H1C0.9600C18—C131.386 (5)
C2—O11.357 (5)C18—C171.390 (5)
C2—C31.378 (5)C17—C161.373 (6)
C2—C71.380 (6)C17—H170.9300
C3—C41.356 (5)C16—C151.376 (7)
C3—H30.9300C16—H160.9300
C4—C51.395 (5)C15—C141.360 (6)
C4—H40.9300C15—H150.9300
C5—C61.386 (5)C7—C61.380 (5)
C5—C81.444 (5)C7—H70.9300
C8—C91.337 (5)C6—H60.9300
C8—H80.9300C14—C131.380 (6)
C9—C101.421 (5)C14—H140.9300
C9—H90.9300C13—O31.354 (4)
C10—C111.334 (5)C12—O31.439 (5)
C10—H100.9300C12—H12A0.9700
C11—C191.462 (5)C12—H12B0.9700
O1—C1—H1A109.5C13—C18—C17118.3 (4)
O1—C1—H1B109.5C13—C18—C19120.5 (3)
H1A—C1—H1B109.5C17—C18—C19121.0 (3)
O1—C1—H1C109.5C16—C17—C18121.1 (4)
H1A—C1—H1C109.5C16—C17—H17119.4
H1B—C1—H1C109.5C18—C17—H17119.4
O1—C2—C3116.0 (3)C17—C16—C15119.1 (4)
O1—C2—C7125.1 (4)C17—C16—H16120.5
C3—C2—C7118.9 (4)C15—C16—H16120.5
C4—C3—C2121.2 (4)C14—C15—C16121.2 (5)
C4—C3—H3119.4C14—C15—H15119.4
C2—C3—H3119.4C16—C15—H15119.4
C3—C4—C5121.5 (4)C2—C7—C6119.7 (4)
C3—C4—H4119.3C2—C7—H7120.1
C5—C4—H4119.3C6—C7—H7120.1
C6—C5—C4116.8 (4)C7—C6—C5122.0 (4)
C6—C5—C8120.2 (3)C7—C6—H6119.0
C4—C5—C8123.0 (4)C5—C6—H6119.0
C9—C8—C5127.0 (4)C15—C14—C13119.7 (4)
C9—C8—H8116.5C15—C14—H14120.1
C5—C8—H8116.5C13—C14—H14120.1
C8—C9—C10124.4 (4)O3—C13—C14116.9 (4)
C8—C9—H9117.8O3—C13—C18122.5 (4)
C10—C9—H9117.8C14—C13—C18120.6 (4)
C11—C10—C9127.0 (4)O3—C12—C11114.2 (3)
C11—C10—H10116.5O3—C12—H12A108.7
C9—C10—H10116.5C11—C12—H12A108.7
C10—C11—C19121.0 (3)O3—C12—H12B108.7
C10—C11—C12122.8 (3)C11—C12—H12B108.7
C19—C11—C12116.1 (3)H12A—C12—H12B107.6
O2—C19—C11123.0 (4)C2—O1—C1119.0 (4)
O2—C19—C18121.0 (3)C13—O3—C12116.3 (3)
C11—C19—C18116.0 (3)
O1—C2—C3—C4179.8 (3)C18—C17—C16—C150.8 (7)
C7—C2—C3—C41.3 (6)C17—C16—C15—C140.8 (8)
C2—C3—C4—C50.0 (6)O1—C2—C7—C6179.9 (3)
C3—C4—C5—C61.0 (5)C3—C2—C7—C61.6 (6)
C3—C4—C5—C8177.1 (3)C2—C7—C6—C50.6 (6)
C6—C5—C8—C9176.1 (3)C4—C5—C6—C70.8 (5)
C4—C5—C8—C92.0 (6)C8—C5—C6—C7177.4 (3)
C5—C8—C9—C10179.1 (3)C16—C15—C14—C130.0 (8)
C8—C9—C10—C11178.7 (3)C15—C14—C13—O3179.1 (4)
C9—C10—C11—C19177.7 (3)C15—C14—C13—C180.9 (7)
C9—C10—C11—C120.6 (6)C17—C18—C13—O3179.0 (3)
C10—C11—C19—O210.5 (5)C19—C18—C13—O33.7 (5)
C12—C11—C19—O2166.8 (3)C17—C18—C13—C141.0 (6)
C10—C11—C19—C18168.7 (3)C19—C18—C13—C14174.3 (4)
C12—C11—C19—C1814.0 (4)C10—C11—C12—O3143.7 (3)
O2—C19—C18—C13171.7 (3)C19—C11—C12—O339.0 (5)
C11—C19—C18—C137.5 (5)C3—C2—O1—C1174.7 (4)
O2—C19—C18—C173.5 (5)C7—C2—O1—C17.0 (6)
C11—C19—C18—C17177.3 (3)C14—C13—O3—C12159.3 (4)
C13—C18—C17—C160.2 (6)C18—C13—O3—C1222.6 (5)
C19—C18—C17—C16175.2 (4)C11—C12—O3—C1343.5 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O2i0.932.593.362 (5)141
C17—H17···O3ii0.932.533.342 (5)146
Symmetry codes: (i) x+2, y, z+1; (ii) x+1, y, z.
 

Acknowledgements

The authors thank the Central Instrumentation Facility, Queen Mary's College, Chennai-4 for providing computing facilities and SAIF, IIT, Madras, for the X-ray data collection.

References

First citationBruker (2016). APEX3, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationDhar, D. N. (1981). The Chemistry of Chalcones and Related Compounds. New York: John Wiley.  Google Scholar
First citationFarrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationGopaul, K., Shaikh, M. M., Koorbanally, N. A., Ramjugernath, D. & Omondi, B. (2012). Acta Cryst. E68, o1972.  CSD CrossRef IUCr Journals Google Scholar
First citationJasinski, J. P., Pek, A. E., Narayana, B., Kamath, P. K. & Yathirajan, H. S. (2010). Acta Cryst. E66, o1995.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
First citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar

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