Literature DB >> 21582916

4-Hydr-oxy-3-[(2E)-3-(3,4,5-trimethoxy-phen-yl)prop-2-eno-yl]-2H-chromen-2-one.

Lassaad Mechi1, Samar Chtiba, Naceur Hamdi, Rached Ben Hassen.   

Abstract

A new chalcone of the coumarin, C(21)H(18)O(7), containing an annulated α-pyrone ring, was obtained by condensation of the borate complex of ac-yl(hydr-oxy)coumarin with trimethoxy-benzaldehyde. The structure exhibits intra-molecular hydrogen bonding between the hydroxyl oxygen and the ketonic oxygen in the coumarin group. The bicyclic coumarin fragment and the benzene ring form a dihedral angle of 17.1 (4)°. The crystal packing involves dimers inter-connected by C-H⋯O hydrogen bonding.

Entities:  

Year:  2009        PMID: 21582916      PMCID: PMC2969351          DOI: 10.1107/S1600536809022569

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For organic non-linear optical materials (NLO) of aromatic compounds with delocalized electron systems, see: Marcy et al. (1995 ▶); Zhengdong et al. (1997 ▶). For their non-linear susceptibilities, which are larger than those of inorganic optical materials, see: Chemla & Zyss (1987 ▶) and Lakshmana Perumal et al. (2002 ▶), and for their optical properties, see: Sarojini et al. (2006 ▶). For bond-length data, see: Traven et al.(2000 ▶). For the exclusive annulation of the α-pyrone ring, see Traven et al.(2007 ▶). For charge transfer from the phenyl ring to the coumarin system, see Indira et al. (2002 ▶); Sun & Cui (2008 ▶).

Experimental

Crystal data

C21H18O7 M = 382.35 Triclinic, a = 4.1370 (2) Å b = 8.1247 (2) Å c = 14.4101 (2) Å α = 74.549 (10)° β = 85.166 (10)° γ = 81.205 (10)° V = 460.87 (4) Å3 Z = 1 Mo Kα radiation μ = 0.10 mm−1 T = 293 K 0.16 × 0.13 × 0.10 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.981, T max = 0.99 3575 measured reflections 1974 independent reflections 1200 reflections with I > 2σ(I) R int = 0.038 2 standard reflections frequency: 120 min intensity decay: 1.1%

Refinement

R[F 2 > 2σ(F 2)] = 0.045 wR(F 2) = 0.136 S = 1.09 1974 reflections 257 parameters 3 restraints H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.12 e Å−3 Δρmin = −0.19 e Å−3 Data collection: CAD-4 EXPRESS (Duisenberg, 1992 ▶; Macíček & Yordanov, 1992 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809022569/hg2517sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809022569/hg2517Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C21H18O7Z = 1
Mr = 382.35F(000) = 200
Triclinic, P1Dx = 1.378 Mg m3
Hall symbol: P 1Melting point: 466 K
a = 4.1370 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.1247 (2) ÅCell parameters from 25 reflections
c = 14.4101 (2) Åθ = 10–15°
α = 74.549 (10)°µ = 0.10 mm1
β = 85.166 (10)°T = 293 K
γ = 81.205 (10)°Prism, pale yellow
V = 460.87 (4) Å30.16 × 0.13 × 0.10 mm
Enraf–Nonius CAD-4 diffractometer1200 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.038
graphiteθmax = 27.0°, θmin = 2.6°
ω/2θ scansh = −5→5
Absorption correction: ψ scan (North et al., 1968)k = −10→10
Tmin = 0.981, Tmax = 0.99l = −18→18
3575 measured reflections2 standard reflections every 120 min
1974 independent reflections intensity decay: 1.1%
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.136H atoms treated by a mixture of independent and constrained refinement
S = 1.09w = 1/[σ2(Fo2) + (0.0571P)2 + 0.0544P] where P = (Fo2 + 2Fc2)/3
1974 reflections(Δ/σ)max < 0.001
257 parametersΔρmax = 0.12 e Å3
3 restraintsΔρmin = −0.19 e Å3
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.
xyzUiso*/Ueq
O10.2654 (9)−0.1096 (4)0.5125 (2)0.0645 (9)
C80.4138 (11)0.1778 (6)0.4904 (3)0.0540 (12)
O40.5686 (10)0.4521 (5)0.4679 (2)0.0763 (11)
C70.3170 (11)0.2208 (6)0.3944 (3)0.0540 (12)
C40.1785 (11)0.0992 (6)0.3577 (3)0.0529 (12)
O30.3412 (9)0.3741 (5)0.3374 (2)0.0727 (10)
O70.9754 (9)0.6931 (4)0.8955 (2)0.0676 (10)
C140.8343 (12)0.5498 (6)0.7785 (3)0.0574 (12)
H140.89040.63860.72680.069*
C150.8677 (11)0.5584 (6)0.8721 (3)0.0550 (12)
C50.1553 (11)−0.0634 (6)0.4199 (3)0.0563 (12)
C110.5772 (13)0.2864 (7)0.6294 (3)0.0620 (13)
H110.54080.18370.67370.074*
C180.6315 (12)0.2749 (6)0.8389 (3)0.0550 (12)
H180.55270.18100.82770.066*
C170.6645 (11)0.2824 (6)0.9330 (3)0.0574 (13)
C100.5255 (12)0.3065 (6)0.5273 (3)0.0557 (12)
O60.8319 (9)0.4264 (5)1.0432 (2)0.0717 (10)
O20.5147 (10)−0.0605 (5)0.6284 (2)0.0818 (12)
O50.5901 (9)0.1598 (4)1.0150 (2)0.0676 (10)
C160.7836 (12)0.4233 (7)0.9499 (3)0.0574 (12)
C130.7168 (11)0.4083 (6)0.7613 (3)0.0533 (12)
C120.6741 (12)0.4098 (6)0.6607 (3)0.0567 (12)
H120.72010.50800.61390.068*
C90.4048 (11)0.0011 (6)0.5495 (3)0.0561 (12)
C60.0243 (14)−0.1878 (8)0.3905 (4)0.0703 (14)
H60.0077−0.29550.43240.084*
C30.0705 (12)0.1366 (7)0.2638 (3)0.0658 (14)
H30.08570.24420.22160.079*
C2−0.0584 (14)0.0129 (8)0.2341 (4)0.0771 (17)
H2−0.13000.03740.17180.093*
C191.0800 (14)0.8268 (7)0.8172 (4)0.0708 (14)
H19A1.15210.91280.84210.106*
H19B0.90080.87840.77620.106*
H19C1.25730.77880.78080.106*
C210.4581 (15)0.0164 (7)1.0030 (4)0.0723 (15)
H21A0.4186−0.06021.06490.108*
H21B0.6104−0.04330.96500.108*
H21C0.25590.05550.97080.108*
C1−0.0816 (14)−0.1476 (9)0.2969 (4)0.0784 (16)
H1−0.1693−0.22980.27620.094*
C200.5788 (16)0.5207 (8)1.0864 (4)0.0821 (16)
H20A0.63440.51551.15060.123*
H20B0.37940.47241.08900.123*
H20C0.54950.63851.04920.123*
H40.478 (14)0.441 (7)0.387 (4)0.086 (17)*
U11U22U33U12U13U23
O10.080 (2)0.064 (2)0.0421 (17)−0.0060 (18)−0.0092 (15)−0.0010 (15)
C80.057 (3)0.063 (3)0.036 (2)0.003 (2)−0.0032 (19)−0.009 (2)
O40.113 (3)0.070 (2)0.0431 (19)−0.015 (2)−0.0111 (19)−0.0063 (17)
C70.058 (3)0.063 (3)0.033 (2)0.001 (2)0.005 (2)−0.005 (2)
C40.054 (3)0.062 (3)0.037 (2)0.004 (2)−0.006 (2)−0.010 (2)
O30.107 (3)0.069 (2)0.0371 (17)−0.009 (2)−0.0028 (17)−0.0052 (16)
O70.081 (3)0.067 (2)0.055 (2)−0.0096 (18)−0.0085 (17)−0.0155 (17)
C140.062 (3)0.055 (3)0.047 (2)0.005 (2)−0.004 (2)−0.006 (2)
C150.052 (3)0.065 (3)0.047 (3)0.007 (2)−0.013 (2)−0.020 (2)
C50.053 (3)0.069 (3)0.042 (2)0.002 (2)0.001 (2)−0.013 (2)
C110.073 (3)0.068 (3)0.039 (2)0.003 (3)−0.006 (2)−0.008 (2)
C180.066 (3)0.051 (3)0.044 (2)0.001 (2)−0.011 (2)−0.009 (2)
C170.064 (3)0.062 (3)0.046 (2)0.006 (2)−0.007 (2)−0.019 (2)
C100.065 (3)0.065 (3)0.031 (2)0.002 (2)−0.0040 (19)−0.007 (2)
O60.084 (2)0.086 (2)0.0477 (18)0.0038 (19)−0.0186 (17)−0.0248 (18)
O20.119 (3)0.074 (2)0.0463 (19)−0.012 (2)−0.031 (2)0.0023 (16)
O50.093 (3)0.069 (2)0.0383 (16)−0.0153 (19)−0.0088 (16)−0.0046 (15)
C160.063 (3)0.065 (3)0.040 (2)0.005 (2)−0.013 (2)−0.012 (2)
C130.059 (3)0.054 (3)0.042 (2)0.010 (2)−0.009 (2)−0.012 (2)
C120.069 (3)0.062 (3)0.035 (2)0.000 (2)−0.009 (2)−0.008 (2)
C90.060 (3)0.062 (3)0.043 (3)−0.007 (2)−0.006 (2)−0.008 (2)
C60.072 (3)0.077 (3)0.062 (3)−0.014 (3)0.008 (3)−0.018 (3)
C30.066 (3)0.090 (4)0.040 (2)−0.003 (3)−0.008 (2)−0.016 (2)
C20.071 (4)0.107 (5)0.048 (3)0.001 (3)−0.011 (3)−0.016 (3)
C190.073 (4)0.073 (3)0.062 (3)−0.006 (3)−0.014 (3)−0.010 (3)
C210.094 (4)0.073 (3)0.051 (3)−0.022 (3)0.002 (3)−0.013 (3)
C10.071 (4)0.102 (5)0.072 (4)−0.013 (3)−0.006 (3)−0.039 (3)
C200.097 (4)0.095 (4)0.054 (3)−0.003 (3)0.000 (3)−0.026 (3)
O1—C91.375 (6)C17—O51.375 (6)
O1—C51.384 (5)C17—C161.397 (6)
C8—C71.410 (6)O6—C161.383 (5)
C8—C101.440 (7)O6—C201.403 (6)
C8—C91.466 (6)O2—C91.210 (5)
O4—C101.290 (6)O5—C211.415 (6)
O4—H41.28 (7)C13—C121.471 (6)
C7—O31.310 (5)C12—H120.9300
C7—C41.445 (6)C6—C11.392 (8)
C4—C51.396 (6)C6—H60.9300
C4—C31.402 (6)C3—C21.381 (8)
O3—H41.22 (7)C3—H30.9300
O7—C151.372 (6)C2—C11.387 (9)
O7—C191.431 (6)C2—H20.9300
C14—C151.389 (6)C19—H19A0.9600
C14—C131.401 (7)C19—H19B0.9600
C14—H140.9300C19—H19C0.9600
C15—C161.406 (6)C21—H21A0.9600
C5—C61.388 (7)C21—H21B0.9600
C11—C121.329 (7)C21—H21C0.9600
C11—C101.467 (6)C1—H10.9300
C11—H110.9300C20—H20A0.9600
C18—C171.392 (6)C20—H20B0.9600
C18—C131.398 (6)C20—H20C0.9600
C18—H180.9300
C9—O1—C5122.3 (4)C18—C13—C14119.8 (4)
C7—C8—C10119.6 (4)C18—C13—C12122.2 (4)
C7—C8—C9118.8 (4)C14—C13—C12118.0 (4)
C10—C8—C9121.7 (4)C11—C12—C13127.2 (4)
C10—O4—H4104 (3)C11—C12—H12116.4
O3—C7—C8120.7 (4)C13—C12—H12116.4
O3—C7—C4118.4 (4)O2—C9—O1115.4 (4)
C8—C7—C4120.9 (4)O2—C9—C8126.4 (5)
C5—C4—C3119.3 (4)O1—C9—C8118.2 (4)
C5—C4—C7117.4 (4)C5—C6—C1118.5 (5)
C3—C4—C7123.3 (4)C5—C6—H6120.8
C7—O3—H4102 (3)C1—C6—H6120.8
C15—O7—C19116.8 (4)C2—C3—C4119.7 (5)
C15—C14—C13120.5 (4)C2—C3—H3120.1
C15—C14—H14119.8C4—C3—H3120.1
C13—C14—H14119.8C3—C2—C1120.3 (5)
O7—C15—C14124.4 (4)C3—C2—H2119.9
O7—C15—C16116.2 (4)C1—C2—H2119.9
C14—C15—C16119.4 (4)O7—C19—H19A109.5
O1—C5—C6116.8 (4)O7—C19—H19B109.5
O1—C5—C4122.1 (4)H19A—C19—H19B109.5
C6—C5—C4121.1 (4)O7—C19—H19C109.5
C12—C11—C10122.3 (5)H19A—C19—H19C109.5
C12—C11—H11118.9H19B—C19—H19C109.5
C10—C11—H11118.9O5—C21—H21A109.5
C17—C18—C13120.1 (4)O5—C21—H21B109.5
C17—C18—H18120.0H21A—C21—H21B109.5
C13—C18—H18120.0O5—C21—H21C109.5
O5—C17—C18125.6 (4)H21A—C21—H21C109.5
O5—C17—C16114.5 (4)H21B—C21—H21C109.5
C18—C17—C16120.0 (4)C2—C1—C6121.0 (5)
O4—C10—C8118.3 (4)C2—C1—H1119.5
O4—C10—C11117.4 (5)C6—C1—H1119.5
C8—C10—C11124.2 (4)O6—C20—H20A109.5
C16—O6—C20115.6 (4)O6—C20—H20B109.5
C17—O5—C21117.3 (4)H20A—C20—H20B109.5
O6—C16—C17119.9 (4)O6—C20—H20C109.5
O6—C16—C15119.9 (4)H20A—C20—H20C109.5
C17—C16—C15120.2 (4)H20B—C20—H20C109.5
D—H···AD—HH···AD···AD—H···A
O3—H4···O41.22 (6)1.28 (6)2.437 (5)153 (5)
C2—H2···O5i0.932.523.427 (6)167
C20—H20B···O6ii0.962.523.439 (8)160
C19—H19C···O2iii0.962.483.135 (7)125
C11—H11···O20.932.272.873 (7)122
C12—H12···O40.932.422.772 (5)102
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O3—H4⋯O41.22 (6)1.28 (6)2.437 (5)153 (5)
C2—H2⋯O5i0.932.523.427 (6)167
C20—H20B⋯O6ii0.962.523.439 (8)160
C19—H19C⋯O2iii0.962.483.135 (7)125
C11—H11⋯O20.932.272.873 (7)122
C12—H12⋯O40.932.422.772 (5)102

Symmetry codes: (i) ; (ii) ; (iii) .

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