organic compounds
Ethyl (E)-2-(2,7-dimethyl-5-oxo-4H,5H-pyrano[4,3-b]pyran-4-ylidene)acetate
aLaboratoire de Chimie Organique et Analytique, Université Sultan Moulay Slimane, Faculté des Sciences et Techniques, Béni-Mellal, BP 523, Morocco, and bLaboratoire de Chimie du Solide Appliquée, Faculty of Sciences, Mohammed V University in Rabat, Avenue Ibn Battouta, BP 1014, Rabat, Morocco
*Correspondence e-mail: o_bassou@yahoo.com
In the title compound, C14H14O5, the two heterocyclic rings are coplanar (r.m.s. deviation = 0.008 Å), with the largest deviation from the mean plane being 0.012 (1) Å. The mean plane through the acetate group is inclined slightly with respect to the oxopyrano[4,3-b]pyran-4-yl system, as indicated by the dihedral angle of 1.70 (7)° between them. Two intramolecular hydrogen bonds, completing S(6) ring motifs, are observed in the molecule. In the crystal, molecules are linked by weak C—H⋯O hydrogen bonds involving the same acceptor atom, forming chains propagating along the c-axis direction and enclosing R21(6) ring motifs. The chains are linked via offset π–π interactions [intercentroid distance = 3.622 (1) Å], involving inversion-related oxopyrano[4,3-b]pyran-4-yl ring systems, forming slabs parallel to the bc plane.
Keywords: crystal structure; oxopyrano[4,3-b]pyran-4-ylidene; heterocyclic compounds; C—H⋯O hydrogen bonding; offset π–π interactions.
CCDC reference: 1531805
Structure description
Pyrones are among the most important heterocyclic structures in medicinal chemistry and specifically, 2-pyrones can be found in a wide range of medicinally significant natural products (Lee et al., 2000; Fairlamb et al., 2004; McGlacken & Fairlamb, 2005; Perchellet et al., 1998; Defant et al., 2015). As heterocyclic aromatic they have a high acidity and dense functionality, which leads to a diverse reactivity profile. This means that 4-hydroxy-2-pyrones are also useful precursors to a number of other structural units and versatile intermediates in organic synthesis (Burns et al., 2014; Aggarwal et al., 2013).
The molecule of the title compound is build up from a bicyclic oxopyrano[4,3-b]pyran-4-ylidene ring system linked to two methyl groups and one acetate group, as shown in Fig. 1. The fused heterocyclic rings are virtually coplanar with the maximum deviation from the mean plane being 0.012 (2) Å for atom C9. The oxopyrano[4,3-b]pyran-4-yl system makes a dihedral angle of 1.70 (7)° with the mean plane through the acetate group. Two intramolecular C—H⋯O contacts, enclosing S(6) ring motifs, are observed in the molecule (Fig. 1 and Table 1).
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In the crystal, molecules are linked by weak C—H⋯O hydrogen bonds involving the same acceptor atom (see Table 1), forming chains propagating along the c-axis direction and enclosing (6) ring motifs (Fig. 2). The chains are linked via offset π–π interactions involving inversion-related oxopyrano[4,3-b]pyran-4-yl ring systems, [intercentroid distance = 3.622 (1) Å], forming slabs parallel to the bc plane (Fig. 3).
Synthesis and crystallization
To a solution of 6-aminouracil (1 mmol) in 25 ml of ethanol, 4-hydroxy-6-methyl-2-pyrone (1.1 mmol) and drops of triethylamine were added. The mixture was refluxed for 8 h. After cooling to room temperature, the solvent was removed under reduced pressure. The crude product was purified on silica gel using hexane:ethyl acetate (2/8) as
The title compound was recrystallized from ethanol giving colourless block-like crystals (yield: 54%, m.p. 376 K). It should be noted that in the reaction of 6-aminouracil with 4-hydroxy-6-methyl-2-pyrone, under reflux of ethanol in the presence of Et3N, we observed another competitive reaction between two molecules of 4-hydroxy-6 -methyl-2-pyrone, this reaction is kinetically favored over the first reaction. Details are given in the Supporting information.Refinement
Crystal data, data collection and structure .
details are summarized in Table 2Structural data
CCDC reference: 1531805
https://doi.org/10.1107/S2414314617002085/su4128sup1.cif
contains datablocks I, Global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314617002085/su4128Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314617002085/su4128Isup3.cml
Supporting information file. DOI: https://doi.org/10.1107/S2414314617002085/su4128sup4.pdf
Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); 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) and Mercury (Macrae et al., 2008); software used to prepare material for publication: PLATON (Spek, 2009) and publCIF (Westrip, 2010).C14H14O5 | Dx = 1.310 Mg m−3 |
Mr = 262.25 | Melting point: 376 K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.5679 (12) Å | Cell parameters from 2939 reflections |
b = 11.4330 (13) Å | θ = 2.5–27.1° |
c = 12.7993 (15) Å | µ = 0.10 mm−1 |
β = 108.257 (4)° | T = 296 K |
V = 1329.6 (3) Å3 | Block, colourless |
Z = 4 | 0.32 × 0.26 × 0.21 mm |
F(000) = 552 |
Bruker X8 APEX diffractometer | 2939 independent reflections |
Radiation source: fine-focus sealed tube | 1909 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.037 |
φ and ω scans | θmax = 27.1°, θmin = 2.5° |
Absorption correction: multi-scan (SADABS; Krause et al., 2015) | h = −12→12 |
Tmin = 0.663, Tmax = 0.746 | k = −14→14 |
16353 measured reflections | l = −13→16 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.043 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.137 | H-atom parameters constrained |
S = 1.03 | w = 1/[σ2(Fo2) + (0.0699P)2 + 0.1184P] where P = (Fo2 + 2Fc2)/3 |
2939 reflections | (Δ/σ)max < 0.001 |
180 parameters | Δρmax = 0.17 e Å−3 |
0 restraints | Δρmin = −0.15 e Å−3 |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.7176 (3) | 0.4822 (2) | 1.10578 (18) | 0.1053 (9) | |
H1A | 0.7896 | 0.5034 | 1.1742 | 0.158* | |
H1B | 0.6384 | 0.5376 | 1.0884 | 0.158* | |
H1C | 0.6801 | 0.4055 | 1.1122 | 0.158* | |
C2 | 0.7864 (2) | 0.4820 (2) | 1.01765 (16) | 0.0901 (7) | |
H2A | 0.8250 | 0.5590 | 1.0105 | 0.108* | |
H2B | 0.8670 | 0.4263 | 1.0345 | 0.108* | |
C3 | 0.7183 (2) | 0.43027 (15) | 0.82769 (14) | 0.0584 (5) | |
C4 | 0.59172 (17) | 0.40172 (14) | 0.73274 (13) | 0.0523 (4) | |
H4 | 0.5000 | 0.3988 | 0.7433 | 0.063* | |
C5 | 0.59770 (16) | 0.37903 (12) | 0.62997 (12) | 0.0442 (4) | |
C6 | 0.73205 (17) | 0.38065 (13) | 0.60097 (14) | 0.0496 (4) | |
H6 | 0.8198 | 0.3960 | 0.6563 | 0.060* | |
C7 | 0.73778 (16) | 0.36155 (14) | 0.50021 (14) | 0.0508 (4) | |
C8 | 0.48137 (16) | 0.33460 (12) | 0.43348 (13) | 0.0453 (4) | |
C9 | 0.46732 (15) | 0.35306 (12) | 0.53543 (12) | 0.0420 (4) | |
C10 | 0.31964 (17) | 0.34808 (14) | 0.54336 (13) | 0.0488 (4) | |
C11 | 0.22563 (17) | 0.30720 (14) | 0.34851 (13) | 0.0515 (4) | |
C12 | 0.35992 (17) | 0.31137 (14) | 0.33862 (14) | 0.0519 (4) | |
H12 | 0.3739 | 0.2993 | 0.2707 | 0.062* | |
C13 | 0.08513 (19) | 0.2864 (2) | 0.26002 (16) | 0.0752 (6) | |
H13A | 0.0281 | 0.3571 | 0.2461 | 0.130 (10)* | |
H13B | 0.0310 | 0.2259 | 0.2824 | 0.109 (8)* | |
H13C | 0.1052 | 0.2627 | 0.1942 | 0.100 (7)* | |
C14 | 0.8690 (2) | 0.36234 (18) | 0.46180 (18) | 0.0702 (6) | |
H14A | 0.8813 | 0.2865 | 0.4338 | 0.109 (8)* | |
H14B | 0.9548 | 0.3815 | 0.5222 | 0.100 (7)* | |
H14C | 0.8558 | 0.4196 | 0.4046 | 0.102 (8)* | |
O1 | 0.67347 (14) | 0.44936 (12) | 0.91578 (10) | 0.0756 (4) | |
O2 | 0.84654 (14) | 0.43692 (14) | 0.83266 (11) | 0.0822 (5) | |
O3 | 0.61171 (11) | 0.33840 (10) | 0.41328 (9) | 0.0557 (3) | |
O4 | 0.28225 (13) | 0.36313 (13) | 0.62435 (10) | 0.0714 (4) | |
O5 | 0.20544 (11) | 0.32427 (10) | 0.44793 (9) | 0.0546 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.110 (2) | 0.129 (2) | 0.0675 (13) | 0.0096 (16) | 0.0138 (14) | −0.0315 (14) |
C2 | 0.0758 (15) | 0.1147 (18) | 0.0611 (12) | 0.0024 (13) | −0.0055 (11) | −0.0259 (12) |
C3 | 0.0485 (11) | 0.0619 (11) | 0.0556 (10) | 0.0028 (8) | 0.0030 (8) | −0.0001 (8) |
C4 | 0.0406 (9) | 0.0584 (10) | 0.0531 (10) | −0.0007 (7) | 0.0079 (7) | 0.0046 (7) |
C5 | 0.0348 (8) | 0.0411 (8) | 0.0515 (9) | 0.0014 (6) | 0.0061 (7) | 0.0063 (6) |
C6 | 0.0318 (8) | 0.0524 (9) | 0.0573 (10) | 0.0009 (6) | 0.0034 (7) | 0.0027 (7) |
C7 | 0.0304 (8) | 0.0516 (9) | 0.0676 (11) | 0.0000 (6) | 0.0111 (8) | −0.0013 (8) |
C8 | 0.0329 (8) | 0.0445 (8) | 0.0577 (10) | −0.0009 (6) | 0.0132 (7) | −0.0020 (7) |
C9 | 0.0326 (8) | 0.0417 (8) | 0.0484 (9) | 0.0006 (6) | 0.0079 (7) | 0.0046 (6) |
C10 | 0.0350 (8) | 0.0586 (10) | 0.0495 (9) | −0.0038 (7) | 0.0084 (8) | 0.0085 (7) |
C11 | 0.0386 (9) | 0.0580 (10) | 0.0532 (9) | −0.0056 (7) | 0.0075 (7) | −0.0067 (7) |
C12 | 0.0400 (9) | 0.0636 (10) | 0.0510 (9) | −0.0047 (7) | 0.0125 (7) | −0.0103 (7) |
C13 | 0.0416 (10) | 0.1101 (17) | 0.0657 (12) | −0.0123 (11) | 0.0050 (9) | −0.0200 (11) |
C14 | 0.0401 (10) | 0.0861 (15) | 0.0874 (14) | −0.0025 (9) | 0.0243 (10) | −0.0080 (12) |
O1 | 0.0609 (8) | 0.1019 (10) | 0.0552 (7) | 0.0007 (7) | 0.0055 (6) | −0.0196 (7) |
O2 | 0.0457 (8) | 0.1220 (12) | 0.0674 (9) | −0.0020 (7) | 0.0014 (7) | −0.0103 (8) |
O3 | 0.0336 (6) | 0.0732 (8) | 0.0607 (7) | −0.0042 (5) | 0.0151 (5) | −0.0125 (5) |
O4 | 0.0439 (7) | 0.1199 (11) | 0.0522 (7) | −0.0059 (7) | 0.0176 (6) | 0.0078 (7) |
O5 | 0.0321 (6) | 0.0744 (8) | 0.0546 (7) | −0.0077 (5) | 0.0097 (5) | −0.0009 (5) |
C1—C2 | 1.473 (3) | C7—C14 | 1.485 (2) |
C1—H1A | 0.9600 | C8—O3 | 1.3513 (18) |
C1—H1B | 0.9600 | C8—C9 | 1.369 (2) |
C1—H1C | 0.9600 | C8—C12 | 1.418 (2) |
C2—O1 | 1.458 (2) | C9—C10 | 1.449 (2) |
C2—H2A | 0.9700 | C10—O4 | 1.2102 (19) |
C2—H2B | 0.9700 | C10—O5 | 1.3869 (18) |
C3—O2 | 1.211 (2) | C11—C12 | 1.331 (2) |
C3—O1 | 1.344 (2) | C11—O5 | 1.3596 (19) |
C3—C4 | 1.459 (2) | C11—C13 | 1.481 (2) |
C4—C5 | 1.359 (2) | C12—H12 | 0.9300 |
C4—H4 | 0.9300 | C13—H13A | 0.9600 |
C5—C6 | 1.446 (2) | C13—H13B | 0.9600 |
C5—C9 | 1.471 (2) | C13—H13C | 0.9600 |
C6—C7 | 1.326 (2) | C14—H14A | 0.9600 |
C6—H6 | 0.9300 | C14—H14B | 0.9600 |
C7—O3 | 1.3864 (18) | C14—H14C | 0.9600 |
C2—C1—H1A | 109.5 | C9—C8—C12 | 123.09 (14) |
C2—C1—H1B | 109.5 | C8—C9—C10 | 116.72 (14) |
H1A—C1—H1B | 109.5 | C8—C9—C5 | 120.27 (13) |
C2—C1—H1C | 109.5 | C10—C9—C5 | 123.00 (14) |
H1A—C1—H1C | 109.5 | O4—C10—O5 | 114.81 (14) |
H1B—C1—H1C | 109.5 | O4—C10—C9 | 127.65 (15) |
O1—C2—C1 | 107.53 (19) | O5—C10—C9 | 117.54 (14) |
O1—C2—H2A | 110.2 | C12—C11—O5 | 120.55 (14) |
C1—C2—H2A | 110.2 | C12—C11—C13 | 127.24 (17) |
O1—C2—H2B | 110.2 | O5—C11—C13 | 112.20 (14) |
C1—C2—H2B | 110.2 | C11—C12—C8 | 118.81 (16) |
H2A—C2—H2B | 108.5 | C11—C12—H12 | 120.6 |
O2—C3—O1 | 122.03 (16) | C8—C12—H12 | 120.6 |
O2—C3—C4 | 128.38 (18) | C11—C13—H13A | 109.5 |
O1—C3—C4 | 109.59 (15) | C11—C13—H13B | 109.5 |
C5—C4—C3 | 124.97 (16) | H13A—C13—H13B | 109.5 |
C5—C4—H4 | 117.5 | C11—C13—H13C | 109.5 |
C3—C4—H4 | 117.5 | H13A—C13—H13C | 109.5 |
C4—C5—C6 | 123.81 (14) | H13B—C13—H13C | 109.5 |
C4—C5—C9 | 123.55 (14) | C7—C14—H14A | 109.5 |
C6—C5—C9 | 112.62 (14) | C7—C14—H14B | 109.5 |
C7—C6—C5 | 123.96 (15) | H14A—C14—H14B | 109.5 |
C7—C6—H6 | 118.0 | C7—C14—H14C | 109.5 |
C5—C6—H6 | 118.0 | H14A—C14—H14C | 109.5 |
C6—C7—O3 | 121.42 (14) | H14B—C14—H14C | 109.5 |
C6—C7—C14 | 128.16 (16) | C3—O1—C2 | 116.73 (16) |
O3—C7—C14 | 110.42 (15) | C8—O3—C7 | 118.41 (12) |
O3—C8—C9 | 123.32 (14) | C11—O5—C10 | 123.28 (13) |
O3—C8—C12 | 113.58 (14) |
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4···O4 | 0.93 | 2.20 | 2.883 (2) | 130 |
C6—H6···O2 | 0.93 | 2.24 | 2.894 (2) | 127 |
C12—H12···O4i | 0.93 | 2.59 | 3.283 (2) | 132 |
C13—H13C···O4i | 0.96 | 2.59 | 3.398 (2) | 143 |
Symmetry code: (i) x, −y+1/2, z−1/2. |
Acknowledgements
The authors thank the Unit of Support for Technical and Scientific Research (UATRS, CNRST) for the X-ray measurements.
Funding information
Funding for this research was provided by: University Sultan Moulay Slimane, Beni-Mellal, Morocco
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