organic compounds
10-Phenyl-6b,7,8,9,9a,10-hexahydro-6H-cyclopenta[4,5]pyrano[3,2-c]chromen-6,9-dione
aBeijing National Laboratory for Molecular Science (BNLMS), CAS Key Laboratory for Molecular Recognition and Function, Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, People's Republic of China
*Correspondence e-mail: lliu@iccas.ac.cn
In the title compound, C21H16O4, the dihedral angle between the phenyl ring and the 2H-chromene ring system is 59.8 (2)°. The crystal packing is stabilized by weak π–π stacking interactions [centroid–centroid distances = 3.667 (2) Å] and intermolecular C—H⋯O hydrogen-bonding interactions.
Related literature
For applications of coumarin, see: Vu et al. (2008); Maresca et al. (2009); Maresca et al. (2010). For bond-length data, see: Allen et al. (1987).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku, 2007); cell CrystalClear; data reduction: CrystalClear; 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).
Supporting information
10.1107/S1600536811006192/hg2800sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811006192/hg2800Isup2.hkl
A mixture of 9-amino-9-deoxyepiquinine QA (20 mol %) in the combination with TFA (40 mol %) exhibited high
for the Michael addition followed by of 4-hydroxycoumarin to cyclopent-2-enone-derived MBH alcohol in acetone at 60 °C for 72 h, yield 61%. Single crystals suitable for X-ray measurements were obtained by recrystallization from acetonitrile at room temperature.H atoms were positioned geometrically and refined using a riding model, with C—H = 0.95 to 1.00 Å and with Uiso(H) = 1.2 times Ueq(C).
Data collection: CrystalClear (Rigaku, 2007); cell
CrystalClear (Rigaku, 2007); data reduction: CrystalClear (Rigaku, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXL97 (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).Fig. 1. The molecular structure of (I), with atom labels and 40% probability displacement ellipsoids for non-H atoms. |
C21H16O4 | F(000) = 696 |
Mr = 332.34 | Dx = 1.399 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 4768 reflections |
a = 9.1672 (14) Å | θ = 1.0–27.5° |
b = 8.6538 (14) Å | µ = 0.10 mm−1 |
c = 19.899 (3) Å | T = 173 K |
β = 91.295 (3)° | Block, colorless |
V = 1578.2 (4) Å3 | 0.50 × 0.50 × 0.41 mm |
Z = 4 |
Rigaku Saturn724+ CCD diffractometer | 3608 independent reflections |
Radiation source: sealed tube | 3469 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.030 |
ω scans at fixed χ = 45° | θmax = 27.5°, θmin = 3.1° |
Absorption correction: numerical (CrystalClear; Rigaku, 2007) | h = −11→11 |
Tmin = 0.953, Tmax = 0.961 | k = −10→11 |
13128 measured reflections | l = −22→25 |
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)] = 0.055 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.144 | H-atom parameters constrained |
S = 1.10 | w = 1/[σ2(Fo2) + (0.0704P)2 + 0.6329P] where P = (Fo2 + 2Fc2)/3 |
3608 reflections | (Δ/σ)max < 0.001 |
226 parameters | Δρmax = 0.38 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
C21H16O4 | V = 1578.2 (4) Å3 |
Mr = 332.34 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 9.1672 (14) Å | µ = 0.10 mm−1 |
b = 8.6538 (14) Å | T = 173 K |
c = 19.899 (3) Å | 0.50 × 0.50 × 0.41 mm |
β = 91.295 (3)° |
Rigaku Saturn724+ CCD diffractometer | 3608 independent reflections |
Absorption correction: numerical (CrystalClear; Rigaku, 2007) | 3469 reflections with I > 2σ(I) |
Tmin = 0.953, Tmax = 0.961 | Rint = 0.030 |
13128 measured reflections |
R[F2 > 2σ(F2)] = 0.055 | 0 restraints |
wR(F2) = 0.144 | H-atom parameters constrained |
S = 1.10 | Δρmax = 0.38 e Å−3 |
3608 reflections | Δρmin = −0.22 e Å−3 |
226 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 | ||
O1 | 0.50827 (10) | 0.14483 (13) | 0.10143 (5) | 0.0292 (2) | |
O2 | 0.30494 (11) | 0.31578 (13) | −0.06936 (5) | 0.0342 (3) | |
O3 | 0.21059 (14) | −0.10952 (16) | 0.24113 (6) | 0.0472 (3) | |
O4 | 0.09368 (13) | 0.21341 (18) | −0.04206 (7) | 0.0509 (4) | |
C1 | 0.45295 (15) | 0.33318 (17) | −0.05937 (7) | 0.0293 (3) | |
C2 | 0.52778 (18) | 0.41320 (18) | −0.10830 (8) | 0.0344 (3) | |
H2A | 0.4773 | 0.4543 | −0.1465 | 0.041* | |
C3 | 0.67665 (18) | 0.43206 (18) | −0.10057 (8) | 0.0358 (3) | |
H3A | 0.7289 | 0.4869 | −0.1337 | 0.043* | |
C4 | 0.75115 (17) | 0.37144 (19) | −0.04468 (8) | 0.0358 (3) | |
H4A | 0.8538 | 0.3846 | −0.0400 | 0.043* | |
C5 | 0.67574 (16) | 0.29218 (18) | 0.00397 (8) | 0.0321 (3) | |
H5A | 0.7267 | 0.2512 | 0.0420 | 0.039* | |
C6 | 0.52458 (15) | 0.27221 (16) | −0.00277 (7) | 0.0268 (3) | |
C7 | 0.43568 (15) | 0.19240 (16) | 0.04545 (7) | 0.0260 (3) | |
C8 | 0.41941 (15) | 0.10574 (17) | 0.15850 (7) | 0.0275 (3) | |
H8A | 0.3765 | 0.2025 | 0.1771 | 0.033* | |
C9 | 0.29535 (15) | −0.00278 (17) | 0.13564 (7) | 0.0289 (3) | |
H9A | 0.3352 | −0.1037 | 0.1198 | 0.035* | |
C10 | 0.18782 (18) | −0.02793 (19) | 0.19294 (8) | 0.0356 (3) | |
C11 | 0.0505 (2) | 0.0604 (3) | 0.17786 (11) | 0.0564 (5) | |
H11A | 0.0224 | 0.1227 | 0.2173 | 0.068* | |
H11B | −0.0305 | −0.0110 | 0.1661 | 0.068* | |
C12 | 0.08425 (18) | 0.1647 (2) | 0.11868 (9) | 0.0412 (4) | |
H12A | 0.1231 | 0.2656 | 0.1342 | 0.049* | |
H12B | −0.0039 | 0.1824 | 0.0900 | 0.049* | |
C13 | 0.20060 (15) | 0.07317 (18) | 0.08039 (7) | 0.0308 (3) | |
H13A | 0.1506 | −0.0100 | 0.0537 | 0.037* | |
C14 | 0.29132 (15) | 0.16801 (17) | 0.03381 (7) | 0.0285 (3) | |
C15 | 0.22106 (16) | 0.22987 (19) | −0.02619 (8) | 0.0343 (3) | |
C16 | 0.51992 (15) | 0.03462 (17) | 0.21074 (7) | 0.0274 (3) | |
C17 | 0.62801 (17) | −0.06787 (19) | 0.19234 (8) | 0.0360 (3) | |
H17A | 0.6423 | −0.0896 | 0.1462 | 0.043* | |
C18 | 0.71543 (18) | −0.1389 (2) | 0.24094 (9) | 0.0440 (4) | |
H18A | 0.7886 | −0.2101 | 0.2280 | 0.053* | |
C19 | 0.69637 (19) | −0.1066 (2) | 0.30784 (9) | 0.0453 (4) | |
H19A | 0.7564 | −0.1553 | 0.3411 | 0.054* | |
C20 | 0.59009 (19) | −0.0033 (2) | 0.32673 (8) | 0.0413 (4) | |
H20A | 0.5775 | 0.0194 | 0.3729 | 0.050* | |
C21 | 0.50157 (17) | 0.06724 (18) | 0.27822 (7) | 0.0325 (3) | |
H21A | 0.4283 | 0.1380 | 0.2913 | 0.039* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0241 (5) | 0.0389 (6) | 0.0247 (5) | −0.0026 (4) | 0.0003 (4) | 0.0033 (4) |
O2 | 0.0283 (5) | 0.0438 (6) | 0.0306 (5) | 0.0048 (4) | 0.0013 (4) | 0.0074 (4) |
O3 | 0.0493 (7) | 0.0534 (8) | 0.0387 (6) | −0.0192 (6) | 0.0001 (5) | 0.0139 (5) |
O4 | 0.0280 (6) | 0.0765 (10) | 0.0478 (7) | −0.0013 (6) | −0.0061 (5) | 0.0182 (6) |
C1 | 0.0289 (7) | 0.0296 (7) | 0.0295 (7) | 0.0032 (5) | 0.0043 (5) | −0.0011 (5) |
C2 | 0.0418 (8) | 0.0309 (7) | 0.0307 (7) | 0.0054 (6) | 0.0077 (6) | 0.0029 (6) |
C3 | 0.0416 (8) | 0.0309 (7) | 0.0356 (8) | −0.0024 (6) | 0.0145 (6) | 0.0004 (6) |
C4 | 0.0303 (7) | 0.0372 (8) | 0.0402 (8) | −0.0051 (6) | 0.0093 (6) | −0.0060 (6) |
C5 | 0.0281 (7) | 0.0369 (8) | 0.0315 (7) | −0.0019 (6) | 0.0028 (5) | −0.0040 (6) |
C6 | 0.0261 (7) | 0.0279 (7) | 0.0264 (6) | 0.0002 (5) | 0.0044 (5) | −0.0029 (5) |
C7 | 0.0256 (6) | 0.0274 (7) | 0.0251 (6) | 0.0016 (5) | 0.0007 (5) | −0.0012 (5) |
C8 | 0.0263 (6) | 0.0307 (7) | 0.0256 (6) | −0.0004 (5) | 0.0042 (5) | −0.0006 (5) |
C9 | 0.0291 (7) | 0.0273 (7) | 0.0303 (7) | −0.0015 (5) | 0.0017 (5) | −0.0004 (5) |
C10 | 0.0367 (8) | 0.0374 (8) | 0.0327 (7) | −0.0132 (6) | 0.0032 (6) | 0.0016 (6) |
C11 | 0.0377 (9) | 0.0749 (14) | 0.0572 (11) | 0.0069 (9) | 0.0193 (8) | 0.0207 (10) |
C12 | 0.0290 (7) | 0.0491 (10) | 0.0460 (9) | 0.0061 (7) | 0.0093 (6) | 0.0064 (7) |
C13 | 0.0251 (7) | 0.0342 (7) | 0.0332 (7) | −0.0023 (5) | 0.0004 (5) | 0.0018 (6) |
C14 | 0.0261 (7) | 0.0326 (7) | 0.0269 (6) | 0.0019 (5) | 0.0023 (5) | 0.0009 (5) |
C15 | 0.0266 (7) | 0.0431 (9) | 0.0333 (7) | 0.0032 (6) | 0.0009 (6) | 0.0046 (6) |
C16 | 0.0270 (6) | 0.0284 (7) | 0.0267 (7) | −0.0024 (5) | 0.0001 (5) | −0.0003 (5) |
C17 | 0.0346 (8) | 0.0390 (8) | 0.0345 (8) | 0.0058 (6) | 0.0007 (6) | −0.0031 (6) |
C18 | 0.0330 (8) | 0.0438 (9) | 0.0550 (10) | 0.0062 (7) | −0.0019 (7) | 0.0089 (8) |
C19 | 0.0363 (8) | 0.0534 (10) | 0.0456 (9) | −0.0102 (7) | −0.0133 (7) | 0.0196 (8) |
C20 | 0.0456 (9) | 0.0494 (10) | 0.0288 (7) | −0.0187 (8) | −0.0053 (6) | 0.0039 (7) |
C21 | 0.0363 (8) | 0.0328 (7) | 0.0287 (7) | −0.0073 (6) | 0.0031 (6) | −0.0022 (6) |
O1—C7 | 1.3491 (17) | C9—H9A | 1.0000 |
O1—C8 | 1.4524 (16) | C10—C11 | 1.498 (3) |
O2—C1 | 1.3751 (17) | C11—C12 | 1.521 (3) |
O2—C15 | 1.3828 (18) | C11—H11A | 0.9900 |
O3—C10 | 1.205 (2) | C11—H11B | 0.9900 |
O4—C15 | 1.2112 (19) | C12—C13 | 1.543 (2) |
C1—C2 | 1.389 (2) | C12—H12A | 0.9900 |
C1—C6 | 1.394 (2) | C12—H12B | 0.9900 |
C2—C3 | 1.380 (2) | C13—C14 | 1.503 (2) |
C2—H2A | 0.9500 | C13—H13A | 1.0000 |
C3—C4 | 1.394 (2) | C14—C15 | 1.446 (2) |
C3—H3A | 0.9500 | C16—C17 | 1.385 (2) |
C4—C5 | 1.384 (2) | C16—C21 | 1.386 (2) |
C4—H4A | 0.9500 | C17—C18 | 1.386 (2) |
C5—C6 | 1.3999 (19) | C17—H17A | 0.9500 |
C5—H5A | 0.9500 | C18—C19 | 1.375 (3) |
C6—C7 | 1.4483 (19) | C18—H18A | 0.9500 |
C7—C14 | 1.3548 (19) | C19—C20 | 1.380 (3) |
C8—C16 | 1.5050 (19) | C19—H19A | 0.9500 |
C8—C9 | 1.5359 (19) | C20—C21 | 1.388 (2) |
C8—H8A | 1.0000 | C20—H20A | 0.9500 |
C9—C13 | 1.534 (2) | C21—H21A | 0.9500 |
C9—C10 | 1.540 (2) | ||
C7—O1—C8 | 116.22 (10) | C12—C11—H11A | 110.6 |
C1—O2—C15 | 121.99 (11) | C10—C11—H11B | 110.6 |
O2—C1—C2 | 117.04 (13) | C12—C11—H11B | 110.6 |
O2—C1—C6 | 121.37 (12) | H11A—C11—H11B | 108.7 |
C2—C1—C6 | 121.59 (14) | C11—C12—C13 | 103.48 (14) |
C3—C2—C1 | 118.94 (14) | C11—C12—H12A | 111.1 |
C3—C2—H2A | 120.5 | C13—C12—H12A | 111.1 |
C1—C2—H2A | 120.5 | C11—C12—H12B | 111.1 |
C2—C3—C4 | 120.66 (14) | C13—C12—H12B | 111.1 |
C2—C3—H3A | 119.7 | H12A—C12—H12B | 109.0 |
C4—C3—H3A | 119.7 | C14—C13—C9 | 111.33 (12) |
C5—C4—C3 | 120.06 (14) | C14—C13—C12 | 114.99 (13) |
C5—C4—H4A | 120.0 | C9—C13—C12 | 104.62 (12) |
C3—C4—H4A | 120.0 | C14—C13—H13A | 108.6 |
C4—C5—C6 | 120.20 (14) | C9—C13—H13A | 108.6 |
C4—C5—H5A | 119.9 | C12—C13—H13A | 108.6 |
C6—C5—H5A | 119.9 | C7—C14—C15 | 119.90 (13) |
C1—C6—C5 | 118.54 (13) | C7—C14—C13 | 122.11 (13) |
C1—C6—C7 | 116.98 (12) | C15—C14—C13 | 117.96 (13) |
C5—C6—C7 | 124.48 (13) | O4—C15—O2 | 116.59 (14) |
O1—C7—C14 | 123.74 (13) | O4—C15—C14 | 125.49 (15) |
O1—C7—C6 | 114.72 (12) | O2—C15—C14 | 117.93 (13) |
C14—C7—C6 | 121.54 (13) | C17—C16—C21 | 119.32 (14) |
O1—C8—C16 | 106.85 (11) | C17—C16—C8 | 120.64 (13) |
O1—C8—C9 | 109.60 (11) | C21—C16—C8 | 120.00 (13) |
C16—C8—C9 | 113.09 (12) | C16—C17—C18 | 120.36 (15) |
O1—C8—H8A | 109.1 | C16—C17—H17A | 119.8 |
C16—C8—H8A | 109.1 | C18—C17—H17A | 119.8 |
C9—C8—H8A | 109.1 | C19—C18—C17 | 120.06 (17) |
C13—C9—C8 | 110.72 (12) | C19—C18—H18A | 120.0 |
C13—C9—C10 | 103.28 (12) | C17—C18—H18A | 120.0 |
C8—C9—C10 | 110.45 (12) | C18—C19—C20 | 120.08 (15) |
C13—C9—H9A | 110.7 | C18—C19—H19A | 120.0 |
C8—C9—H9A | 110.7 | C20—C19—H19A | 120.0 |
C10—C9—H9A | 110.7 | C19—C20—C21 | 120.03 (15) |
O3—C10—C11 | 126.03 (15) | C19—C20—H20A | 120.0 |
O3—C10—C9 | 124.73 (16) | C21—C20—H20A | 120.0 |
C11—C10—C9 | 109.21 (13) | C16—C21—C20 | 120.14 (15) |
C10—C11—C12 | 105.83 (13) | C16—C21—H21A | 119.9 |
C10—C11—H11A | 110.6 | C20—C21—H21A | 119.9 |
C15—O2—C1—C2 | 175.79 (14) | C8—C9—C13—C14 | 36.94 (16) |
C15—O2—C1—C6 | −3.8 (2) | C10—C9—C13—C14 | 155.18 (12) |
O2—C1—C2—C3 | −179.40 (13) | C8—C9—C13—C12 | −87.86 (14) |
C6—C1—C2—C3 | 0.2 (2) | C10—C9—C13—C12 | 30.38 (15) |
C1—C2—C3—C4 | 0.2 (2) | C11—C12—C13—C14 | −159.98 (15) |
C2—C3—C4—C5 | −0.4 (2) | C11—C12—C13—C9 | −37.54 (17) |
C3—C4—C5—C6 | 0.1 (2) | O1—C7—C14—C15 | 176.95 (13) |
O2—C1—C6—C5 | 179.16 (13) | C6—C7—C14—C15 | −3.5 (2) |
C2—C1—C6—C5 | −0.4 (2) | O1—C7—C14—C13 | −5.1 (2) |
O2—C1—C6—C7 | −1.1 (2) | C6—C7—C14—C13 | 174.40 (13) |
C2—C1—C6—C7 | 179.32 (13) | C9—C13—C14—C7 | −6.2 (2) |
C4—C5—C6—C1 | 0.3 (2) | C12—C13—C14—C7 | 112.55 (16) |
C4—C5—C6—C7 | −179.48 (14) | C9—C13—C14—C15 | 171.73 (13) |
C8—O1—C7—C14 | −17.6 (2) | C12—C13—C14—C15 | −69.51 (18) |
C8—O1—C7—C6 | 162.78 (12) | C1—O2—C15—O4 | −175.20 (15) |
C1—C6—C7—O1 | −175.67 (12) | C1—O2—C15—C14 | 5.1 (2) |
C5—C6—C7—O1 | 4.1 (2) | C7—C14—C15—O4 | 178.92 (16) |
C1—C6—C7—C14 | 4.7 (2) | C13—C14—C15—O4 | 0.9 (3) |
C5—C6—C7—C14 | −175.52 (14) | C7—C14—C15—O2 | −1.4 (2) |
C7—O1—C8—C16 | 171.88 (11) | C13—C14—C15—O2 | −179.35 (13) |
C7—O1—C8—C9 | 49.00 (16) | O1—C8—C16—C17 | −40.89 (18) |
O1—C8—C9—C13 | −58.49 (15) | C9—C8—C16—C17 | 79.79 (17) |
C16—C8—C9—C13 | −177.59 (11) | O1—C8—C16—C21 | 141.38 (13) |
O1—C8—C9—C10 | −172.27 (12) | C9—C8—C16—C21 | −97.94 (15) |
C16—C8—C9—C10 | 68.63 (15) | C21—C16—C17—C18 | 1.0 (2) |
C13—C9—C10—O3 | 165.87 (15) | C8—C16—C17—C18 | −176.74 (15) |
C8—C9—C10—O3 | −75.70 (19) | C16—C17—C18—C19 | −0.8 (3) |
C13—C9—C10—C11 | −12.28 (18) | C17—C18—C19—C20 | 0.1 (3) |
C8—C9—C10—C11 | 106.14 (16) | C18—C19—C20—C21 | 0.4 (3) |
O3—C10—C11—C12 | 170.98 (17) | C17—C16—C21—C20 | −0.5 (2) |
C9—C10—C11—C12 | −10.9 (2) | C8—C16—C21—C20 | 177.23 (13) |
C10—C11—C12—C13 | 29.6 (2) | C19—C20—C21—C16 | −0.2 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
C8—H8A···O3i | 1.00 | 2.45 | 3.4042 (19) | 160 |
C17—H17A···O2ii | 0.95 | 2.54 | 3.322 (2) | 140 |
Symmetry codes: (i) −x+1/2, y+1/2, −z+1/2; (ii) −x+1, −y, −z. |
Experimental details
Crystal data | |
Chemical formula | C21H16O4 |
Mr | 332.34 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 173 |
a, b, c (Å) | 9.1672 (14), 8.6538 (14), 19.899 (3) |
β (°) | 91.295 (3) |
V (Å3) | 1578.2 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.10 |
Crystal size (mm) | 0.50 × 0.50 × 0.41 |
Data collection | |
Diffractometer | Rigaku Saturn724+ CCD diffractometer |
Absorption correction | Numerical (CrystalClear; Rigaku, 2007) |
Tmin, Tmax | 0.953, 0.961 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 13128, 3608, 3469 |
Rint | 0.030 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.055, 0.144, 1.10 |
No. of reflections | 3608 |
No. of parameters | 226 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.38, −0.22 |
Computer programs: CrystalClear (Rigaku, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C8—H8A···O3i | 1.00 | 2.45 | 3.4042 (19) | 160 |
C17—H17A···O2ii | 0.95 | 2.54 | 3.322 (2) | 140 |
Symmetry codes: (i) −x+1/2, y+1/2, −z+1/2; (ii) −x+1, −y, −z. |
References
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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.
Coumarins constitute a ubiquitous class of heterocycles found in numerous natural products, food industry, marketed drugs, and drug candidates [Vu et al., 2008; Maresca et al., 2009; Maresca et al., 2010]. Alkylations of electron-rich arenes such as 4-hydroxycoumarin are of great importance for the synthesis of many natural products and pharmaceuticals. Therefore, multiple approaches have been undertaken to develop catalytic enantioselective additions of 4-hydroxycoumarin to α,β-unsaturated carbonyl compounds. In this context the use of cyclic Morita Baylis Hillman alcohol is of particular interest since they not only exhibit regioselectivity but also can be cyclized readily followed by reaction of the resultant allylic cation with a suitable O nucleophile. In continuation of our work in this direction, we report here the crystal structure of the title compound.
In title compound, all bond lengths in the molecular are normal (Allen et al., 1987). The dihedral angle between benzene (C16—C21) and 2H-chromene (C1—C7/C14/C15/O1) rings is 59.8 (2) °. π—π interactions are indicated by the short distance (Cg1···Cg2 distance of 3.667 (2) Å, symmetry code: 1 - x,1 - y,z) between the centroids of the 2H-pyran ring (C1/C6/C7/C14/C15/O2) (Cg1) and benzene ring C1—C6 (Cg2) (Table 1). There are weaker C—H···O intermolecular interactions, which stabilized the structure (Table 1).