Abstract
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
C21H16O4
M r = 332.34
Monoclinic,
a = 9.1672 (14) Å
b = 8.6538 (14) Å
c = 19.899 (3) Å
β = 91.295 (3)°
V = 1578.2 (4) Å3
Z = 4
Mo Kα radiation
μ = 0.10 mm−1
T = 173 K
0.50 × 0.50 × 0.41 mm
Data collection
Rigaku Saturn724+ CCD diffractometer
Absorption correction: numerical (CrystalClear; Rigaku, 2007 ▶) T min = 0.953, T max = 0.961
13128 measured reflections
3608 independent reflections
3469 reflections with I > 2σ(I)
R int = 0.030
Refinement
R[F 2 > 2σ(F 2)] = 0.055
wR(F 2) = 0.144
S = 1.10
3608 reflections
226 parameters
H-atom parameters constrained
Δρmax = 0.38 e Å−3
Δρmin = −0.22 e Å−3
Data collection: CrystalClear (Rigaku, 2007 ▶); cell refinement: 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 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811006192/hg2800sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006192/hg2800Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| 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)
; (ii)
.
supplementary crystallographic information
Comment
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).
Experimental
A mixture of 9-amino-9-deoxyepiquinine QA (20 mol %) in the combination with TFA (40 mol %) exhibited high catalytic activity for the Michael addition followed by cycloaddition 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.
Refinement
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).
Figures
Fig. 1.
The molecular structure of (I), with atom labels and 40% probability displacement ellipsoids for non-H atoms.
Crystal data
| 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 |
Data collection
| Rigaku Saturn724+ CCD diffractometer | 3608 independent reflections |
| Radiation source: sealed tube | 3469 reflections with I > 2σ(I) |
| graphite | 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
| 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 |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| 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* |
Atomic displacement parameters (Å2)
| 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) |
Geometric parameters (Å, °)
| 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) |
Hydrogen-bond geometry (Å, °)
| 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.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG2800).
References
- Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
- Maresca, A., Temperini, C., Pochet, L., Masereel, B., Scozzafava, A. & Supuran, C. T. (2010). J. Med. Chem. 53, 335–344. [DOI] [PubMed]
- Maresca, A., Temperini, C., Vu, H., Pham, N. B., Poulsen, S. A., Scozzafava, A., Quinn, R. J. & Supuran, C. T. (2009). J. Am. Chem. Soc. 131, 3057–3062. [DOI] [PubMed]
- Rigaku (2007). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Vu, H., Pham, N. B. & Quinn, R. J. (2008). J. Biomol. Screen. 13, 265–275. [DOI] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811006192/hg2800sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006192/hg2800Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

