Abstract
In the title compound, C14H15NO3, all non-H atoms except for those of the methyl and the disordered ethyl groupare approximately co-planar, the largest deviation from the mean plane being 0.0223 (13) Å at the N atom. In the crystal, the packing of molecules through weak intermolecular C—H⋯O hydrogen-bonding interactions leads to the formation of layers parallel to bc plane. Within these layers, there exist slipped π–π stacking interactions between symmetry-related fused rings [centroid–centroid distances = 3.527 (3) and 3.554 (3), slippage = 0.988 and 1.011 Å, respectively]. One ethyl group is disordered over two sets of sites with site-occupation factors of 0.54 and 0.46.
Related literature
For background to the title compound, an organic intermediate and a fluorescent probe for cyanide and amino acids, see: Kim et al. (2010 ▶). For electronic and photonic applications of coumarins, see: Murray et al. (1982 ▶). For the synthesis, see: Wu et al. (2007 ▶).
Experimental
Crystal data
C14H15NO3
M r = 245.27
Monoclinic,
a = 25.488 (17) Å
b = 7.844 (6) Å
c = 12.599 (12) Å
β = 92.39 (3)°
V = 2517 (3) Å3
Z = 8
Mo Kα radiation
μ = 0.09 mm−1
T = 295 K
0.41 × 0.39 × 0.21 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.963, T max = 0.981
11514 measured reflections
2850 independent reflections
1724 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.048
wR(F 2) = 0.144
S = 1.06
2850 reflections
184 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.14 e Å−3
Δρmin = −0.15 e Å−3
Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEPIII (Burnett & Johnson, 1996 ▶) and ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681102294X/dn2698sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102294X/dn2698Isup2.hkl
Supplementary material file. DOI: 10.1107/S160053681102294X/dn2698Isup3.cml
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—H8⋯O3i | 0.93 | 2.58 | 3.367 (4) | 143 |
| C9—H9⋯O1ii | 0.93 | 2.55 | 3.432 (3) | 158 |
| C13—H13B⋯O2iii | 0.97 | 2.53 | 3.388 (3) | 147 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
The authors acknowledge financial support from the National Natural Science Foundation of China (grant No. 21062022) and the Open Project of the State Key Laboratory of Supramolecular Structure and Materials, Jilin University.
supplementary crystallographic information
Comment
Coumarins are an important class of naturally occurring and synthetic compounds, which have been extentively investigated for electronic and photonic applications (Murray et al., 1982). Herein, we reported the crystal structure of the title compound, an important organic intermediate and a fluorescent probe for cyanide and amino acids (Kim et al., 2010).
The molecule of title compound formed by two fused rings is mainly planar with the exception of the methyl and disordered ethyl group (Fig. 1). The weak intermolcular C—H···O hydrogen bonds (Table 1) link the molecules into layers parallel to the (100) plane. Futhermore, slipped π-π stacking occurs between symetry related fused rings within the layers (Table 2)
Experimental
The title compound was prepared according to the literature (Wu et al., 2007). Single crystals suitable for X-ray diffraction were prepared by recrystallization from mixture of dichloromethane and petroleum (60–90 °C).
Refinement
Carbon-bound H-atoms were placed in calculated positions (C—H 0.93 to 0.97 Å) and were included in the refinement in the riding model with Uiso(H) = 1.2 or 1.5 Ueq(Cmethyl).
One of the ethyl group is disordered over two positions with a site occupancy in the ratio 0.54/0.46. The refinement of the disordered moieties was carried out using the PART instruction and restraining them to have identical geometry with the SAME instruction available in SHELXL-97 (Sheldrick, 2008)
Figures
Fig. 1.
The crystal structure of the title compound, with the atom numbering scheme. Displacement ellipsoids of non-H atoms are drawn at the 30% probalility level. H atoms are shown as small spheres of arbitrary radii. Only the major component of the disordered ethyl is represented for clarity.
Crystal data
| C14H15NO3 | F(000) = 1040 |
| Mr = 245.27 | Dx = 1.295 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 6542 reflections |
| a = 25.488 (17) Å | θ = 3.2–27.5° |
| b = 7.844 (6) Å | µ = 0.09 mm−1 |
| c = 12.599 (12) Å | T = 295 K |
| β = 92.39 (3)° | Block, brown |
| V = 2517 (3) Å3 | 0.41 × 0.39 × 0.21 mm |
| Z = 8 |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 2850 independent reflections |
| Radiation source: fine-focus sealed tube | 1724 reflections with I > 2σ(I) |
| graphite | Rint = 0.033 |
| ω scans | θmax = 27.5°, θmin = 3.2° |
| Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | h = −32→32 |
| Tmin = 0.963, Tmax = 0.981 | k = −9→10 |
| 11514 measured reflections | l = −16→16 |
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)] = 0.048 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.144 | H-atom parameters constrained |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.0674P)2 + 0.3544P] where P = (Fo2 + 2Fc2)/3 |
| 2850 reflections | (Δ/σ)max < 0.001 |
| 184 parameters | Δρmax = 0.14 e Å−3 |
| 1 restraint | Δρmin = −0.15 e Å−3 |
Special details
| Experimental. (See detailed section in the paper) |
| 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. 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 | Occ. (<1) | |
| O1 | 0.24299 (4) | 0.00447 (14) | 0.88750 (8) | 0.0556 (3) | |
| O2 | 0.17217 (5) | −0.12688 (18) | 0.82505 (10) | 0.0787 (4) | |
| O3 | 0.12022 (6) | −0.24463 (18) | 1.11710 (12) | 0.0874 (5) | |
| N1 | 0.40226 (6) | 0.2780 (2) | 0.99586 (12) | 0.0747 (5) | |
| C1 | 0.19772 (6) | −0.0872 (2) | 0.90386 (13) | 0.0562 (4) | |
| C2 | 0.18575 (6) | −0.12332 (19) | 1.01323 (12) | 0.0533 (4) | |
| C3 | 0.21890 (6) | −0.0707 (2) | 1.09396 (12) | 0.0546 (4) | |
| H3 | 0.2105 | −0.0940 | 1.1636 | 0.066* | |
| C4 | 0.26540 (6) | 0.01794 (19) | 1.07523 (11) | 0.0503 (4) | |
| C5 | 0.27674 (6) | 0.05510 (19) | 0.96975 (11) | 0.0478 (4) | |
| C6 | 0.32073 (6) | 0.1413 (2) | 0.94200 (12) | 0.0533 (4) | |
| H6 | 0.3261 | 0.1652 | 0.8710 | 0.064* | |
| C7 | 0.35790 (6) | 0.1938 (2) | 1.02108 (13) | 0.0578 (4) | |
| C8 | 0.34695 (7) | 0.1572 (2) | 1.12853 (13) | 0.0636 (5) | |
| H8 | 0.3707 | 0.1906 | 1.1826 | 0.076* | |
| C9 | 0.30257 (7) | 0.0747 (2) | 1.15318 (12) | 0.0613 (4) | |
| H9 | 0.2963 | 0.0546 | 1.2243 | 0.074* | |
| C10 | 0.13764 (7) | −0.2172 (2) | 1.03121 (16) | 0.0679 (5) | |
| H10 | 0.1189 | −0.2592 | 0.9719 | 0.081* | |
| C11A | 0.4515 (3) | 0.2676 (10) | 1.0761 (7) | 0.086 (2) | 0.46 |
| H11A | 0.4478 | 0.1756 | 1.1267 | 0.103* | 0.46 |
| H11B | 0.4836 | 0.2509 | 1.0387 | 0.103* | 0.46 |
| C12A | 0.4513 (2) | 0.4378 (8) | 1.1303 (5) | 0.1030 (17) | 0.46 |
| H12A | 0.4539 | 0.5266 | 1.0784 | 0.154* | 0.46 |
| H12B | 0.4807 | 0.4448 | 1.1805 | 0.154* | 0.46 |
| H12C | 0.4193 | 0.4510 | 1.1669 | 0.154* | 0.46 |
| C11B | 0.4390 (2) | 0.3468 (8) | 1.0753 (5) | 0.0750 (15) | 0.54 |
| H11C | 0.4204 | 0.3835 | 1.1370 | 0.090* | 0.54 |
| H11D | 0.4570 | 0.4445 | 1.0469 | 0.090* | 0.54 |
| C12B | 0.4784 (2) | 0.2088 (8) | 1.1068 (5) | 0.125 (2) | 0.54 |
| H12D | 0.4602 | 0.1130 | 1.1354 | 0.188* | 0.54 |
| H12E | 0.5031 | 0.2527 | 1.1595 | 0.188* | 0.54 |
| H12F | 0.4966 | 0.1734 | 1.0455 | 0.188* | 0.54 |
| C13 | 0.41299 (8) | 0.3169 (3) | 0.88577 (15) | 0.0742 (5) | |
| H13A | 0.4374 | 0.4116 | 0.8847 | 0.089* | |
| H13B | 0.3806 | 0.3533 | 0.8495 | 0.089* | |
| C14 | 0.43552 (9) | 0.1696 (3) | 0.8251 (2) | 0.1025 (8) | |
| H14A | 0.4692 | 0.1394 | 0.8563 | 0.154* | |
| H14B | 0.4393 | 0.2024 | 0.7524 | 0.154* | |
| H14C | 0.4123 | 0.0735 | 0.8280 | 0.154* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0602 (6) | 0.0714 (7) | 0.0356 (6) | −0.0004 (6) | 0.0062 (4) | 0.0006 (5) |
| O2 | 0.0830 (8) | 0.1019 (10) | 0.0503 (7) | −0.0158 (7) | −0.0056 (6) | 0.0026 (7) |
| O3 | 0.0943 (10) | 0.0941 (10) | 0.0756 (9) | −0.0150 (8) | 0.0259 (8) | 0.0101 (7) |
| N1 | 0.0630 (8) | 0.1053 (12) | 0.0559 (9) | −0.0141 (8) | 0.0021 (7) | 0.0042 (8) |
| C1 | 0.0627 (9) | 0.0599 (10) | 0.0459 (9) | 0.0078 (8) | 0.0030 (7) | 0.0007 (7) |
| C2 | 0.0613 (9) | 0.0508 (9) | 0.0486 (9) | 0.0078 (8) | 0.0114 (7) | 0.0042 (7) |
| C3 | 0.0697 (10) | 0.0563 (9) | 0.0387 (8) | 0.0110 (8) | 0.0125 (7) | 0.0036 (7) |
| C4 | 0.0612 (9) | 0.0544 (9) | 0.0357 (8) | 0.0106 (7) | 0.0091 (6) | 0.0020 (6) |
| C5 | 0.0565 (8) | 0.0530 (9) | 0.0342 (7) | 0.0129 (7) | 0.0044 (6) | −0.0019 (6) |
| C6 | 0.0602 (9) | 0.0646 (10) | 0.0358 (8) | 0.0082 (8) | 0.0089 (6) | 0.0018 (7) |
| C7 | 0.0604 (9) | 0.0651 (10) | 0.0479 (9) | 0.0078 (8) | 0.0044 (7) | 0.0016 (7) |
| C8 | 0.0707 (11) | 0.0787 (12) | 0.0408 (9) | 0.0001 (9) | −0.0031 (7) | 0.0005 (8) |
| C9 | 0.0784 (11) | 0.0727 (11) | 0.0329 (8) | 0.0061 (9) | 0.0046 (7) | 0.0034 (7) |
| C10 | 0.0754 (11) | 0.0657 (11) | 0.0631 (12) | 0.0018 (9) | 0.0103 (9) | 0.0037 (9) |
| C11A | 0.069 (4) | 0.099 (6) | 0.091 (4) | 0.013 (4) | 0.007 (3) | 0.022 (4) |
| C12A | 0.093 (4) | 0.121 (5) | 0.094 (4) | −0.022 (3) | −0.009 (3) | −0.008 (4) |
| C11B | 0.065 (3) | 0.086 (4) | 0.073 (3) | −0.015 (3) | −0.013 (2) | 0.005 (3) |
| C12B | 0.083 (3) | 0.152 (5) | 0.137 (5) | 0.036 (3) | −0.040 (3) | 0.021 (4) |
| C13 | 0.0713 (11) | 0.0878 (13) | 0.0643 (11) | −0.0101 (10) | 0.0123 (9) | 0.0046 (10) |
| C14 | 0.0940 (15) | 0.1172 (19) | 0.0991 (18) | 0.0080 (14) | 0.0368 (13) | −0.0051 (15) |
Geometric parameters (Å, °)
| O1—C5 | 1.3774 (19) | C9—H9 | 0.9300 |
| O1—C1 | 1.382 (2) | C10—H10 | 0.9300 |
| O2—C1 | 1.205 (2) | C11A—C12A | 1.500 (8) |
| O3—C10 | 1.206 (2) | C11A—H11A | 0.9700 |
| N1—C7 | 1.358 (2) | C11A—H11B | 0.9700 |
| N1—C11B | 1.446 (6) | C12A—H12A | 0.9600 |
| N1—C13 | 1.457 (3) | C12A—H12B | 0.9600 |
| N1—C11A | 1.581 (8) | C12A—H12C | 0.9600 |
| C1—C2 | 1.452 (3) | C11B—C12B | 1.517 (7) |
| C2—C3 | 1.359 (2) | C11B—H11C | 0.9700 |
| C2—C10 | 1.456 (3) | C11B—H11D | 0.9700 |
| C3—C4 | 1.402 (2) | C12B—H12D | 0.9600 |
| C3—H3 | 0.9300 | C12B—H12E | 0.9600 |
| C4—C5 | 1.402 (2) | C12B—H12F | 0.9600 |
| C4—C9 | 1.408 (2) | C13—C14 | 1.512 (3) |
| C5—C6 | 1.367 (2) | C13—H13A | 0.9700 |
| C6—C7 | 1.408 (2) | C13—H13B | 0.9700 |
| C6—H6 | 0.9300 | C14—H14A | 0.9600 |
| C7—C8 | 1.423 (2) | C14—H14B | 0.9600 |
| C8—C9 | 1.351 (2) | C14—H14C | 0.9600 |
| C8—H8 | 0.9300 | ||
| C5—O1—C1 | 122.47 (12) | O3—C10—C2 | 125.00 (19) |
| C7—N1—C11B | 122.7 (3) | O3—C10—H10 | 117.5 |
| C7—N1—C13 | 121.03 (15) | C2—C10—H10 | 117.5 |
| C11B—N1—C13 | 116.1 (3) | C12A—C11A—N1 | 103.2 (5) |
| C7—N1—C11A | 118.2 (3) | C12A—C11A—H11A | 111.1 |
| C13—N1—C11A | 116.3 (3) | N1—C11A—H11A | 111.1 |
| O2—C1—O1 | 115.93 (15) | C12A—C11A—H11B | 111.1 |
| O2—C1—C2 | 127.14 (17) | N1—C11A—H11B | 111.1 |
| O1—C1—C2 | 116.93 (14) | H11A—C11A—H11B | 109.1 |
| C3—C2—C1 | 120.15 (16) | N1—C11B—C12B | 108.5 (5) |
| C3—C2—C10 | 122.59 (16) | N1—C11B—H11C | 110.0 |
| C1—C2—C10 | 117.26 (16) | C12B—C11B—H11C | 110.0 |
| C2—C3—C4 | 121.88 (14) | N1—C11B—H11D | 110.0 |
| C2—C3—H3 | 119.1 | C12B—C11B—H11D | 110.0 |
| C4—C3—H3 | 119.1 | H11C—C11B—H11D | 108.4 |
| C3—C4—C5 | 118.13 (14) | C11B—C12B—H12D | 109.5 |
| C3—C4—C9 | 126.03 (14) | C11B—C12B—H12E | 109.5 |
| C5—C4—C9 | 115.84 (15) | H12D—C12B—H12E | 109.5 |
| C6—C5—O1 | 116.32 (13) | C11B—C12B—H12F | 109.5 |
| C6—C5—C4 | 123.28 (14) | H12D—C12B—H12F | 109.5 |
| O1—C5—C4 | 120.40 (15) | H12E—C12B—H12F | 109.5 |
| C5—C6—C7 | 119.92 (15) | N1—C13—C14 | 114.33 (19) |
| C5—C6—H6 | 120.0 | N1—C13—H13A | 108.7 |
| C7—C6—H6 | 120.0 | C14—C13—H13A | 108.7 |
| N1—C7—C6 | 121.26 (15) | N1—C13—H13B | 108.7 |
| N1—C7—C8 | 121.26 (16) | C14—C13—H13B | 108.7 |
| C6—C7—C8 | 117.48 (16) | H13A—C13—H13B | 107.6 |
| C9—C8—C7 | 120.99 (16) | C13—C14—H14A | 109.5 |
| C9—C8—H8 | 119.5 | C13—C14—H14B | 109.5 |
| C7—C8—H8 | 119.5 | H14A—C14—H14B | 109.5 |
| C8—C9—C4 | 122.47 (15) | C13—C14—H14C | 109.5 |
| C8—C9—H9 | 118.8 | H14A—C14—H14C | 109.5 |
| C4—C9—H9 | 118.8 | H14B—C14—H14C | 109.5 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C8—H8···O3i | 0.93 | 2.58 | 3.367 (4) | 143. |
| C9—H9···O1ii | 0.93 | 2.55 | 3.432 (3) | 158. |
| C13—H13B···O2iii | 0.97 | 2.53 | 3.388 (3) | 147. |
Symmetry codes: (i) −x+1/2, y+1/2, −z+5/2; (ii) x, −y, z+1/2; (iii) −x+1/2, y+1/2, −z+3/2.
Table 2 Table 2 π-π stacking interactions (Å,°)
Cg1 is the centroid of the O1—C5 ring.Cg2 is the centroid of the C4—C9 ring
| CgI | CgJ | CgI···CgJa | CgI···P(J)b | CgJ···P(I)c | Slippage |
| Cg1 | Cg1iv | 3.527 (3) | -3.3856 (6) | -3.3856 (6) | 0.988 |
| Cg1 | Cg2iv | 3.554 (3) | 3.4110 (6) | 3.4044 (6) | 1.011 |
Symmetry codes: (iv)1/2-x,-1/2-y,2-z Notes:a : Distance between centroidsb : Perpendicular distance of CgI on ring plan Jc : Perpendicular distance of CgJ on ring plan ISlippage = vertical displacement between ring centroids.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2698).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681102294X/dn2698sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102294X/dn2698Isup2.hkl
Supplementary material file. DOI: 10.1107/S160053681102294X/dn2698Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

