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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 18;67(Pt 7):o1713. doi: 10.1107/S160053681102294X

7-Diethyl­amino-2-oxo-2H-chromene-3-carbaldehyde

Hong-Da Li a, Bing-Zhu Yin a,*
PMCID: PMC3151821  PMID: 21837106

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).graphic file with name e-67-o1713-scheme1.jpg

Experimental

Crystal data

  • C14H15NO3

  • M r = 245.27

  • Monoclinic, Inline graphic

  • 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

e-67-o1713-sup1.cif (22.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102294X/dn2698Isup2.hkl

e-67-o1713-Isup2.hkl (140KB, 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 DA 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) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

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.

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 m3
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 mm1
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 Å3
1 restraint Δρmin = −0.15 e Å3

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

  1. Burnett, M. N. & Johnson, C. K. (1996). ORTEPIII Report ORNL-6895. Oak Ridge National Laboratory, Tennessee, USA.
  2. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  3. Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
  4. Kim, G. J. & Kim, H. J. (2010). Tetrahedron Lett. 51, 2914–2916.
  5. Murray, R. D., Mendez, J. & Brown, S. A. (1982). The Natural Coumarins: Occurrence, Chemistry and Biochemistry, p. 227. New York: John Wiley and Sons.
  6. Rigaku (1998). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
  7. Rigaku (2002). CrystalStructure Rigaku/MSC Inc., The Woodlands, Texas, USA.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Wu, J. S., Liu, W. M., Zhuang, X. Q., Wang, F., Wang, P. F., Tao, S. L., Zhang, X. H., Wu, S. K. & Lee, S. T. (2007). Org. Lett. 9, 33–36. [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 datablock(s) global, I. DOI: 10.1107/S160053681102294X/dn2698sup1.cif

e-67-o1713-sup1.cif (22.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102294X/dn2698Isup2.hkl

e-67-o1713-Isup2.hkl (140KB, hkl)

Supplementary material file. DOI: 10.1107/S160053681102294X/dn2698Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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