supplementary materials


cv5040 scheme

Acta Cryst. (2011). E67, o832    [ doi:10.1107/S1600536811008130 ]

2-Amino-5-oxo-4-phenyl-5,6,7,8-tetrahydro-4H-chromene-3-carbonitrile

X. Wang

Abstract top

In the title molecule, C16H14N2O2, the fused cyclohexene and pyran rings adopt an envelope and a flattened boat conformation, respectively. In the crystal, N-H...N and N-H...O hydrogen bonds link the molecules into corrugated sheets parallel to the bc plane.

Comment top

Much interest has recently been paid to the design of polyfunctionalized substituted pyran derivatives, owing to their wide range of biological activities (Lokaj et al., 1990; Marco et al., 1993). We obtained the title compound, (I), and report here its crystal structure.

In (I) (Fig. 1), the bond lengths and angles of the main molecule are normal and correspond to those observed in 2-amino-7,7-dimethyl- 5-oxo-4-phenyl-5,6,7,8-tetra- hydro-4H-chromene-3-carbonitrile (Tu et al., 2001). The fused cyclohexene and pyran rings adopt an envelope and a flattened bath conformations, respecteviley. The dihedral angle between the O1/C1/C2/C5/C6 and C2/C4/C5 planes is 16.67 (14) °. The O1/ C1/C2/C5/C6 plane forms an angle of 89.01 (8)° with the phenyl plane. In the crystal, the nitrile group is typical [NC = 1.146 (3) Å] and the carbonyl group also is reasonable [CO =1.228 (3) Å]. The C5/C6/C7/C8/C9/C10 plane also adopt an chair configuration in the compound, and the the dihedral angle between the C5/C6/C7/C9/C10 plane and the C7/C8/C9 plane is 46.14 (3)°.

In the crystal structure, there exist typical intermolecular N—H···O and N—H···N hydrogen bonds (Table 1). The amino N1 atom of one molecule links through H1B to the nitrile N2 atom of another molecule, creating a dimer. The amino N1 atom of one molecule also links through H1A to the keto O2 atom of another molecule to form the two-dimensional framework.

Related literature top

For the biological activities of substituted pyran derivatives, see: Lokaj et al. (1990); Marco et al. (1993). For the crystal structure of a related compound, see: Tu et al. (2001).

Experimental top

Malononitrile (10 mmol), 1,3-cyclohexanedione (10 mmol),and benzaldehyde(10 mmol)was dissolved in 20 ml e thanol ml in a round-bottom flask. The mixture was warmed, with agitation, to 353 K over a period of 3 h. The resulting solution was cooled. Crystal of (I) suitable for X-ray diffraction analysis were obtained by slow evaporation.

Refinement top

All H atoms were placed in geometrically idealized positions (N—H 0.86 and C—H 0.93–0.98 Å) and treated as riding on their parent atoms, with Uiso(H) = 1.2Ueq(C) (C,N).

Computing details top

Data collection: SMART (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. View of (I) showing the atomic numbering and 30% probability displacement ellipsoids.
2-Amino-5-oxo-4-phenyl-5,6,7,8-tetrahydro-4H-chromene-3-carbonitrile top
Crystal data top
C16H14N2O2F(000) = 1120
Mr = 266.29Dx = 1.229 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 20.210 (2) ÅCell parameters from 851 reflections
b = 8.8161 (5) Åθ = 2.5–19.1°
c = 16.3862 (13) ŵ = 0.08 mm1
β = 99.537 (1)°T = 298 K
V = 2879.2 (4) Å3Block, red
Z = 80.32 × 0.21 × 0.15 mm
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2535 independent reflections
Radiation source: fine-focus sealed tube1083 reflections with I > 2σ(I)
graphiteRint = 0.063
φ and ω scansθmax = 25.0°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2417
Tmin = 0.974, Tmax = 0.988k = 1010
7077 measured reflectionsl = 1919
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.114 w = 1/[σ2(Fo2) + (0.0454P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.81(Δ/σ)max = 0.001
2535 reflectionsΔρmax = 0.12 e Å3
182 parametersΔρmin = 0.11 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0017 (2)
Crystal data top
C16H14N2O2V = 2879.2 (4) Å3
Mr = 266.29Z = 8
Monoclinic, C2/cMo Kα radiation
a = 20.210 (2) ŵ = 0.08 mm1
b = 8.8161 (5) ÅT = 298 K
c = 16.3862 (13) Å0.32 × 0.21 × 0.15 mm
β = 99.537 (1)°
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2535 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1083 reflections with I > 2σ(I)
Tmin = 0.974, Tmax = 0.988Rint = 0.063
7077 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.114Δρmax = 0.12 e Å3
S = 0.81Δρmin = 0.11 e Å3
2535 reflectionsAbsolute structure: ?
182 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

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) top
xyzUiso*/Ueq
O10.10075 (8)0.98207 (19)1.01594 (9)0.0666 (5)
C10.07153 (12)0.8416 (3)1.00139 (16)0.0571 (7)
C50.09662 (11)1.0170 (3)0.87111 (15)0.0550 (7)
C20.05849 (11)0.7806 (3)0.92527 (13)0.0501 (6)
N10.05983 (10)0.7810 (2)1.07271 (11)0.0759 (7)
H1A0.04190.69261.07290.091*
H1B0.07030.83051.11820.091*
C40.08060 (11)0.8555 (3)0.85109 (13)0.0549 (7)
H40.04270.85280.80530.066*
O20.08103 (10)1.0779 (2)0.73126 (12)0.0897 (7)
C100.09649 (13)1.1227 (3)0.80287 (19)0.0686 (8)
C110.13891 (14)0.7707 (3)0.82384 (15)0.0569 (7)
C30.02554 (13)0.6406 (4)0.91435 (14)0.0586 (7)
C60.10774 (12)1.0700 (3)0.94811 (17)0.0604 (7)
N20.00226 (12)0.5272 (3)0.90338 (13)0.0839 (8)
C70.12867 (14)1.2263 (3)0.97399 (16)0.0790 (8)
H7A0.16221.22251.02370.095*
H7B0.09031.28250.98650.095*
C90.11266 (18)1.2848 (4)0.82299 (19)0.1061 (11)
H9A0.07121.34000.82320.127*
H9B0.13461.32790.77990.127*
C160.13116 (16)0.6985 (3)0.74839 (18)0.0867 (9)
H160.09040.70560.71270.104*
C80.15751 (17)1.3064 (3)0.9057 (2)0.1100 (12)
H8A0.16211.41390.91810.132*
H8B0.20181.26630.90290.132*
C120.19982 (16)0.7600 (3)0.87459 (18)0.0894 (10)
H120.20640.80830.92580.107*
C150.1828 (2)0.6155 (4)0.7246 (3)0.1201 (14)
H150.17660.56670.67360.144*
C140.2420 (2)0.6057 (5)0.7757 (3)0.1254 (17)
H140.27670.54920.76000.150*
C130.25165 (18)0.6783 (5)0.8505 (3)0.1215 (14)
H130.29300.67270.88500.146*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0811 (13)0.0612 (12)0.0571 (11)0.0126 (10)0.0103 (9)0.0013 (10)
C10.0571 (17)0.0574 (18)0.0580 (17)0.0072 (14)0.0135 (14)0.0012 (15)
C50.0524 (16)0.0553 (18)0.0593 (17)0.0015 (13)0.0151 (13)0.0061 (15)
C20.0532 (16)0.0537 (17)0.0443 (15)0.0037 (13)0.0104 (12)0.0004 (13)
N10.1060 (19)0.0758 (16)0.0488 (13)0.0279 (13)0.0216 (13)0.0051 (12)
C40.0530 (16)0.0653 (18)0.0462 (15)0.0032 (14)0.0073 (12)0.0070 (13)
O20.1089 (16)0.0947 (16)0.0703 (13)0.0135 (12)0.0287 (13)0.0276 (12)
C100.071 (2)0.063 (2)0.078 (2)0.0115 (15)0.0308 (18)0.0157 (18)
C110.0616 (18)0.0584 (17)0.0533 (16)0.0055 (14)0.0177 (15)0.0073 (14)
C30.0683 (18)0.066 (2)0.0439 (16)0.0033 (16)0.0159 (14)0.0034 (14)
C60.0599 (18)0.0542 (18)0.0675 (18)0.0019 (14)0.0115 (14)0.0077 (16)
N20.110 (2)0.0755 (18)0.0680 (16)0.0249 (16)0.0210 (14)0.0018 (14)
C70.084 (2)0.062 (2)0.093 (2)0.0100 (16)0.0226 (17)0.0057 (17)
C90.150 (3)0.072 (2)0.110 (3)0.007 (2)0.061 (2)0.019 (2)
C160.100 (3)0.088 (2)0.076 (2)0.0078 (18)0.0265 (18)0.0177 (18)
C80.137 (3)0.064 (2)0.141 (3)0.031 (2)0.058 (3)0.008 (2)
C120.066 (2)0.116 (3)0.088 (2)0.015 (2)0.018 (2)0.0002 (19)
C150.162 (4)0.091 (3)0.130 (4)0.003 (3)0.089 (3)0.020 (2)
C140.119 (4)0.101 (3)0.181 (5)0.021 (3)0.098 (4)0.025 (3)
C130.071 (2)0.144 (4)0.155 (4)0.023 (2)0.036 (3)0.018 (3)
Geometric parameters (Å, °) top
O1—C11.376 (3)C6—C71.482 (3)
O1—C61.381 (3)C7—C81.520 (3)
C1—N11.341 (3)C7—H7A0.9700
C1—C21.344 (3)C7—H7B0.9700
C5—C61.329 (3)C9—C81.512 (4)
C5—C101.455 (3)C9—H9A0.9700
C5—C41.484 (3)C9—H9B0.9700
C2—C31.400 (3)C16—C151.382 (4)
C2—C41.514 (3)C16—H160.9300
N1—H1A0.8600C8—H8A0.9700
N1—H1B0.8600C8—H8B0.9700
C4—C111.524 (3)C12—C131.382 (4)
C4—H40.9800C12—H120.9300
O2—C101.228 (3)C15—C141.344 (5)
C10—C91.491 (4)C15—H150.9300
C11—C121.370 (3)C14—C131.368 (5)
C11—C161.376 (3)C14—H140.9300
C3—N21.146 (3)C13—H130.9300
C1—O1—C6117.64 (19)C8—C7—H7A109.6
N1—C1—C2127.8 (2)C6—C7—H7B109.6
N1—C1—O1109.9 (2)C8—C7—H7B109.6
C2—C1—O1122.3 (2)H7A—C7—H7B108.1
C6—C5—C10118.9 (3)C10—C9—C8113.3 (3)
C6—C5—C4122.9 (2)C10—C9—H9A108.9
C10—C5—C4118.1 (2)C8—C9—H9A108.9
C1—C2—C3119.2 (2)C10—C9—H9B108.9
C1—C2—C4122.1 (2)C8—C9—H9B108.9
C3—C2—C4118.6 (2)H9A—C9—H9B107.7
C1—N1—H1A120.0C11—C16—C15121.3 (3)
C1—N1—H1B120.0C11—C16—H16119.4
H1A—N1—H1B120.0C15—C16—H16119.4
C5—C4—C2108.9 (2)C9—C8—C7110.8 (3)
C5—C4—C11112.61 (19)C9—C8—H8A109.5
C2—C4—C11111.50 (19)C7—C8—H8A109.5
C5—C4—H4107.9C9—C8—H8B109.5
C2—C4—H4107.9C7—C8—H8B109.5
C11—C4—H4107.9H8A—C8—H8B108.1
O2—C10—C5119.7 (3)C11—C12—C13120.6 (3)
O2—C10—C9122.1 (3)C11—C12—H12119.7
C5—C10—C9118.1 (3)C13—C12—H12119.7
C12—C11—C16118.1 (3)C14—C15—C16119.7 (4)
C12—C11—C4121.1 (2)C14—C15—H15120.2
C16—C11—C4120.8 (3)C16—C15—H15120.2
N2—C3—C2178.2 (3)C15—C14—C13120.4 (4)
C5—C6—O1122.9 (2)C15—C14—H14119.8
C5—C6—C7126.4 (2)C13—C14—H14119.8
O1—C6—C7110.7 (2)C14—C13—C12119.9 (4)
C6—C7—C8110.3 (2)C14—C13—H13120.0
C6—C7—H7A109.6C12—C13—H13120.0
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···N2i0.862.163.007 (3)170
N1—H1B···O2ii0.862.002.848 (2)169
Symmetry codes: (i) −x, −y+1, −z+2; (ii) x, −y+2, z+1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1A···N2i0.862.163.007 (3)170
N1—H1B···O2ii0.862.002.848 (2)169
Symmetry codes: (i) −x, −y+1, −z+2; (ii) x, −y+2, z+1/2.
Acknowledgements top

The authors acknowledge financial support from the Shenyang University of Technology.

references
References top

Bruker (2007). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Lokaj, J., Kettmann, V., Pavelčík, F., Ilavský, D. & Marchalín, Š. (1990). Acta Cryst. C46, 788–791.

Marco, J. L., Martin, G., Martin, N., Martinez-Grau, A., Seoane, C., Albert, A. & Cano, F. H. (1993). Tetrahedron, 49, 7133–7144.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Tu, S.-J., Deng, X., Fang, Y.-Y., Guo, Y.-M., Du, M. & Liu, X.-H. (2001). Acta Cryst. E57, o358–o359.