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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 27;67(Pt 9):o2468. doi: 10.1107/S1600536811033873

2-Oxo-4-phenyl-1,2,5,6-tetra­hydro­benzo[h]quinoline-3-carbonitrile

Abdullah M Asiri a, Hassan M Faidallah a, Abdulrahman O Al-Youbi a, Khalid A Alamry a, Seik Weng Ng b,a,*
PMCID: PMC3200766  PMID: 22065624

Abstract

In the mol­ecule of the title compound, C20H14N2O, the tetra­hydro­benzo[h]quinoline fused-ring system is buckled owing to the ethyl­ene –CH2CH2– fragment, the benzene ring and the pyridine ring being twisted by 19.7 (1)°. The 4-substituted aromatic ring is bent away from the pyridine ring by 62.9 (1)° in order to avoid crowding the cyanide substituent. In the crystal, two mol­ecules are linked by a pair of N—H⋯O hydrogen bonds to form a centrosymmetric dimer.

Related literature

The title compound belongs to a series of cyano-pyridino­nes that have been evaluated for their anti­cancer properties, see: Rostom et al. (2011).graphic file with name e-67-o2468-scheme1.jpg

Experimental

Crystal data

  • C20H14N2O

  • M r = 298.33

  • Triclinic, Inline graphic

  • a = 7.4075 (5) Å

  • b = 9.7204 (4) Å

  • c = 10.7358 (6) Å

  • α = 77.001 (4)°

  • β = 74.348 (6)°

  • γ = 81.674 (5)°

  • V = 722.36 (7) Å3

  • Z = 2

  • Cu Kα radiation

  • μ = 0.68 mm−1

  • T = 100 K

  • 0.35 × 0.30 × 0.25 mm

Data collection

  • Agilent SuperNova Dual diffractometer with Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) T min = 0.797, T max = 0.848

  • 4086 measured reflections

  • 2785 independent reflections

  • 2576 reflections with I > 2σ(I)

  • R int = 0.015

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.106

  • S = 1.03

  • 2785 reflections

  • 212 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.24 e Å−3

  • Δρmin = −0.27 e Å−3

Data collection: CrysAlis PRO (Agilent, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811033873/xu5290sup1.cif

e-67-o2468-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033873/xu5290Isup2.hkl

e-67-o2468-Isup2.hkl (136.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811033873/xu5290Isup3.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
N1—H1⋯O1i 0.97 (2) 1.89 (2) 2.848 (1) 168 (1)

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank King Abdulaziz University and the University of Malaya for supporting this study.

supplementary crystallographic information

Comment

The compound (Scheme I) belongs to a series of cyano-pyridinones that have been evaluated for their anticancer properties (Rostom et al., 2011). The tetrahydrobenzo[h]quinoline fused-ring system is buckled owing to the ethylene –CH2CH2– fragment, the benzene ring and the pyridine ring being twisted by 19.7 (1)°. The 4-subsituted aromatic ring is bent away from the pyridine ring by 62.9 (1) ° in order to avoid crowding the cyanide substituent (Fig. 1). Two molecules are linked by an N—H···O hydrogen bonds to form a centrosymmetric dimer (Table 1).

Experimental

A mixture of benzaldehyde (1.06 g, 10 mmol), 1-tetralone (1.46 g, 10 mmol), ethyl cyanoacetate (1.1 g, 10 mmol) and ammonium acetate (6.2 g, 80 mmol) in absolute ethanol (50 ml) was refluxed for 6 h. The reaction mixture was allowed to cool, and the orange precipitate that formed was filtered, washed with water, dried and recrystallized from ethanol; m.p. 585–597 K.

Refinement

Carbon- and nitrogen-bound H atoms were placed in calculated positions [C—H 0.95 to 0.99 Å, Uiso(H) = 1.2Ueq(C)] and were included in the refinement in the riding model approximation.

The amino H atom was located in a difference Fourier map and was freely refined.

The diffraction data are 94% complete at a 2θ limit of 150° but are 99% complete at 135°.

Figures

Fig. 1.

Fig. 1.

Thermal ellipsoid plot (Barbour, 2001) of C20H14N2O at the 70% probability level; hydrogen atoms are drawn as spheres of arbitrary radius.

Crystal data

C20H14N2O Z = 2
Mr = 298.33 F(000) = 312
Triclinic, P1 Dx = 1.372 Mg m3
Hall symbol: -P 1 Cu Kα radiation, λ = 1.54184 Å
a = 7.4075 (5) Å Cell parameters from 2774 reflections
b = 9.7204 (4) Å θ = 4.4–74.3°
c = 10.7358 (6) Å µ = 0.68 mm1
α = 77.001 (4)° T = 100 K
β = 74.348 (6)° Block, yellow
γ = 81.674 (5)° 0.35 × 0.30 × 0.25 mm
V = 722.36 (7) Å3

Data collection

Agilent SuperNova Dual diffractometer with Atlas detector 2785 independent reflections
Radiation source: SuperNova (Cu) X-ray Source 2576 reflections with I > 2σ(I)
mirror Rint = 0.015
Detector resolution: 10.4041 pixels mm-1 θmax = 74.5°, θmin = 4.4°
ω scans h = −9→8
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) k = −12→9
Tmin = 0.797, Tmax = 0.848 l = −12→13
4086 measured reflections

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)] = 0.037 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.106 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0667P)2 + 0.1847P] where P = (Fo2 + 2Fc2)/3
2785 reflections (Δ/σ)max = 0.001
212 parameters Δρmax = 0.24 e Å3
0 restraints Δρmin = −0.27 e Å3

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
O1 0.36679 (10) 0.61389 (8) 0.41605 (8) 0.0164 (2)
N1 0.24537 (13) 0.48620 (10) 0.62038 (9) 0.0133 (2)
N2 0.01407 (14) 0.86078 (10) 0.31963 (10) 0.0196 (2)
C1 0.10482 (15) 0.45737 (11) 0.73289 (11) 0.0134 (2)
C2 0.14223 (15) 0.34124 (11) 0.83986 (11) 0.0144 (2)
C3 0.32488 (15) 0.28586 (12) 0.84832 (11) 0.0163 (2)
H3 0.4303 0.3258 0.7854 0.020*
C4 0.35215 (16) 0.17277 (12) 0.94846 (12) 0.0188 (3)
H4 0.4762 0.1361 0.9545 0.023*
C5 0.19842 (17) 0.11307 (12) 1.03992 (12) 0.0197 (3)
H5 0.2173 0.0342 1.1071 0.024*
C6 0.01712 (16) 0.16880 (12) 1.03297 (11) 0.0186 (3)
H6 −0.0874 0.1280 1.0963 0.022*
C7 −0.01372 (15) 0.28330 (12) 0.93487 (11) 0.0157 (2)
C8 −0.20935 (15) 0.34442 (12) 0.92477 (11) 0.0185 (3)
H8A −0.2982 0.3238 1.0126 0.022*
H8B −0.2498 0.2995 0.8639 0.022*
C9 −0.21419 (16) 0.50443 (12) 0.87427 (11) 0.0178 (3)
H9A −0.3407 0.5420 0.8612 0.021*
H9B −0.1885 0.5508 0.9401 0.021*
C10 −0.06775 (15) 0.53738 (12) 0.74493 (11) 0.0142 (2)
C11 −0.09384 (15) 0.64960 (11) 0.64016 (11) 0.0140 (2)
C12 0.05055 (15) 0.67305 (11) 0.52614 (11) 0.0138 (2)
C13 0.23126 (15) 0.59235 (11) 0.51369 (11) 0.0132 (2)
C14 0.02822 (14) 0.77868 (11) 0.41323 (11) 0.0148 (2)
C15 −0.26822 (15) 0.74948 (12) 0.65116 (11) 0.0146 (2)
C16 −0.44492 (16) 0.70524 (12) 0.66625 (11) 0.0186 (3)
H16 −0.4573 0.6088 0.6681 0.022*
C17 −0.60284 (16) 0.80230 (14) 0.67855 (12) 0.0217 (3)
H17 −0.7230 0.7722 0.6877 0.026*
C18 −0.58610 (17) 0.94329 (13) 0.67750 (12) 0.0218 (3)
H18 −0.6949 1.0088 0.6878 0.026*
C19 −0.41072 (17) 0.98783 (12) 0.66149 (12) 0.0210 (3)
H19 −0.3989 1.0843 0.6600 0.025*
C20 −0.25188 (16) 0.89167 (12) 0.64761 (11) 0.0176 (2)
H20 −0.1315 0.9228 0.6356 0.021*
H1 0.372 (2) 0.4387 (17) 0.6103 (16) 0.029 (4)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0117 (4) 0.0184 (4) 0.0152 (4) 0.0000 (3) 0.0004 (3) −0.0005 (3)
N1 0.0103 (4) 0.0144 (4) 0.0135 (5) −0.0003 (3) −0.0016 (3) −0.0017 (4)
N2 0.0182 (5) 0.0197 (5) 0.0192 (5) 0.0001 (4) −0.0040 (4) −0.0019 (4)
C1 0.0123 (5) 0.0149 (5) 0.0134 (5) −0.0031 (4) −0.0017 (4) −0.0042 (4)
C2 0.0154 (5) 0.0148 (5) 0.0131 (5) −0.0013 (4) −0.0024 (4) −0.0046 (4)
C3 0.0142 (5) 0.0179 (5) 0.0147 (5) −0.0018 (4) −0.0004 (4) −0.0026 (4)
C4 0.0175 (5) 0.0194 (6) 0.0182 (6) 0.0011 (4) −0.0048 (4) −0.0019 (4)
C5 0.0244 (6) 0.0170 (5) 0.0154 (6) −0.0011 (4) −0.0037 (5) −0.0005 (4)
C6 0.0186 (6) 0.0193 (6) 0.0150 (6) −0.0047 (4) 0.0012 (4) −0.0020 (4)
C7 0.0151 (5) 0.0174 (5) 0.0146 (5) −0.0025 (4) −0.0017 (4) −0.0050 (4)
C8 0.0133 (5) 0.0231 (6) 0.0162 (6) −0.0042 (4) 0.0005 (4) −0.0009 (4)
C9 0.0143 (5) 0.0217 (6) 0.0143 (6) 0.0008 (4) 0.0002 (4) −0.0031 (4)
C10 0.0122 (5) 0.0161 (5) 0.0145 (5) −0.0018 (4) −0.0016 (4) −0.0049 (4)
C11 0.0122 (5) 0.0153 (5) 0.0162 (5) −0.0019 (4) −0.0034 (4) −0.0061 (4)
C12 0.0120 (5) 0.0145 (5) 0.0152 (5) −0.0009 (4) −0.0033 (4) −0.0037 (4)
C13 0.0127 (5) 0.0136 (5) 0.0132 (5) −0.0026 (4) −0.0020 (4) −0.0031 (4)
C14 0.0103 (5) 0.0154 (5) 0.0186 (6) −0.0013 (4) −0.0013 (4) −0.0056 (5)
C15 0.0133 (5) 0.0178 (5) 0.0117 (5) 0.0013 (4) −0.0022 (4) −0.0038 (4)
C16 0.0168 (6) 0.0204 (6) 0.0197 (6) −0.0006 (4) −0.0038 (4) −0.0074 (5)
C17 0.0126 (5) 0.0319 (7) 0.0219 (6) 0.0008 (5) −0.0046 (4) −0.0091 (5)
C18 0.0176 (6) 0.0258 (6) 0.0192 (6) 0.0084 (5) −0.0040 (4) −0.0060 (5)
C19 0.0235 (6) 0.0176 (6) 0.0195 (6) 0.0032 (5) −0.0033 (5) −0.0044 (4)
C20 0.0156 (5) 0.0190 (6) 0.0171 (6) −0.0009 (4) −0.0024 (4) −0.0039 (4)

Geometric parameters (Å, °)

O1—C13 1.2429 (13) C8—H8B 0.9900
N1—C1 1.3694 (14) C9—C10 1.5150 (15)
N1—C13 1.3745 (14) C9—H9A 0.9900
N1—H1 0.970 (17) C9—H9B 0.9900
N2—C14 1.1530 (15) C10—C11 1.4130 (16)
C1—C10 1.3870 (15) C11—C12 1.3904 (15)
C1—C2 1.4723 (15) C11—C15 1.4938 (15)
C2—C3 1.4007 (16) C12—C14 1.4318 (15)
C2—C7 1.4094 (15) C12—C13 1.4393 (15)
C3—C4 1.3879 (16) C15—C16 1.3934 (16)
C3—H3 0.9500 C15—C20 1.3959 (16)
C4—C5 1.3890 (16) C16—C17 1.3889 (16)
C4—H4 0.9500 C16—H16 0.9500
C5—C6 1.3884 (17) C17—C18 1.3911 (18)
C5—H5 0.9500 C17—H17 0.9500
C6—C7 1.3888 (16) C18—C19 1.3834 (18)
C6—H6 0.9500 C18—H18 0.9500
C7—C8 1.5071 (16) C19—C20 1.3892 (16)
C8—C9 1.5262 (16) C19—H19 0.9500
C8—H8A 0.9900 C20—H20 0.9500
C1—N1—C13 124.83 (9) C8—C9—H9B 109.7
C1—N1—H1 123.1 (9) H9A—C9—H9B 108.2
C13—N1—H1 111.8 (9) C1—C10—C11 118.74 (10)
N1—C1—C10 120.15 (10) C1—C10—C9 117.52 (10)
N1—C1—C2 118.52 (9) C11—C10—C9 123.63 (10)
C10—C1—C2 121.33 (10) C12—C11—C10 119.34 (10)
C3—C2—C7 119.71 (10) C12—C11—C15 118.71 (10)
C3—C2—C1 122.50 (10) C10—C11—C15 121.85 (10)
C7—C2—C1 117.78 (10) C11—C12—C14 121.99 (10)
C4—C3—C2 120.15 (10) C11—C12—C13 122.24 (10)
C4—C3—H3 119.9 C14—C12—C13 115.77 (9)
C2—C3—H3 119.9 O1—C13—N1 121.03 (9)
C3—C4—C5 120.14 (11) O1—C13—C12 124.38 (10)
C3—C4—H4 119.9 N1—C13—C12 114.59 (9)
C5—C4—H4 119.9 N2—C14—C12 177.69 (12)
C6—C5—C4 119.91 (11) C16—C15—C20 119.43 (10)
C6—C5—H5 120.0 C16—C15—C11 122.37 (10)
C4—C5—H5 120.0 C20—C15—C11 118.19 (10)
C5—C6—C7 121.00 (11) C17—C16—C15 119.90 (11)
C5—C6—H6 119.5 C17—C16—H16 120.1
C7—C6—H6 119.5 C15—C16—H16 120.1
C6—C7—C2 119.05 (10) C16—C17—C18 120.39 (11)
C6—C7—C8 121.83 (10) C16—C17—H17 119.8
C2—C7—C8 119.09 (10) C18—C17—H17 119.8
C7—C8—C9 110.56 (9) C19—C18—C17 119.86 (10)
C7—C8—H8A 109.5 C19—C18—H18 120.1
C9—C8—H8A 109.5 C17—C18—H18 120.1
C7—C8—H8B 109.5 C18—C19—C20 120.05 (11)
C9—C8—H8B 109.5 C18—C19—H19 120.0
H8A—C8—H8B 108.1 C20—C19—H19 120.0
C10—C9—C8 109.84 (9) C19—C20—C15 120.35 (11)
C10—C9—H9A 109.7 C19—C20—H20 119.8
C8—C9—H9A 109.7 C15—C20—H20 119.8
C10—C9—H9B 109.7
C13—N1—C1—C10 0.43 (17) C1—C10—C11—C12 2.66 (16)
C13—N1—C1—C2 −179.06 (9) C9—C10—C11—C12 178.76 (10)
N1—C1—C2—C3 18.21 (16) C1—C10—C11—C15 −173.72 (10)
C10—C1—C2—C3 −161.28 (11) C9—C10—C11—C15 2.38 (17)
N1—C1—C2—C7 −160.55 (10) C10—C11—C12—C14 175.67 (10)
C10—C1—C2—C7 19.96 (15) C15—C11—C12—C14 −7.84 (16)
C7—C2—C3—C4 1.16 (17) C10—C11—C12—C13 −3.94 (17)
C1—C2—C3—C4 −177.57 (10) C15—C11—C12—C13 172.55 (9)
C2—C3—C4—C5 0.66 (17) C1—N1—C13—O1 178.43 (10)
C3—C4—C5—C6 −1.51 (18) C1—N1—C13—C12 −1.51 (15)
C4—C5—C6—C7 0.53 (18) C11—C12—C13—O1 −176.65 (10)
C5—C6—C7—C2 1.27 (17) C14—C12—C13—O1 3.71 (16)
C5—C6—C7—C8 179.37 (11) C11—C12—C13—N1 3.27 (16)
C3—C2—C7—C6 −2.10 (16) C14—C12—C13—N1 −176.36 (9)
C1—C2—C7—C6 176.69 (10) C12—C11—C15—C16 119.29 (12)
C3—C2—C7—C8 179.74 (10) C10—C11—C15—C16 −64.31 (15)
C1—C2—C7—C8 −1.47 (15) C12—C11—C15—C20 −61.49 (14)
C6—C7—C8—C9 146.11 (11) C10—C11—C15—C20 114.91 (12)
C2—C7—C8—C9 −35.79 (14) C20—C15—C16—C17 −0.47 (17)
C7—C8—C9—C10 54.80 (13) C11—C15—C16—C17 178.75 (10)
N1—C1—C10—C11 −0.94 (16) C15—C16—C17—C18 −0.78 (18)
C2—C1—C10—C11 178.54 (9) C16—C17—C18—C19 1.29 (18)
N1—C1—C10—C9 −177.28 (10) C17—C18—C19—C20 −0.54 (18)
C2—C1—C10—C9 2.20 (16) C18—C19—C20—C15 −0.70 (18)
C8—C9—C10—C1 −39.57 (14) C16—C15—C20—C19 1.21 (17)
C8—C9—C10—C11 144.29 (11) C11—C15—C20—C19 −178.04 (10)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···O1i 0.97 (2) 1.89 (2) 2.848 (1) 168 (1)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5290).

References

  1. Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
  2. Barbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.
  3. Rostom, S. A. F., Faidallah, H. M. & Al-Saadi, M. S. (2011). Med. Chem. Res. 20 (DOI: 10.1007/s00044-010-9469-0).
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

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/S1600536811033873/xu5290sup1.cif

e-67-o2468-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033873/xu5290Isup2.hkl

e-67-o2468-Isup2.hkl (136.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811033873/xu5290Isup3.cml

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


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