supplementary materials


hk2449 scheme

Acta Cryst. (2008). E64, o831    [ doi:10.1107/S1600536808009239 ]

2-Chloro-12-phenyl-6,7,8,9,10,11-hexahydrocycloocta[b]quinoline

A. Bazgir and A. M. Astaraki

Abstract top

In the molecule of the title compound, C21H20ClN, the quinoline group is nearly planar and is oriented at a dihedral angle of 77.21 (3)° with respect to the phenyl ring. The conformation of the cyclooctane ring is twist-boat. In the crystal structure, there are some weak [pi]-[pi] interactions [centroid-to-centroid distances of 3.7414 (11) and 3.8633 (12) Å] between the rings of the quinoline groups.

Comment top

Quinoline nucleus is a backbone of many natural products and pharmacologicallly significant compounds displaying a broad range of biological activities and many functionalized quinolines are widely used as antimalarial, antiasthmatic, antiinflamatory, antibacterial, antihypertensive and tyrosine kinase PDGF-RTK inhibiting agents (Kalluraya & Sreenivasa, 1998; Doube et al., 1998; Maguire et al., 1994). We report herein the synthesis and crystal structure of the title compound, (I).

In the molecule of the title compound, (I), (Fig. 1) the bond lengths (Allen et al., 1987) and angles are within normal ranges. Rings A (C1-C6), B (N1/C1/C6-C8/C15) and C (C16-C21) are, of course, planar, and they are oriented at dihedral angles of A/B = 0.88 (3)°, A/C = 76.76 (4)° and B/C = 77.64 (3)°. So, rings A and B are also nearly coplanar. The dihedral angle between the coplanar ring system and ring C is 77.21 (3)°.

In the crystal structure, the weak ππ interactions between the two adjacent A rings and A and B rings, with centroid-centroid distances of 3.7414 (11) Å and 3.8633 (12) Å, may be effective in the stabilization of the structure (Fig. 2).

Related literature top

For general background, see: Kalluraya & Sreenivasa (1998); Doube et al. (1998); Maguire et al. (1994). For bond-length data, see: Allen et al. (1987).

Experimental top

A mixture of 2-amino-5-chlorophenyl(phenyl)methanone (0.23 g, 1 mmol), cyclooctanone (1.26 g, 1 mmol) and Dewax-50 W ion exchange resin (0.3 g) was heated at 353 K. After 2 h the reaction mixture was washed with ethyl acetate (10 ml). Evaporation of the solvent followed by recrystallization from ethanol to afford the pure product (yield; 0.278 g, 75%).

Refinement top

H atoms were positioned geometrically with C-H = 0.93 and 0.97 Å for aromatic and methylene H atoms, respectively, and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA (Stoe & Cie, 2002); data reduction: X-RED (Stoe & Cie, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. A packing diagram of (I).
2-Chloro-12-phenyl-6,7,8,9,10,11-hexahydrocycloocta[b]quinoline top
Crystal data top
C21H20Cl1N1Z = 2
Mr = 321.83F000 = 340
Triclinic, P1Dx = 1.298 Mg m3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 9.837 (2) ÅCell parameters from 2086 reflections
b = 9.980 (2) Åθ = 2.4–28.0º
c = 10.175 (2) ŵ = 0.23 mm1
α = 74.600 (17)ºT = 298 (2) K
β = 70.575 (16)ºBlock, colorless
γ = 61.829 (15)º0.5 × 0.5 × 0.25 mm
V = 823.4 (3) Å3
Data collection top
Stoe IPDSII
diffractometer
Rint = 0.045
rotation method scansθmax = 28.0º
Absorption correction: numerical
shape of crystal determined optically [PROGRAM NAME? reference?
θmin = 2.4º
Tmin = 0.889, Tmax = 0.949h = 12→11
8123 measured reflectionsk = 13→10
3801 independent reflectionsl = 13→13
3493 reflections with I > 2σ(I)
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full  w = 1/[σ2(Fo2) + (0.0607P)2 + 0.1883P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.046(Δ/σ)max = 0.006
wR(F2) = 0.126Δρmax = 0.25 e Å3
S = 1.04Δρmin = 0.19 e Å3
3801 reflectionsExtinction correction: none
208 parameters
Crystal data top
C21H20Cl1N1γ = 61.829 (15)º
Mr = 321.83V = 823.4 (3) Å3
Triclinic, P1Z = 2
a = 9.837 (2) ÅMo Kα
b = 9.980 (2) ŵ = 0.23 mm1
c = 10.175 (2) ÅT = 298 (2) K
α = 74.600 (17)º0.5 × 0.5 × 0.25 mm
β = 70.575 (16)º
Data collection top
Stoe IPDSII
diffractometer
3801 independent reflections
Absorption correction: numerical
shape of crystal determined optically [PROGRAM NAME? reference?
3493 reflections with I > 2σ(I)
Tmin = 0.889, Tmax = 0.949Rint = 0.045
8123 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.046208 parameters
wR(F2) = 0.126H-atom parameters constrained
S = 1.04Δρmax = 0.25 e Å3
3801 reflectionsΔρmin = 0.19 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.59962 (5)0.96565 (4)0.17975 (4)0.06276 (16)
N10.51106 (12)0.54812 (13)0.69575 (11)0.0391 (2)
C10.53821 (13)0.64045 (14)0.57445 (12)0.0354 (2)
C20.42557 (15)0.79582 (15)0.56208 (15)0.0440 (3)
H20.33770.83130.63660.053*
C30.44417 (16)0.89348 (15)0.44312 (16)0.0462 (3)
H30.36930.99490.43540.055*
C40.57823 (15)0.83909 (14)0.33177 (14)0.0418 (3)
C50.69071 (14)0.69125 (14)0.33901 (13)0.0392 (3)
H50.77870.6590.26390.047*
C60.67271 (13)0.58733 (13)0.46148 (12)0.0333 (2)
C70.78256 (13)0.43037 (13)0.47776 (12)0.0339 (2)
C80.75403 (14)0.33702 (14)0.60027 (12)0.0357 (2)
C90.86347 (17)0.16885 (15)0.62161 (14)0.0456 (3)
H9A0.91110.13130.5310.055*
H9B0.80030.11390.67960.055*
C100.99695 (16)0.13077 (18)0.69016 (16)0.0542 (4)
H10A1.04550.02070.71670.065*
H10B1.07770.15840.620.065*
C110.94953 (18)0.2078 (2)0.81886 (16)0.0549 (4)
H11A0.90850.31780.79090.066*
H11B1.04450.17650.85010.066*
C120.82614 (19)0.17430 (19)0.94328 (16)0.0553 (4)
H12A0.85680.16061.02890.066*
H12B0.82890.0780.9360.066*
C130.65535 (18)0.29655 (18)0.95684 (14)0.0510 (3)
H13A0.65510.39480.95290.061*
H13B0.59270.27481.04910.061*
C140.57222 (16)0.31198 (17)0.84728 (14)0.0470 (3)
H14A0.59880.21010.83070.056*
H14B0.45820.36050.88550.056*
C150.61401 (13)0.40276 (14)0.70838 (12)0.0370 (3)
C160.92569 (13)0.37293 (13)0.35925 (12)0.0359 (2)
C170.91195 (17)0.34403 (19)0.23968 (14)0.0498 (3)
H170.81390.35750.23350.06*
C181.0449 (2)0.2949 (2)0.12879 (17)0.0655 (5)
H181.03550.27460.04890.079*
C191.1906 (2)0.2758 (2)0.13600 (18)0.0631 (4)
H191.27920.24210.06170.076*
C201.20421 (17)0.30678 (19)0.25315 (18)0.0564 (4)
H201.3020.29550.25780.068*
C211.07270 (15)0.35483 (16)0.36480 (15)0.0453 (3)
H211.0830.37520.44420.054*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0600 (3)0.0434 (2)0.0641 (3)0.01716 (17)0.01096 (18)0.01044 (16)
N10.0288 (5)0.0426 (5)0.0396 (5)0.0107 (4)0.0059 (4)0.0076 (4)
C10.0271 (5)0.0369 (6)0.0400 (6)0.0093 (4)0.0084 (4)0.0094 (4)
C20.0304 (6)0.0392 (6)0.0524 (7)0.0063 (5)0.0053 (5)0.0130 (5)
C30.0367 (6)0.0334 (6)0.0607 (8)0.0071 (5)0.0131 (6)0.0078 (5)
C40.0396 (6)0.0357 (6)0.0486 (7)0.0157 (5)0.0132 (5)0.0006 (5)
C50.0327 (6)0.0376 (6)0.0426 (6)0.0123 (5)0.0068 (5)0.0059 (5)
C60.0268 (5)0.0346 (5)0.0377 (5)0.0102 (4)0.0084 (4)0.0083 (4)
C70.0277 (5)0.0358 (6)0.0366 (5)0.0095 (4)0.0080 (4)0.0096 (4)
C80.0318 (5)0.0346 (6)0.0391 (6)0.0103 (4)0.0104 (4)0.0074 (4)
C90.0475 (7)0.0333 (6)0.0455 (7)0.0086 (5)0.0103 (5)0.0065 (5)
C100.0372 (7)0.0478 (7)0.0542 (8)0.0030 (6)0.0116 (6)0.0008 (6)
C110.0457 (7)0.0622 (9)0.0552 (8)0.0218 (7)0.0207 (6)0.0034 (7)
C120.0548 (8)0.0573 (9)0.0470 (7)0.0206 (7)0.0186 (6)0.0057 (6)
C130.0531 (8)0.0526 (8)0.0366 (6)0.0188 (6)0.0069 (5)0.0013 (5)
C140.0372 (6)0.0509 (7)0.0463 (7)0.0197 (6)0.0053 (5)0.0001 (6)
C150.0301 (5)0.0413 (6)0.0387 (6)0.0142 (5)0.0091 (4)0.0050 (5)
C160.0308 (5)0.0325 (5)0.0378 (6)0.0083 (4)0.0052 (4)0.0085 (4)
C170.0420 (7)0.0655 (9)0.0450 (7)0.0231 (6)0.0054 (5)0.0178 (6)
C180.0635 (10)0.0914 (13)0.0468 (8)0.0362 (9)0.0029 (7)0.0309 (8)
C190.0472 (8)0.0739 (11)0.0574 (9)0.0243 (8)0.0123 (7)0.0265 (8)
C200.0323 (6)0.0617 (9)0.0695 (9)0.0167 (6)0.0022 (6)0.0190 (7)
C210.0348 (6)0.0471 (7)0.0513 (7)0.0118 (5)0.0087 (5)0.0152 (6)
Geometric parameters (Å, °) top
C1—N11.3612 (16)C11—H11A0.97
C1—C61.4153 (16)C11—H11B0.97
C1—C21.4194 (17)C12—C131.526 (2)
C2—C31.358 (2)C12—H12A0.97
C2—H20.93C12—H12B0.97
C3—C41.4051 (19)C13—C141.527 (2)
C3—H30.93C13—H13A0.97
C4—C51.3644 (18)C13—H13B0.97
C4—Cl11.7405 (14)C14—C151.5075 (18)
C5—C61.4143 (17)C14—H14A0.97
C5—H50.93C14—H14B0.97
C6—C71.4255 (16)C15—N11.3217 (17)
C7—C81.3777 (17)C16—C171.3836 (18)
C7—C161.4969 (16)C16—C211.3890 (18)
C8—C151.4353 (17)C17—C181.390 (2)
C8—C91.5096 (17)C17—H170.93
C9—C101.534 (2)C18—C191.378 (3)
C9—H9A0.97C18—H180.93
C9—H9B0.97C19—C201.370 (2)
C10—C111.521 (2)C19—H190.93
C10—H10A0.97C20—C211.3857 (19)
C10—H10B0.97C20—H200.93
C11—C121.524 (2)C21—H210.93
N1—C1—C6122.66 (11)H11A—C11—H11B107.4
N1—C1—C2117.98 (11)C11—C12—C13115.65 (13)
C6—C1—C2119.36 (11)C11—C12—H12A108.4
C3—C2—C1121.00 (12)C13—C12—H12A108.4
C3—C2—H2119.5C11—C12—H12B108.4
C1—C2—H2119.5C13—C12—H12B108.4
C2—C3—C4119.00 (12)H12A—C12—H12B107.4
C2—C3—H3120.5C12—C13—C14116.62 (13)
C4—C3—H3120.5C12—C13—H13A108.1
C5—C4—C3122.25 (12)C14—C13—H13A108.1
C5—C4—Cl1119.37 (10)C12—C13—H13B108.1
C3—C4—Cl1118.37 (10)C14—C13—H13B108.1
C4—C5—C6119.61 (11)H13A—C13—H13B107.3
C4—C5—H5120.2C15—C14—C13114.79 (11)
C6—C5—H5120.2C15—C14—H14A108.6
C5—C6—C1118.77 (11)C13—C14—H14A108.6
C5—C6—C7123.61 (10)C15—C14—H14B108.6
C1—C6—C7117.63 (11)C13—C14—H14B108.6
C8—C7—C6119.53 (10)H14A—C14—H14B107.5
C8—C7—C16122.32 (10)N1—C15—C8123.17 (11)
C6—C7—C16118.15 (10)N1—C15—C14114.02 (11)
C7—C8—C15118.28 (11)C8—C15—C14122.80 (11)
C7—C8—C9121.86 (11)C17—C16—C21118.98 (11)
C15—C8—C9119.85 (11)C17—C16—C7120.43 (11)
C8—C9—C10115.07 (12)C21—C16—C7120.52 (11)
C8—C9—H9A108.5C16—C17—C18119.87 (13)
C10—C9—H9A108.5C16—C17—H17120.1
C8—C9—H9B108.5C18—C17—H17120.1
C10—C9—H9B108.5C19—C18—C17120.65 (15)
H9A—C9—H9B107.5C19—C18—H18119.7
C11—C10—C9116.56 (12)C17—C18—H18119.7
C11—C10—H10A108.2C20—C19—C18119.70 (13)
C9—C10—H10A108.2C20—C19—H19120.2
C11—C10—H10B108.2C18—C19—H19120.1
C9—C10—H10B108.2C19—C20—C21120.16 (14)
H10A—C10—H10B107.3C19—C20—H20119.9
C10—C11—C12116.04 (14)C21—C20—H20119.9
C10—C11—H11A108.3C20—C21—C16120.63 (13)
C12—C11—H11A108.3C20—C21—H21119.7
C10—C11—H11B108.3C16—C21—H21119.7
C12—C11—H11B108.3C15—N1—C1118.73 (10)
N1—C1—C2—C3178.99 (12)C10—C11—C12—C1398.63 (17)
C6—C1—C2—C30.70 (19)C11—C12—C13—C1470.55 (19)
C1—C2—C3—C40.6 (2)C12—C13—C14—C1580.42 (17)
C2—C3—C4—C50.0 (2)C7—C8—C15—N10.29 (18)
C2—C3—C4—Cl1179.69 (11)C9—C8—C15—N1178.45 (11)
C3—C4—C5—C60.7 (2)C7—C8—C15—C14179.14 (11)
Cl1—C4—C5—C6179.07 (9)C9—C8—C15—C142.13 (18)
C4—C5—C6—C10.59 (18)C13—C14—C15—N196.60 (14)
C4—C5—C6—C7178.98 (11)C13—C14—C15—C882.88 (16)
N1—C1—C6—C5179.60 (10)C8—C7—C16—C17103.88 (15)
C2—C1—C6—C50.07 (17)C6—C7—C16—C1775.90 (16)
N1—C1—C6—C70.00 (17)C8—C7—C16—C2179.21 (16)
C2—C1—C6—C7179.67 (11)C6—C7—C16—C21101.02 (14)
C5—C6—C7—C8179.10 (11)C21—C16—C17—C181.2 (2)
C1—C6—C7—C80.48 (16)C7—C16—C17—C18178.19 (15)
C5—C6—C7—C160.69 (17)C16—C17—C18—C190.6 (3)
C1—C6—C7—C16179.74 (10)C17—C18—C19—C200.5 (3)
C6—C7—C8—C150.62 (17)C18—C19—C20—C211.0 (3)
C16—C7—C8—C15179.61 (10)C19—C20—C21—C160.3 (2)
C6—C7—C8—C9178.09 (11)C17—C16—C21—C200.8 (2)
C16—C7—C8—C91.68 (18)C7—C16—C21—C20177.74 (13)
C7—C8—C9—C1091.27 (15)C8—C15—N1—C10.19 (18)
C15—C8—C9—C1090.04 (15)C14—C15—N1—C1179.66 (10)
C8—C9—C10—C1146.24 (18)C6—C1—N1—C150.33 (18)
C9—C10—C11—C1259.62 (18)C2—C1—N1—C15179.34 (11)
Acknowledgements top

I am grateful to the Islamic Azad University, Dorood Branch, for financial support.

references
References top

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Stoe & Cie (2002). X-AREA and X-RED. Stoe & Cie, Darmstadt, Germany.