organic compounds
3-Chloro-4-methylquinolin-2(1H)-one
aDepartment of Pharmaceutical Chemistry, College of Pharmacy, King Saud University, PO Box 2457, Riyadh 11451, Saudi Arabia, and bX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia
*Correspondence e-mail: hkfun@usm.my
The title compound, C10H8ClNO, is almost planar (r.m.s. deviation for the 13 non-H atoms = 0.023 Å). In the crystal, inversion dimers linked by pairs of N—H⋯O hydrogen bonds generate R22(8) rings. Weak aromatic π–π stacking interactions [centroid–centroid distance = 3.7622 (12) Å] also occur.
Related literature
For the biological activity of quinoline, see: Michael et al. (1996). For the synthesis, see: Hodgkinson & Staskun (1969). For hydrogen-bond motifs, see: Bernstein et al. (1995). For a related structure, see: Vasuki et al. (2001). For bond-length data, see: Allen et al. (1987).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2009); cell SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).
Supporting information
10.1107/S1600536812009889/hb6671sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812009889/hb6671Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812009889/hb6671Isup3.cml
This compound was prepared according to the reported method (Hodgkinson & Staskun, 1969). Colorless needles of the title compound were grown from a mixed solution of EtOH/DMF (V/V = 2/1) by slow evaporation at room temperature.
Atom H1 was located from the difference map and was fixed at their found positions with Uiso(H) = 1.2 Ueq(N) [N–H = 0.9256 Å]. The remaining H atoms were positioned geometrically and refined using a riding model with Uiso(H) = 1.2 or 1.5Ueq(C) (C—H = 0.93 and 0.96 Å). A rotating group model was applied to the methyl group.
For the previous reports of the chemistry and the biological activity of quinolines, see Michael et al. (1996).
In the title compound (Fig. 1), the quinoline ring (N1/C1–C9) is essentially planar with a maximum deviation of 0.012 (2) Å at atom C1. The bond lengths (Allen et al., 1987) and angles are within normal ranges are comparable to the related structure (Vasuki et al., 2001).
In the π—π interactions between the benzene ring (Cg1; C4–C9) and quinoline ring (Cg2; N1/C1–C9). [Cg1···Cg2 = 3.7622 (12) Å; 1+x, y, z].
(Fig. 2), the adjacent molecules are linked via pair of N1—H1···O1 (Table 1) hydrogen bonds, forming dimers with an R22 (8) ring motif (Bernstein et al., 1995). The is further stabilized by weakFor the biological activity of quinoline, see: Michael et al. (1996). For the synthesis, see: Hodgkinson & Staskun (1969). For hydrogen-bond motifs, see: Bernstein et al. (1995). For a related structure, see: Vasuki et al. (2001). For bond-length data, see: Allen et al. (1987).
Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).C10H8ClNO | F(000) = 400 |
Mr = 193.62 | Dx = 1.502 Mg m−3 |
Monoclinic, P21/c | Cu Kα radiation, λ = 1.54178 Å |
Hall symbol: -P 2ybc | Cell parameters from 615 reflections |
a = 3.9361 (2) Å | θ = 4.3–63.6° |
b = 12.9239 (6) Å | µ = 3.56 mm−1 |
c = 17.1019 (7) Å | T = 296 K |
β = 100.197 (4)° | Needle, colourless |
V = 856.23 (7) Å3 | 0.92 × 0.10 × 0.10 mm |
Z = 4 |
Bruker APEXII CCD diffractometer | 1434 independent reflections |
Radiation source: fine-focus sealed tube | 1178 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.040 |
φ and ω scans | θmax = 64.9°, θmin = 4.3° |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −4→3 |
Tmin = 0.138, Tmax = 0.720 | k = −15→14 |
5522 measured reflections | l = −20→17 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.037 | H-atom parameters constrained |
wR(F2) = 0.105 | w = 1/[σ2(Fo2) + (0.0755P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.00 | (Δ/σ)max = 0.001 |
1434 reflections | Δρmax = 0.18 e Å−3 |
120 parameters | Δρmin = −0.21 e Å−3 |
0 restraints | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0031 (9) |
C10H8ClNO | V = 856.23 (7) Å3 |
Mr = 193.62 | Z = 4 |
Monoclinic, P21/c | Cu Kα radiation |
a = 3.9361 (2) Å | µ = 3.56 mm−1 |
b = 12.9239 (6) Å | T = 296 K |
c = 17.1019 (7) Å | 0.92 × 0.10 × 0.10 mm |
β = 100.197 (4)° |
Bruker APEXII CCD diffractometer | 1434 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | 1178 reflections with I > 2σ(I) |
Tmin = 0.138, Tmax = 0.720 | Rint = 0.040 |
5522 measured reflections |
R[F2 > 2σ(F2)] = 0.037 | 0 restraints |
wR(F2) = 0.105 | H-atom parameters constrained |
S = 1.00 | Δρmax = 0.18 e Å−3 |
1434 reflections | Δρmin = −0.21 e Å−3 |
120 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 1.04066 (14) | 0.51266 (4) | 0.76645 (3) | 0.0516 (2) | |
O1 | 1.0673 (4) | 0.46152 (12) | 0.60239 (9) | 0.0560 (4) | |
N1 | 0.7804 (4) | 0.60196 (13) | 0.54512 (9) | 0.0422 (4) | |
H1 | 0.7928 | 0.5780 | 0.4947 | 0.051* | |
C1 | 0.9152 (5) | 0.54435 (15) | 0.60939 (12) | 0.0414 (4) | |
C2 | 0.8689 (5) | 0.58782 (15) | 0.68546 (11) | 0.0386 (4) | |
C3 | 0.7149 (4) | 0.68001 (14) | 0.69302 (11) | 0.0371 (4) | |
C4 | 0.5836 (5) | 0.73765 (14) | 0.62192 (11) | 0.0368 (4) | |
C5 | 0.4234 (5) | 0.83478 (16) | 0.62245 (12) | 0.0446 (5) | |
H5A | 0.3935 | 0.8637 | 0.6706 | 0.054* | |
C6 | 0.3104 (6) | 0.88763 (17) | 0.55307 (14) | 0.0529 (6) | |
H6A | 0.2094 | 0.9525 | 0.5546 | 0.064* | |
C7 | 0.3468 (6) | 0.84441 (18) | 0.48054 (14) | 0.0552 (6) | |
H7A | 0.2690 | 0.8804 | 0.4337 | 0.066* | |
C8 | 0.4965 (5) | 0.74913 (17) | 0.47760 (12) | 0.0477 (5) | |
H8A | 0.5166 | 0.7198 | 0.4290 | 0.057* | |
C9 | 0.6184 (5) | 0.69643 (15) | 0.54803 (11) | 0.0385 (4) | |
C10 | 0.6782 (6) | 0.72335 (16) | 0.77284 (11) | 0.0468 (5) | |
H10A | 0.7537 | 0.6728 | 0.8133 | 0.070* | |
H10B | 0.4407 | 0.7403 | 0.7728 | 0.070* | |
H10C | 0.8168 | 0.7846 | 0.7833 | 0.070* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0660 (4) | 0.0475 (3) | 0.0416 (3) | 0.0056 (2) | 0.0105 (2) | 0.0074 (2) |
O1 | 0.0806 (11) | 0.0439 (9) | 0.0462 (9) | 0.0171 (8) | 0.0183 (7) | −0.0027 (7) |
N1 | 0.0548 (10) | 0.0398 (9) | 0.0339 (9) | 0.0011 (7) | 0.0134 (7) | −0.0035 (7) |
C1 | 0.0486 (11) | 0.0363 (10) | 0.0412 (10) | −0.0011 (8) | 0.0129 (8) | −0.0036 (8) |
C2 | 0.0443 (10) | 0.0376 (10) | 0.0351 (10) | −0.0038 (7) | 0.0104 (7) | 0.0000 (8) |
C3 | 0.0386 (10) | 0.0392 (10) | 0.0349 (10) | −0.0065 (7) | 0.0105 (7) | −0.0042 (8) |
C4 | 0.0369 (10) | 0.0363 (10) | 0.0382 (10) | −0.0046 (7) | 0.0090 (7) | −0.0041 (8) |
C5 | 0.0451 (11) | 0.0415 (11) | 0.0474 (12) | −0.0002 (8) | 0.0086 (8) | −0.0062 (9) |
C6 | 0.0528 (12) | 0.0430 (11) | 0.0610 (14) | 0.0065 (9) | 0.0046 (10) | 0.0014 (10) |
C7 | 0.0574 (13) | 0.0547 (14) | 0.0506 (13) | 0.0009 (10) | 0.0014 (10) | 0.0121 (10) |
C8 | 0.0559 (12) | 0.0498 (12) | 0.0374 (11) | −0.0005 (9) | 0.0084 (8) | 0.0017 (9) |
C9 | 0.0395 (10) | 0.0389 (10) | 0.0380 (10) | −0.0045 (7) | 0.0096 (7) | −0.0026 (8) |
C10 | 0.0551 (12) | 0.0491 (12) | 0.0380 (10) | 0.0024 (9) | 0.0128 (8) | −0.0080 (9) |
Cl1—C2 | 1.728 (2) | C5—C6 | 1.373 (3) |
O1—C1 | 1.243 (3) | C5—H5A | 0.9300 |
N1—C1 | 1.355 (3) | C6—C7 | 1.391 (3) |
N1—C9 | 1.382 (3) | C6—H6A | 0.9300 |
N1—H1 | 0.9256 | C7—C8 | 1.370 (3) |
C1—C2 | 1.458 (3) | C7—H7A | 0.9300 |
C2—C3 | 1.353 (3) | C8—C9 | 1.393 (3) |
C3—C4 | 1.442 (3) | C8—H8A | 0.9300 |
C3—C10 | 1.506 (2) | C10—H10A | 0.9600 |
C4—C9 | 1.400 (3) | C10—H10B | 0.9600 |
C4—C5 | 1.406 (3) | C10—H10C | 0.9600 |
C1—N1—C9 | 124.95 (17) | C5—C6—C7 | 120.2 (2) |
C1—N1—H1 | 119.6 | C5—C6—H6A | 119.9 |
C9—N1—H1 | 115.4 | C7—C6—H6A | 119.9 |
O1—C1—N1 | 121.42 (18) | C8—C7—C6 | 120.4 (2) |
O1—C1—C2 | 123.80 (19) | C8—C7—H7A | 119.8 |
N1—C1—C2 | 114.78 (17) | C6—C7—H7A | 119.8 |
C3—C2—C1 | 123.60 (18) | C7—C8—C9 | 119.5 (2) |
C3—C2—Cl1 | 122.45 (15) | C7—C8—H8A | 120.3 |
C1—C2—Cl1 | 113.93 (15) | C9—C8—H8A | 120.3 |
C2—C3—C4 | 118.30 (17) | N1—C9—C8 | 119.43 (18) |
C2—C3—C10 | 122.04 (18) | N1—C9—C4 | 119.21 (18) |
C4—C3—C10 | 119.65 (17) | C8—C9—C4 | 121.37 (19) |
C9—C4—C5 | 117.48 (18) | C3—C10—H10A | 109.5 |
C9—C4—C3 | 119.13 (18) | C3—C10—H10B | 109.5 |
C5—C4—C3 | 123.38 (18) | H10A—C10—H10B | 109.5 |
C6—C5—C4 | 121.0 (2) | C3—C10—H10C | 109.5 |
C6—C5—H5A | 119.5 | H10A—C10—H10C | 109.5 |
C4—C5—H5A | 119.5 | H10B—C10—H10C | 109.5 |
C9—N1—C1—O1 | −177.64 (19) | C9—C4—C5—C6 | −0.9 (3) |
C9—N1—C1—C2 | 1.9 (3) | C3—C4—C5—C6 | 178.36 (19) |
O1—C1—C2—C3 | 177.3 (2) | C4—C5—C6—C7 | 1.4 (3) |
N1—C1—C2—C3 | −2.2 (3) | C5—C6—C7—C8 | −0.3 (3) |
O1—C1—C2—Cl1 | −0.8 (3) | C6—C7—C8—C9 | −1.2 (3) |
N1—C1—C2—Cl1 | 179.65 (14) | C1—N1—C9—C8 | 178.74 (18) |
C1—C2—C3—C4 | 1.2 (3) | C1—N1—C9—C4 | −0.6 (3) |
Cl1—C2—C3—C4 | 179.19 (13) | C7—C8—C9—N1 | −177.72 (19) |
C1—C2—C3—C10 | −178.76 (18) | C7—C8—C9—C4 | 1.6 (3) |
Cl1—C2—C3—C10 | −0.7 (3) | C5—C4—C9—N1 | 178.79 (17) |
C2—C3—C4—C9 | 0.2 (3) | C3—C4—C9—N1 | −0.5 (3) |
C10—C3—C4—C9 | −179.84 (16) | C5—C4—C9—C8 | −0.5 (3) |
C2—C3—C4—C5 | −179.06 (18) | C3—C4—C9—C8 | −179.88 (17) |
C10—C3—C4—C5 | 0.9 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.93 | 1.91 | 2.816 (2) | 166 |
Symmetry code: (i) −x+2, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C10H8ClNO |
Mr | 193.62 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 296 |
a, b, c (Å) | 3.9361 (2), 12.9239 (6), 17.1019 (7) |
β (°) | 100.197 (4) |
V (Å3) | 856.23 (7) |
Z | 4 |
Radiation type | Cu Kα |
µ (mm−1) | 3.56 |
Crystal size (mm) | 0.92 × 0.10 × 0.10 |
Data collection | |
Diffractometer | Bruker APEXII CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2009) |
Tmin, Tmax | 0.138, 0.720 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5522, 1434, 1178 |
Rint | 0.040 |
(sin θ/λ)max (Å−1) | 0.587 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.037, 0.105, 1.00 |
No. of reflections | 1434 |
No. of parameters | 120 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.18, −0.21 |
Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.93 | 1.91 | 2.816 (2) | 166 |
Symmetry code: (i) −x+2, −y+1, −z+1. |
Footnotes
‡Thomson Reuters ResearcherID: A-3561-2009.
Acknowledgements
HKF and CWO thank Universiti Sains Malaysia (USM) for the Research University Grant (1001/PFIZIK/811160). CWO also thanks the Malaysian Government and USM for the award of the post of research assistant under the Research University Grant (1001/PFIZIK/811151). The authors thank the Deanship of Scientific Research and the Research Center, College of Pharmacy, King Saud University.
References
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For the previous reports of the chemistry and the biological activity of quinolines, see Michael et al. (1996).
In the title compound (Fig. 1), the quinoline ring (N1/C1–C9) is essentially planar with a maximum deviation of 0.012 (2) Å at atom C1. The bond lengths (Allen et al., 1987) and angles are within normal ranges are comparable to the related structure (Vasuki et al., 2001).
In the crystal structure (Fig. 2), the adjacent molecules are linked via pair of N1—H1···O1 (Table 1) hydrogen bonds, forming dimers with an R22 (8) ring motif (Bernstein et al., 1995). The crystal structure is further stabilized by weak π—π interactions between the benzene ring (Cg1; C4–C9) and quinoline ring (Cg2; N1/C1–C9). [Cg1···Cg2 = 3.7622 (12) Å; 1+x, y, z].