organic compounds
2,4-Dichloroquinoline
aDepartment of Chemistry, Faculty of Technology, Tomas Bata University in Zlin, Nám. T.G. Masaryka 275, Zlín,762 72, Czech Republic, and bDepartment of Chemistry, Faculty of Science, Masaryk University in Brno, Kamenice 5, Brno-Bohunice, 625 00, Czech Republic
*Correspondence e-mail: rvicha@ft.utb.cz
The 9H5Cl2N, consists of two crystallographically independent molecules. In both molecules the quinoline ring system is essentially planar [maximum deviations from the best plane of 0.0232 (13) 0.0089 (15) Å]. The angle between these planes is 22.40 (3)°. Conformers A and B are arranged face-to-face along the c axis, forming alternating pairs in the order AABB. The interplanar distances AA, AB and BB are 3.3166 (11), 3.2771 (11) and 3.3935 (11) Å, respectively. The crystal packing is stabilized by weak C—H⋯Cl and C—H⋯N interactions.
of the title compound, CRelated literature
For previous syntheses of title compound, see: Baeyer & Bloem (1882); Steinschifter & Stadlbauer (1994). For the use of the title compound in organic synthesis, see: Buchmann & Hamilton (1942).
Experimental
Crystal data
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Refinement
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Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97.
Supporting information
https://doi.org/10.1107/S160053681001576X/bg2343sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S160053681001576X/bg2343Isup2.hkl
4-Hydroxyquinolin-2-one (322 mg, 2 mmol) and POCl3 (2 ml) were treated for 15 min. at 100°C. Reaction mixture was poured onto finely crushed ice to decompose an excess of POCl3. Basicity was adjusted to pH =8 using Na2CO3 and resulting precipitate was filtered off. The solid on the filter was washed with water and dried at room temperature to yield 292 mg (74%) of title compound.The single crystal used for data collection was obtained by crystallisation from diethyl ether at room temperature.
Although the 2,4-dichloroquinoline is well known for more than hundred years (Baeyer & Bloem, 1882) and has been widely used in quinoline chemistry (Buchmann & Hamilton, 1942; Steinschifter & Stadlbauer, 1994), no structure data has been published so far.
The title compound (Fig. 1) crystallises with two crystallographical independent molecules in π–π interactions. The distances between AA, AB and BB planes calculated as a distance of nitrogen atom from adjacent ring plane are 3.3166 (11), 3.2771 (11) and 3.3935 (11) Å, respectively. Molecular packing is stabilised by C—H···Cl and C—H···N weak interactions (Fig. 2, Table 1).
Conformers A and B differ very little in geometrical parameters. Both of them consist of essentially planar quinoline ring with maximum deviations from the best planes being 0.0232 (13) Å for atom C2 (conformer A) and 0.0089 (15) Å for atom C17 (conformer B). The angle between these quinoline best planes is 22.40 (3)°. Chlorine atoms lay almost in the ring best planes with the deviations 0.0035 (4) Å for atom Cl1 and -0.0011 (4) for atom Cl2 (conformer A) and -0.0081 (4) Å for atom Cl3 and 0.0121 (4) Å for atom Cl4 (conformer B). Pairs of conformers are stacked along the c axes in AABB arrangement stabilised via offsetFor previous syntheses of title compound, see: Baeyer & Bloem (1882); Steinschifter & Stadlbauer (1994). For the use of the title compound in organic synthesis, see: Buchmann & Hamilton (1942).
Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell
CrysAlis CCD (Oxford Diffraction, 2006); data reduction: CrysAlis RED (Oxford Diffraction, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C9H5Cl2N | F(000) = 800 |
Mr = 198.04 | Dx = 1.580 Mg m−3 |
Monoclinic, P21/n | Melting point: 335(1) K |
Hall symbol: -P 2yn | Mo Kα radiation, λ = 0.71073 Å |
a = 10.3689 (3) Å | Cell parameters from 14773 reflections |
b = 11.9215 (3) Å | θ = 2.9–27.1° |
c = 13.6380 (5) Å | µ = 0.71 mm−1 |
β = 98.937 (3)° | T = 120 K |
V = 1665.37 (9) Å3 | Block, yellow |
Z = 8 | 0.40 × 0.40 × 0.30 mm |
Kuma KM-4-CCD diffractometer | 2927 independent reflections |
Radiation source: fine-focus sealed tube | 2504 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.012 |
ω scan | θmax = 25.0°, θmin = 2.9° |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2006) | h = −12→12 |
Tmin = 0.60, Tmax = 0.81 | k = −14→14 |
13224 measured reflections | l = −16→13 |
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)] = 0.021 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.066 | H-atom parameters constrained |
S = 1.08 | w = 1/[σ2(Fo2) + (0.041P)2 + 0.2572P] where P = (Fo2 + 2Fc2)/3 |
2927 reflections | (Δ/σ)max = 0.005 |
217 parameters | Δρmax = 0.25 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
C9H5Cl2N | V = 1665.37 (9) Å3 |
Mr = 198.04 | Z = 8 |
Monoclinic, P21/n | Mo Kα radiation |
a = 10.3689 (3) Å | µ = 0.71 mm−1 |
b = 11.9215 (3) Å | T = 120 K |
c = 13.6380 (5) Å | 0.40 × 0.40 × 0.30 mm |
β = 98.937 (3)° |
Kuma KM-4-CCD diffractometer | 2927 independent reflections |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2006) | 2504 reflections with I > 2σ(I) |
Tmin = 0.60, Tmax = 0.81 | Rint = 0.012 |
13224 measured reflections |
R[F2 > 2σ(F2)] = 0.021 | 0 restraints |
wR(F2) = 0.066 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.25 e Å−3 |
2927 reflections | Δρmin = −0.22 e Å−3 |
217 parameters |
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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ 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 | 0.13384 (3) | 0.03305 (3) | 0.08803 (3) | 0.02540 (11) | |
Cl2 | 0.52857 (3) | 0.32412 (3) | 0.17438 (3) | 0.02529 (11) | |
Cl3 | −0.36457 (3) | 0.59016 (3) | 0.06753 (3) | 0.02745 (11) | |
Cl4 | 0.02870 (3) | 0.30160 (3) | 0.16841 (3) | 0.02323 (11) | |
C1 | 0.30194 (13) | 0.05798 (11) | 0.10998 (10) | 0.0179 (3) | |
C2 | 0.34206 (13) | 0.16982 (11) | 0.12943 (10) | 0.0184 (3) | |
H2A | 0.2808 | 0.2290 | 0.1297 | 0.022* | |
C3 | 0.47285 (13) | 0.18864 (11) | 0.14782 (10) | 0.0170 (3) | |
C4 | 0.56380 (13) | 0.09974 (11) | 0.14534 (9) | 0.0174 (3) | |
C5 | 0.70140 (13) | 0.11242 (12) | 0.16231 (10) | 0.0218 (3) | |
H5A | 0.7389 | 0.1842 | 0.1779 | 0.026* | |
C6 | 0.78035 (14) | 0.02124 (13) | 0.15621 (11) | 0.0262 (3) | |
H6A | 0.8725 | 0.0303 | 0.1677 | 0.031* | |
C7 | 0.72627 (14) | −0.08561 (13) | 0.13307 (10) | 0.0252 (3) | |
H7A | 0.7821 | −0.1479 | 0.1285 | 0.030* | |
C8 | 0.59391 (14) | −0.10019 (12) | 0.11718 (10) | 0.0217 (3) | |
H8A | 0.5585 | −0.1728 | 0.1021 | 0.026* | |
C9 | 0.50939 (13) | −0.00843 (11) | 0.12290 (9) | 0.0171 (3) | |
N1 | 0.37727 (11) | −0.02819 (9) | 0.10649 (8) | 0.0178 (3) | |
C11 | −0.19672 (13) | 0.56562 (11) | 0.09168 (10) | 0.0185 (3) | |
C12 | −0.15678 (13) | 0.45494 (11) | 0.11711 (10) | 0.0179 (3) | |
H12A | −0.2182 | 0.3964 | 0.1204 | 0.022* | |
C13 | −0.02595 (13) | 0.43615 (11) | 0.13660 (9) | 0.0165 (3) | |
C14 | 0.06551 (13) | 0.52382 (11) | 0.13046 (9) | 0.0175 (3) | |
C15 | 0.20256 (13) | 0.51151 (12) | 0.14938 (10) | 0.0217 (3) | |
H15A | 0.2400 | 0.4406 | 0.1684 | 0.026* | |
C16 | 0.28175 (14) | 0.60210 (13) | 0.14029 (11) | 0.0274 (3) | |
H16A | 0.3739 | 0.5931 | 0.1530 | 0.033* | |
C17 | 0.22853 (15) | 0.70773 (13) | 0.11250 (11) | 0.0281 (4) | |
H17A | 0.2847 | 0.7694 | 0.1063 | 0.034* | |
C18 | 0.09590 (15) | 0.72227 (12) | 0.09421 (10) | 0.0248 (3) | |
H18A | 0.0607 | 0.7941 | 0.0756 | 0.030* | |
C19 | 0.01108 (13) | 0.63129 (11) | 0.10277 (10) | 0.0183 (3) | |
N2 | −0.12097 (11) | 0.65102 (9) | 0.08387 (8) | 0.0200 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.01550 (19) | 0.0246 (2) | 0.0355 (2) | −0.00423 (13) | 0.00217 (15) | −0.00300 (15) |
Cl2 | 0.0226 (2) | 0.01604 (18) | 0.0354 (2) | −0.00448 (13) | −0.00113 (16) | −0.00104 (14) |
Cl3 | 0.0184 (2) | 0.0270 (2) | 0.0358 (2) | 0.00475 (14) | 0.00067 (15) | 0.00256 (16) |
Cl4 | 0.0236 (2) | 0.01571 (18) | 0.0307 (2) | 0.00392 (13) | 0.00519 (15) | 0.00299 (13) |
C1 | 0.0150 (7) | 0.0223 (7) | 0.0163 (7) | −0.0019 (5) | 0.0016 (6) | 0.0001 (5) |
C2 | 0.0180 (7) | 0.0169 (7) | 0.0202 (7) | 0.0016 (5) | 0.0027 (6) | 0.0009 (5) |
C3 | 0.0210 (7) | 0.0151 (7) | 0.0145 (7) | −0.0023 (5) | 0.0011 (6) | 0.0006 (5) |
C4 | 0.0188 (7) | 0.0208 (7) | 0.0122 (7) | 0.0017 (5) | 0.0016 (5) | 0.0024 (5) |
C5 | 0.0175 (7) | 0.0274 (8) | 0.0203 (7) | −0.0019 (6) | 0.0021 (6) | 0.0027 (6) |
C6 | 0.0165 (7) | 0.0394 (9) | 0.0225 (8) | 0.0053 (6) | 0.0020 (6) | 0.0050 (7) |
C7 | 0.0258 (8) | 0.0320 (8) | 0.0179 (8) | 0.0129 (6) | 0.0038 (6) | 0.0032 (6) |
C8 | 0.0294 (8) | 0.0197 (7) | 0.0162 (7) | 0.0053 (6) | 0.0043 (6) | 0.0007 (6) |
C9 | 0.0201 (7) | 0.0202 (7) | 0.0108 (7) | 0.0016 (6) | 0.0019 (5) | 0.0022 (5) |
N1 | 0.0198 (6) | 0.0172 (6) | 0.0161 (6) | −0.0011 (5) | 0.0018 (5) | 0.0001 (5) |
C11 | 0.0183 (7) | 0.0204 (7) | 0.0167 (7) | 0.0016 (5) | 0.0023 (6) | −0.0016 (5) |
C12 | 0.0195 (7) | 0.0175 (7) | 0.0174 (7) | −0.0023 (5) | 0.0047 (6) | −0.0007 (5) |
C13 | 0.0212 (7) | 0.0149 (7) | 0.0134 (7) | 0.0020 (5) | 0.0033 (6) | −0.0004 (5) |
C14 | 0.0205 (7) | 0.0195 (7) | 0.0131 (7) | −0.0012 (6) | 0.0041 (6) | −0.0033 (5) |
C15 | 0.0192 (7) | 0.0259 (8) | 0.0201 (7) | 0.0003 (6) | 0.0037 (6) | −0.0035 (6) |
C16 | 0.0198 (8) | 0.0365 (9) | 0.0263 (8) | −0.0075 (6) | 0.0048 (6) | −0.0073 (7) |
C17 | 0.0292 (9) | 0.0296 (8) | 0.0261 (8) | −0.0146 (7) | 0.0060 (7) | −0.0049 (7) |
C18 | 0.0336 (9) | 0.0177 (7) | 0.0234 (8) | −0.0061 (6) | 0.0060 (6) | −0.0029 (6) |
C19 | 0.0228 (7) | 0.0186 (7) | 0.0138 (7) | −0.0017 (6) | 0.0039 (6) | −0.0035 (5) |
N2 | 0.0239 (7) | 0.0165 (6) | 0.0198 (6) | 0.0008 (5) | 0.0040 (5) | −0.0006 (5) |
Cl1—C1 | 1.7475 (13) | C8—H8A | 0.9500 |
Cl2—C3 | 1.7345 (13) | C9—N1 | 1.3738 (17) |
Cl3—C11 | 1.7450 (14) | C11—N2 | 1.3003 (18) |
Cl4—C13 | 1.7338 (13) | C11—C12 | 1.4100 (18) |
C1—N1 | 1.2959 (17) | C12—C13 | 1.3598 (19) |
C1—C2 | 1.4096 (18) | C12—H12A | 0.9500 |
C2—C3 | 1.3589 (19) | C13—C14 | 1.4225 (19) |
C2—H2A | 0.9500 | C14—C15 | 1.4120 (19) |
C3—C4 | 1.4225 (18) | C14—C19 | 1.4270 (19) |
C4—C5 | 1.4175 (19) | C15—C16 | 1.374 (2) |
C4—C9 | 1.4217 (19) | C15—H15A | 0.9500 |
C5—C6 | 1.371 (2) | C16—C17 | 1.403 (2) |
C5—H5A | 0.9500 | C16—H16A | 0.9500 |
C6—C7 | 1.408 (2) | C17—C18 | 1.370 (2) |
C6—H6A | 0.9500 | C17—H17A | 0.9500 |
C7—C8 | 1.367 (2) | C18—C19 | 1.4126 (19) |
C7—H7A | 0.9500 | C18—H18A | 0.9500 |
C8—C9 | 1.4114 (19) | C19—N2 | 1.3736 (18) |
N1—C1—C2 | 126.50 (12) | N2—C11—C12 | 126.50 (13) |
N1—C1—Cl1 | 116.73 (10) | N2—C11—Cl3 | 116.78 (10) |
C2—C1—Cl1 | 116.77 (10) | C12—C11—Cl3 | 116.72 (10) |
C3—C2—C1 | 116.60 (12) | C13—C12—C11 | 116.62 (12) |
C3—C2—H2A | 121.7 | C13—C12—H12A | 121.7 |
C1—C2—H2A | 121.7 | C11—C12—H12A | 121.7 |
C2—C3—C4 | 121.26 (12) | C12—C13—C14 | 121.43 (12) |
C2—C3—Cl2 | 118.87 (10) | C12—C13—Cl4 | 118.60 (10) |
C4—C3—Cl2 | 119.88 (10) | C14—C13—Cl4 | 119.97 (10) |
C5—C4—C3 | 124.81 (12) | C15—C14—C13 | 125.04 (13) |
C5—C4—C9 | 119.18 (12) | C15—C14—C19 | 119.15 (12) |
C3—C4—C9 | 116.01 (12) | C13—C14—C19 | 115.81 (12) |
C6—C5—C4 | 120.06 (13) | C16—C15—C14 | 120.03 (14) |
C6—C5—H5A | 120.0 | C16—C15—H15A | 120.0 |
C4—C5—H5A | 120.0 | C14—C15—H15A | 120.0 |
C5—C6—C7 | 120.67 (13) | C15—C16—C17 | 120.95 (14) |
C5—C6—H6A | 119.7 | C15—C16—H16A | 119.5 |
C7—C6—H6A | 119.7 | C17—C16—H16A | 119.5 |
C8—C7—C6 | 120.38 (13) | C18—C17—C16 | 120.28 (13) |
C8—C7—H7A | 119.8 | C18—C17—H17A | 119.9 |
C6—C7—H7A | 119.8 | C16—C17—H17A | 119.9 |
C7—C8—C9 | 120.63 (13) | C17—C18—C19 | 120.54 (14) |
C7—C8—H8A | 119.7 | C17—C18—H18A | 119.7 |
C9—C8—H8A | 119.7 | C19—C18—H18A | 119.7 |
N1—C9—C8 | 118.04 (12) | N2—C19—C18 | 117.92 (12) |
N1—C9—C4 | 122.89 (12) | N2—C19—C14 | 123.03 (12) |
C8—C9—C4 | 119.07 (12) | C18—C19—C14 | 119.04 (12) |
C1—N1—C9 | 116.71 (11) | C11—N2—C19 | 116.59 (11) |
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H2A···Cl4 | 0.95 | 2.88 | 3.7197 (14) | 148 |
C17—H17A···N1i | 0.95 | 2.60 | 3.5111 (19) | 162 |
C18—H18A···Cl1i | 0.95 | 2.95 | 3.7290 (15) | 141 |
Symmetry code: (i) x, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C9H5Cl2N |
Mr | 198.04 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 120 |
a, b, c (Å) | 10.3689 (3), 11.9215 (3), 13.6380 (5) |
β (°) | 98.937 (3) |
V (Å3) | 1665.37 (9) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 0.71 |
Crystal size (mm) | 0.40 × 0.40 × 0.30 |
Data collection | |
Diffractometer | Kuma KM-4-CCD |
Absorption correction | Multi-scan (CrysAlis RED; Oxford Diffraction, 2006) |
Tmin, Tmax | 0.60, 0.81 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 13224, 2927, 2504 |
Rint | 0.012 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.021, 0.066, 1.08 |
No. of reflections | 2927 |
No. of parameters | 217 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.25, −0.22 |
Computer programs: CrysAlis CCD (Oxford Diffraction, 2006), CrysAlis RED (Oxford Diffraction, 2006), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H2A···Cl4 | 0.95 | 2.88 | 3.7197 (14) | 148.3 |
C17—H17A···N1i | 0.95 | 2.60 | 3.5111 (19) | 162.0 |
C18—H18A···Cl1i | 0.95 | 2.95 | 3.7290 (15) | 140.5 |
Symmetry code: (i) x, y+1, z. |
Acknowledgements
The financial support of this work by the Czech Ministry of Education, project No. MSM 7088352101, and the Tomas Bata Foundation is gratefully acknowledged.
References
Baeyer, A. & Bloem, F. (1882). Ber. Dtsch. Chem. Ges. 15, 2147–2155. CrossRef Google Scholar
Buchmann, F. J. & Hamilton, C. S. (1942). J. Am. Chem. Soc. 64, 1357–1360. CrossRef CAS Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Oxford Diffraction (2006). CrysAlis CCD and CrysAlis RED. Oxford Diffraction Ltd., Abingdon, England. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Steinschifter, W. & Stadlbauer, W. (1994). J. Prakt. Chem. 336, 311–318. CrossRef CAS Web of Science Google Scholar
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Although the 2,4-dichloroquinoline is well known for more than hundred years (Baeyer & Bloem, 1882) and has been widely used in quinoline chemistry (Buchmann & Hamilton, 1942; Steinschifter & Stadlbauer, 1994), no structure data has been published so far.
The title compound (Fig. 1) crystallises with two crystallographical independent molecules in asymmetric unit. Conformers A and B differ very little in geometrical parameters. Both of them consist of essentially planar quinoline ring with maximum deviations from the best planes being 0.0232 (13) Å for atom C2 (conformer A) and 0.0089 (15) Å for atom C17 (conformer B). The angle between these quinoline best planes is 22.40 (3)°. Chlorine atoms lay almost in the ring best planes with the deviations 0.0035 (4) Å for atom Cl1 and -0.0011 (4) for atom Cl2 (conformer A) and -0.0081 (4) Å for atom Cl3 and 0.0121 (4) Å for atom Cl4 (conformer B). Pairs of conformers are stacked along the c axes in AABB arrangement stabilised via offset π–π interactions. The distances between AA, AB and BB planes calculated as a distance of nitrogen atom from adjacent ring plane are 3.3166 (11), 3.2771 (11) and 3.3935 (11) Å, respectively. Molecular packing is stabilised by C—H···Cl and C—H···N weak interactions (Fig. 2, Table 1).