Literature DB >> 21754084

5,7-Dibromo-2-methyl-quinolin-8-ol.

Nicole Schmidt1, Anke Schwarzer, Edwin Weber.   

Abstract

In the title compound, C(10)H(7)Br(2)NO, the mol-ecule possesses a planar geometry with an r.m.s deviation of 0.0383 Å for all non-H atoms. The crystal structure displays O-H⋯N and C-H⋯O hydrogen bonding, as well as Br⋯Br contacts [3.6284 (4) Å].

Entities:  

Year:  2011        PMID: 21754084      PMCID: PMC3099784          DOI: 10.1107/S1600536811007434

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For a review of hy­droxy­quinolines in supra­molecular chemistry, see: Albrecht et al. (2008 ▶). Bei et al. (1997 ▶) report on group 4 metal alkyl complexes. The crystal structure of the parent 8-hy­droxy­quinoline is described by Banerjee & Saha (1986 ▶) and Roychowdhury et al. (1978 ▶). Choi & Chi (2004 ▶) used the title compound as the starting material for alkyl­amino-substituted quinoline-5,8-diones. For halogen inter­actions in mol­ecular crystal structures, see: Awwadi et al. (2006 ▶); Brammer et al. (2001 ▶); Metrangolo et al. (2008 ▶).

Experimental

Crystal data

C10H7Br2NO M = 316.99 Monoclinic, a = 22.2221 (5) Å b = 4.0479 (1) Å c = 21.7221 (4) Å β = 102.167 (1)° V = 1910.07 (7) Å3 Z = 8 Mo Kα radiation μ = 8.45 mm−1 T = 93 K 0.40 × 0.24 × 0.22 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2007 ▶) T min = 0.133, T max = 0.258 13437 measured reflections 1727 independent reflections 1629 reflections with I > 2σ(I) R int = 0.025

Refinement

R[F 2 > 2σ(F 2)] = 0.017 wR(F 2) = 0.046 S = 1.11 1727 reflections 129 parameters H-atom parameters constrained Δρmax = 0.36 e Å−3 Δρmin = −0.60 e Å−3 Data collection: SMART (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811007434/im2267sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536811007434/im2267Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C10H7Br2NOF(000) = 1216
Mr = 316.99Dx = 2.205 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 9610 reflections
a = 22.2221 (5) Åθ = 2.4–29.2°
b = 4.0479 (1) ŵ = 8.45 mm1
c = 21.7221 (4) ÅT = 93 K
β = 102.167 (1)°Piece, colourless
V = 1910.07 (7) Å30.40 × 0.24 × 0.22 mm
Z = 8
Bruker SMART CCD area-detector diffractometer1727 independent reflections
Radiation source: fine-focus sealed tube1629 reflections with I > 2σ(I)
graphiteRint = 0.025
φ and ω scansθmax = 25.2°, θmin = 1.9°
Absorption correction: multi-scan (SADABS; Bruker, 2007)h = −26→25
Tmin = 0.133, Tmax = 0.258k = −4→4
13437 measured reflectionsl = −26→26
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.017Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.046H-atom parameters constrained
S = 1.11w = 1/[σ2(Fo2) + (0.0262P)2 + 2.9807P] where P = (Fo2 + 2Fc2)/3
1727 reflections(Δ/σ)max = 0.001
129 parametersΔρmax = 0.36 e Å3
0 restraintsΔρmin = −0.60 e Å3
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.
xyzUiso*/Ueq
Br10.226304 (10)0.34054 (6)0.083369 (10)0.02104 (8)
Br20.431764 (10)1.01225 (5)0.033388 (9)0.02065 (8)
N10.42288 (8)0.6326 (4)0.26148 (8)0.0151 (4)
O10.47717 (7)0.9601 (4)0.17443 (7)0.0197 (3)
H10.50120.84410.20090.030*
C10.39566 (10)0.4874 (5)0.30307 (10)0.0168 (4)
C20.33816 (10)0.3287 (5)0.28492 (10)0.0198 (5)
H20.32040.22130.31570.024*
C30.30807 (10)0.3291 (5)0.22338 (10)0.0186 (5)
H30.26930.22230.21110.022*
C40.33477 (10)0.4888 (5)0.17805 (10)0.0144 (4)
C50.30664 (10)0.5140 (5)0.11344 (10)0.0155 (4)
C60.33502 (10)0.6709 (5)0.07179 (10)0.0174 (4)
H60.31540.68590.02860.021*
C70.39324 (10)0.8094 (5)0.09334 (10)0.0150 (4)
C80.42345 (10)0.8007 (5)0.15583 (10)0.0145 (4)
C90.39347 (10)0.6360 (5)0.19921 (9)0.0137 (4)
C100.42720 (11)0.4996 (6)0.37143 (10)0.0224 (5)
H10A0.46680.38400.37740.034*
H10B0.40120.39230.39680.034*
H10C0.43420.73030.38470.034*
U11U22U33U12U13U23
Br10.01485 (13)0.02683 (14)0.02053 (13)−0.00403 (8)0.00170 (9)−0.00389 (8)
Br20.02015 (14)0.02857 (14)0.01417 (13)−0.00252 (9)0.00577 (9)0.00366 (8)
N10.0131 (9)0.0189 (9)0.0133 (8)0.0042 (7)0.0024 (7)0.0016 (7)
O10.0130 (8)0.0279 (9)0.0169 (8)−0.0037 (6)0.0001 (6)0.0048 (6)
C10.0168 (11)0.0181 (11)0.0160 (10)0.0068 (8)0.0048 (9)0.0025 (8)
C20.0196 (12)0.0220 (12)0.0198 (11)0.0029 (9)0.0088 (9)0.0040 (9)
C30.0142 (11)0.0193 (11)0.0233 (11)0.0004 (8)0.0063 (9)0.0011 (9)
C40.0124 (11)0.0144 (10)0.0172 (11)0.0037 (8)0.0045 (8)−0.0007 (8)
C50.0114 (10)0.0159 (10)0.0187 (10)0.0005 (8)0.0021 (8)−0.0027 (8)
C60.0174 (11)0.0210 (11)0.0133 (10)0.0041 (9)0.0022 (8)−0.0015 (8)
C70.0157 (11)0.0168 (10)0.0143 (10)0.0023 (8)0.0071 (8)0.0017 (8)
C80.0113 (10)0.0153 (10)0.0174 (10)0.0032 (8)0.0039 (8)0.0003 (8)
C90.0131 (11)0.0152 (10)0.0130 (10)0.0043 (8)0.0030 (8)−0.0011 (8)
C100.0236 (13)0.0286 (13)0.0152 (11)0.0026 (9)0.0047 (9)0.0035 (9)
Br1—C51.901 (2)C3—H30.9500
Br2—C71.890 (2)C4—C51.415 (3)
N1—C11.326 (3)C4—C91.420 (3)
N1—C91.373 (3)C5—C61.364 (3)
O1—C81.342 (3)C6—C71.397 (3)
O1—H10.8400C6—H60.9500
C1—C21.410 (3)C7—C81.382 (3)
C1—C101.503 (3)C8—C91.429 (3)
C2—C31.363 (3)C10—H10A0.9800
C2—H20.9500C10—H10B0.9800
C3—C41.409 (3)C10—H10C0.9800
C1—N1—C9119.01 (18)C5—C6—H6120.3
C8—O1—H1109.5C7—C6—H6120.3
N1—C1—C2121.88 (19)C8—C7—C6122.87 (19)
N1—C1—C10118.3 (2)C8—C7—Br2119.40 (16)
C2—C1—C10119.8 (2)C6—C7—Br2117.73 (15)
C3—C2—C1120.1 (2)O1—C8—C7120.03 (19)
C3—C2—H2119.9O1—C8—C9122.33 (18)
C1—C2—H2119.9C7—C8—C9117.52 (19)
C2—C3—C4119.6 (2)N1—C9—C4121.94 (19)
C2—C3—H3120.2N1—C9—C8117.59 (18)
C4—C3—H3120.2C4—C9—C8120.45 (18)
C3—C4—C5124.3 (2)C1—C10—H10A109.5
C3—C4—C9117.38 (19)C1—C10—H10B109.5
C5—C4—C9118.34 (19)H10A—C10—H10B109.5
C6—C5—C4121.5 (2)C1—C10—H10C109.5
C6—C5—Br1118.43 (16)H10A—C10—H10C109.5
C4—C5—Br1120.05 (16)H10B—C10—H10C109.5
C5—C6—C7119.32 (19)
C9—N1—C1—C21.8 (3)C6—C7—C8—O1−174.87 (19)
C9—N1—C1—C10−177.25 (18)Br2—C7—C8—O15.8 (3)
N1—C1—C2—C3−1.8 (3)C6—C7—C8—C91.2 (3)
C10—C1—C2—C3177.2 (2)Br2—C7—C8—C9−178.10 (15)
C1—C2—C3—C40.0 (3)C1—N1—C9—C40.0 (3)
C2—C3—C4—C5−177.7 (2)C1—N1—C9—C8178.67 (18)
C2—C3—C4—C91.6 (3)C3—C4—C9—N1−1.7 (3)
C3—C4—C5—C6−179.7 (2)C5—C4—C9—N1177.67 (18)
C9—C4—C5—C61.0 (3)C3—C4—C9—C8179.69 (19)
C3—C4—C5—Br12.5 (3)C5—C4—C9—C8−1.0 (3)
C9—C4—C5—Br1−176.86 (14)O1—C8—C9—N1−2.8 (3)
C4—C5—C6—C70.1 (3)C7—C8—C9—N1−178.78 (18)
Br1—C5—C6—C7177.96 (15)O1—C8—C9—C4175.90 (18)
C5—C6—C7—C8−1.3 (3)C7—C8—C9—C4−0.1 (3)
C5—C6—C7—Br2178.09 (16)
D—H···AD—HH···AD···AD—H···A
O1—H1···N1i0.841.922.707 (2)157
C10—H10A···O1ii0.982.523.342 (3)141
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O1—H1⋯N1i0.841.922.707 (2)157
C10—H10A⋯O1ii0.982.523.342 (3)141

Symmetry codes: (i) ; (ii) .

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1.  The nature of halogen...halogen synthons: crystallographic and theoretical studies.

Authors:  Firas F Awwadi; Roger D Willett; Kirk A Peterson; Brendan Twamley
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