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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 May 14;64(Pt 6):o1072. doi: 10.1107/S1600536808013305

Methyl 5-bromo-2-chloro­pyridine-3-carboxyl­ate

Yi Ma a,*, Ya-Lun Liu b
PMCID: PMC2961526  PMID: 21202590

Abstract

The title compound, C7H5BrClNO2, crystallizes with two independent molecules in the asymmetric unit. In the absence of classical inter­molecular inter­actions, the crystal structure exhibits relatively short inter­molecular Br⋯O distances [3.143 (9) and 3.162 (9)Å].

Related literature

For the biological activity of the title compound, see: Colarusso & Narjes (2004); Kim et al. (2006). For related crystal structures, see McArdle et al. (1982).graphic file with name e-64-o1072-scheme1.jpg

Experimental

Crystal data

  • C7H5BrClNO2

  • M r = 250.48

  • Triclinic, Inline graphic

  • a = 3.978 (2) Å

  • b = 8.153 (3) Å

  • c = 14.040 (2) Å

  • α = 96.89 (2)°

  • β = 96.20 (3)°

  • γ = 100.70 (2)°

  • V = 440.2 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 4.93 mm−1

  • T = 298 (2) K

  • 0.16 × 0.14 × 0.10 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2004) T min = 0.506, T max = 0.638

  • 2186 measured reflections

  • 1818 independent reflections

  • 1564 reflections with I > 2σ(I)

  • R int = 0.017

Refinement

  • R[F 2 > 2σ(F 2)] = 0.044

  • wR(F 2) = 0.130

  • S = 1.09

  • 1818 reflections

  • 217 parameters

  • 3 restraints

  • H-atom parameters constrained

  • Δρmax = 1.17 e Å−3

  • Δρmin = −0.90 e Å−3

  • Absolute structure: Flack (1983); 70 Friedel pairs

  • Flack parameter: 0.01 (2)

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); 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 local programs.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808013305/cv2402sup1.cif

e-64-o1072-sup1.cif (17.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808013305/cv2402Isup2.hkl

e-64-o1072-Isup2.hkl (89.5KB, hkl)

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

Table 1. Selected interatomic distances (Å).

Br1⋯O3i 3.143 (9)
Br2⋯O1ii 3.162 (9)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

supplementary crystallographic information

Comment

The title compound, (I), is a useful intermediate for the synthesis of various bioactive compounds (Colarusso et al., 2004; Kim et al., 2006). In this paper, we report its crystal structure.

Compound (I) crystallizes with two independent molecules in the non-centrosymmetric triclinic unit cell (Fig. 1). The bond lengths and angles in the molecules are normal and in a good agreement with those reported previously (McArdle et al., 1982). The dihedral angles between the planes of the methoxycarbonyl group (C6/C7/O1/O2; C13/C23/O3/O4) and pyridine rings in the two independent molecules are 45.8 (2) and 44.0 (3)°, respectively. In the abscence of classical intermolecular interactions, the crystal packing exhibits relatively short intermolecular Br···O distances (Table 1).

Experimental

A solution of 5-bromo-2-hydroxynicotinic acid (0.138 mol) and N, N-dimethylformamide (0.138 mol) in thionyl chloride (160 mL) was refluxed for 2 h. Thionyl chloride was evaporated and the yellow residue dissolved in anhydrous dichloromethane (200 mL), then anhydrous methanol was added dropwise. The resulting mixture was refluxed for 1 h and evaporated to afford slightly yellow oil which crystallized upon standing at room temperature. Crystals suitable for X-ray diffraction analysis were obtained by slow evaporation of an ethanol solution at room temperature over a period of one week.

Refinement

All H atoms were placed in calculated positions, with C—H = 0.93 or 0.96 Å, and included in the final cycles of refinement using a riding model, with Uiso(H) = 1.2–1.5 times Ueq(C).

Figures

Fig. 1.

Fig. 1.

Two independent molecules of (I) with atomic numbering and displacement ellipsoids drawn at the 40% probability level.

Crystal data

C7H5BrClNO2 Z = 2
Mr = 250.48 F000 = 244
Triclinic, P1 Dx = 1.890 Mg m3
Hall symbol: P 1 Mo Kα radiation λ = 0.71073 Å
a = 3.978 (2) Å Cell parameters from 947 reflections
b = 8.153 (3) Å θ = 2.6–24.3º
c = 14.040 (2) Å µ = 4.93 mm1
α = 96.89 (2)º T = 298 (2) K
β = 96.20 (3)º Block, colourless
γ = 100.70 (2)º 0.16 × 0.14 × 0.10 mm
V = 440.2 (3) Å3

Data collection

Bruker SMART CCD area-detector diffractometer 1818 independent reflections
Radiation source: fine-focus sealed tube 1564 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.017
T = 298(2) K θmax = 25.0º
φ and ω scans θmin = 1.5º
Absorption correction: multi-scan(SADABS; Sheldrick, 2004) h = −4→3
Tmin = 0.506, Tmax = 0.639 k = −9→9
2186 measured reflections l = −14→16

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.044   w = 1/[σ2(Fo2) + (0.0806P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.130 (Δ/σ)max < 0.001
S = 1.09 Δρmax = 1.17 e Å3
1818 reflections Δρmin = −0.90 e Å3
217 parameters Extinction correction: none
3 restraints Absolute structure: Flack (1983); 70 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.01 (2)
Secondary atom site location: difference Fourier map

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.
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.

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

x y z Uiso*/Ueq
Br1 0.3498 (2) 0.81123 (11) 0.74398 (8) 0.0523 (3)
Br2 0.3533 (3) 1.31291 (12) −0.24715 (8) 0.0530 (3)
Cl1 0.8539 (9) 0.7931 (4) 0.3331 (2) 0.0552 (7)
Cl2 1.2578 (8) 1.5050 (4) 0.1624 (2) 0.0555 (7)
O1 1.083 (3) 1.2390 (10) 0.5287 (6) 0.074 (3)
O2 0.762 (2) 1.1535 (9) 0.3865 (5) 0.0522 (19)
O3 1.295 (3) 1.8504 (10) −0.0331 (6) 0.080 (3)
O4 1.116 (2) 1.8360 (9) 0.1109 (5) 0.0529 (19)
N1 0.579 (3) 0.6646 (10) 0.4701 (7) 0.050 (2)
N2 0.843 (3) 1.3036 (11) 0.0259 (7) 0.053 (2)
C1 0.703 (3) 0.8099 (12) 0.4449 (7) 0.040 (2)
C2 0.735 (3) 0.9674 (12) 0.5010 (7) 0.037 (2)
C3 0.627 (3) 0.9656 (12) 0.5894 (7) 0.038 (2)
H3A 0.6454 1.0663 0.6303 0.045*
C4 0.490 (3) 0.8134 (12) 0.6187 (7) 0.042 (2)
C5 0.464 (3) 0.6665 (14) 0.5574 (8) 0.055 (3)
H5A 0.3658 0.5650 0.5764 0.066*
C6 0.880 (3) 1.1312 (12) 0.4727 (7) 0.043 (2)
C7 0.885 (3) 1.3097 (13) 0.3515 (8) 0.050 (3)
H7A 0.7729 1.3062 0.2869 0.076*
H7B 1.1297 1.3255 0.3511 0.076*
H7C 0.8330 1.4015 0.3931 0.076*
C8 0.995 (3) 1.4644 (13) 0.0517 (8) 0.042 (2)
C9 0.973 (3) 1.5908 (12) −0.0031 (7) 0.039 (2)
C10 0.783 (3) 1.5431 (12) −0.0957 (7) 0.042 (2)
H10A 0.7706 1.6217 −0.1381 0.050*
C11 0.616 (3) 1.3777 (12) −0.1223 (7) 0.040 (2)
C12 0.647 (3) 1.2631 (13) −0.0611 (8) 0.049 (3)
H12A 0.5287 1.1523 −0.0800 0.059*
C13 1.144 (3) 1.7723 (13) 0.0234 (7) 0.042 (2)
C14 1.289 (3) 2.0069 (11) 0.1478 (8) 0.047 (3)
H14A 1.2448 2.0350 0.2130 0.071*
H14B 1.2055 2.0824 0.1079 0.071*
H14C 1.5334 2.0172 0.1470 0.071*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.0550 (6) 0.0621 (6) 0.0479 (7) 0.0190 (5) 0.0166 (5) 0.0206 (5)
Br2 0.0487 (6) 0.0544 (6) 0.0496 (7) 0.0118 (4) −0.0056 (5) −0.0094 (5)
Cl1 0.068 (2) 0.0575 (15) 0.0389 (14) 0.0144 (14) 0.0110 (12) −0.0028 (12)
Cl2 0.067 (2) 0.0589 (16) 0.0397 (14) 0.0138 (14) −0.0012 (12) 0.0113 (12)
O1 0.092 (7) 0.049 (4) 0.064 (5) −0.012 (5) −0.013 (5) 0.010 (4)
O2 0.058 (5) 0.050 (4) 0.047 (4) 0.005 (4) 0.004 (4) 0.013 (3)
O3 0.115 (8) 0.056 (5) 0.059 (5) −0.019 (5) 0.029 (5) 0.005 (4)
O4 0.073 (6) 0.041 (4) 0.042 (4) 0.005 (4) 0.014 (4) −0.001 (3)
N1 0.059 (7) 0.034 (5) 0.053 (6) 0.009 (4) −0.006 (5) −0.001 (4)
N2 0.066 (7) 0.044 (5) 0.048 (6) 0.007 (5) 0.012 (5) 0.011 (4)
C1 0.035 (6) 0.041 (6) 0.043 (6) 0.006 (4) 0.007 (5) 0.003 (5)
C2 0.033 (6) 0.037 (5) 0.040 (5) 0.005 (4) −0.002 (4) 0.006 (4)
C3 0.042 (6) 0.041 (5) 0.031 (5) 0.011 (4) 0.007 (4) 0.006 (4)
C4 0.039 (6) 0.045 (6) 0.043 (6) 0.013 (4) 0.002 (4) 0.004 (4)
C5 0.057 (8) 0.047 (6) 0.057 (7) 0.005 (5) −0.001 (5) 0.010 (5)
C6 0.043 (7) 0.044 (6) 0.035 (5) 0.005 (5) −0.001 (4) −0.001 (4)
C7 0.070 (8) 0.037 (6) 0.049 (7) 0.005 (5) 0.024 (6) 0.019 (5)
C8 0.049 (7) 0.039 (6) 0.041 (6) 0.015 (5) 0.015 (5) 0.002 (4)
C9 0.047 (6) 0.038 (5) 0.033 (5) 0.006 (5) 0.013 (4) 0.006 (4)
C10 0.051 (7) 0.039 (5) 0.037 (5) 0.011 (5) 0.012 (4) 0.005 (4)
C11 0.031 (6) 0.045 (6) 0.044 (6) 0.004 (4) 0.004 (4) 0.005 (4)
C12 0.049 (7) 0.042 (6) 0.052 (6) 0.003 (5) 0.009 (5) −0.001 (5)
C13 0.038 (6) 0.049 (6) 0.039 (6) 0.007 (5) 0.006 (4) 0.011 (4)
C14 0.060 (7) 0.024 (5) 0.051 (7) 0.003 (5) 0.000 (5) −0.004 (4)

Geometric parameters (Å, °)

Br1—C4 1.902 (11) C3—C4 1.389 (14)
Br2—C11 1.902 (10) C3—H3A 0.9300
Cl1—C1 1.740 (10) C4—C5 1.370 (15)
Cl2—C8 1.736 (12) C5—H5A 0.9300
O1—C6 1.215 (11) C7—H7A 0.9600
O2—C6 1.296 (11) C7—H7B 0.9600
O2—C7 1.439 (12) C7—H7C 0.9600
O3—C13 1.215 (11) C8—C9 1.368 (14)
O4—C13 1.299 (13) C9—C10 1.403 (13)
O4—C14 1.441 (12) C9—C13 1.494 (14)
N1—C1 1.302 (12) C10—C11 1.376 (13)
N1—C5 1.351 (15) C10—H10A 0.9300
N2—C8 1.327 (13) C11—C12 1.357 (13)
N2—C12 1.346 (14) C12—H12A 0.9300
C1—C2 1.400 (13) C14—H14A 0.9600
C2—C3 1.357 (13) C14—H14B 0.9600
C2—C6 1.471 (13) C14—H14C 0.9600
Br1···O3i 3.143 (9) Br2···O1ii 3.162 (9)
C6—O2—C7 119.8 (8) H7A—C7—H7C 109.5
C13—O4—C14 119.5 (9) H7B—C7—H7C 109.5
C1—N1—C5 117.0 (9) N2—C8—C9 125.6 (11)
C8—N2—C12 116.7 (9) N2—C8—Cl2 114.0 (8)
N1—C1—C2 125.8 (9) C9—C8—Cl2 120.4 (8)
N1—C1—Cl1 113.3 (8) C8—C9—C10 116.4 (9)
C2—C1—Cl1 120.9 (7) C8—C9—C13 126.8 (9)
C3—C2—C1 116.1 (8) C10—C9—C13 116.7 (8)
C3—C2—C6 118.3 (9) C11—C10—C9 118.6 (8)
C1—C2—C6 125.6 (9) C11—C10—H10A 120.7
C2—C3—C4 120.0 (9) C9—C10—H10A 120.7
C2—C3—H3A 120.0 C12—C11—C10 120.1 (9)
C4—C3—H3A 120.0 C12—C11—Br2 121.1 (7)
C5—C4—C3 119.2 (10) C10—C11—Br2 118.8 (7)
C5—C4—Br1 121.0 (8) N2—C12—C11 122.5 (9)
C3—C4—Br1 119.8 (7) N2—C12—H12A 118.8
N1—C5—C4 122.0 (10) C11—C12—H12A 118.8
N1—C5—H5A 119.0 O3—C13—O4 124.2 (9)
C4—C5—H5A 119.0 O3—C13—C9 121.9 (9)
O1—C6—O2 123.3 (9) O4—C13—C9 114.0 (8)
O1—C6—C2 121.6 (9) O4—C14—H14A 109.5
O2—C6—C2 115.0 (8) O4—C14—H14B 109.5
O2—C7—H7A 109.5 H14A—C14—H14B 109.5
O2—C7—H7B 109.5 O4—C14—H14C 109.5
H7A—C7—H7B 109.5 H14A—C14—H14C 109.5
O2—C7—H7C 109.5 H14B—C14—H14C 109.5
C5—N1—C1—C2 1.3 (16) C12—N2—C8—C9 −0.8 (17)
C5—N1—C1—Cl1 178.3 (8) C12—N2—C8—Cl2 −177.4 (8)
N1—C1—C2—C3 0.5 (16) N2—C8—C9—C10 −2.7 (16)
Cl1—C1—C2—C3 −176.3 (7) Cl2—C8—C9—C10 173.7 (8)
N1—C1—C2—C6 179.1 (9) N2—C8—C9—C13 −179.3 (11)
Cl1—C1—C2—C6 2.4 (15) Cl2—C8—C9—C13 −3.0 (15)
C1—C2—C3—C4 −1.0 (14) C8—C9—C10—C11 4.3 (14)
C6—C2—C3—C4 −179.8 (10) C13—C9—C10—C11 −178.7 (9)
C2—C3—C4—C5 −0.1 (15) C9—C10—C11—C12 −2.6 (15)
C2—C3—C4—Br1 178.4 (8) C9—C10—C11—Br2 179.2 (8)
C1—N1—C5—C4 −2.5 (16) C8—N2—C12—C11 2.8 (16)
C3—C4—C5—N1 2.0 (16) C10—C11—C12—N2 −1.1 (16)
Br1—C4—C5—N1 −176.5 (8) Br2—C11—C12—N2 177.1 (9)
C7—O2—C6—O1 2.9 (18) C14—O4—C13—O3 −3.9 (17)
C7—O2—C6—C2 179.6 (10) C14—O4—C13—C9 175.8 (10)
C3—C2—C6—O1 43.6 (16) C8—C9—C13—O3 133.7 (12)
C1—C2—C6—O1 −135.1 (12) C10—C9—C13—O3 −42.9 (15)
C3—C2—C6—O2 −133.2 (10) C8—C9—C13—O4 −46.0 (15)
C1—C2—C6—O2 48.2 (15) C10—C9—C13—O4 137.4 (10)

Symmetry codes: (i) x−1, y−1, z+1; (ii) x−1, y, z−1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV2402).

References

  1. Bruker (2001). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Colarusso, S. & Narjes, F. (2004). World Patent WO 04 110 442.
  3. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  4. Kim, Y., Close, J., Duggan, M. E., Hanney, B., Meissner, R. S., Musselman, J., Perkins, J. J. & Wang, J. B. (2006). World Patent WO 06 060 108.
  5. McArdle, J. V., de Laubenfels, E., Shorter, A. L. & Ammon, H. L. (1982). Polyhedron, 1, 471–474.
  6. Sheldrick, G. M. (2004). SADABS University of Göttingen, Germany.
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808013305/cv2402sup1.cif

e-64-o1072-sup1.cif (17.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808013305/cv2402Isup2.hkl

e-64-o1072-Isup2.hkl (89.5KB, hkl)

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


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