organic compounds
Methyl 6-chloronicotinate
aState Key Laboratory of Biotherapy and Cancer Center, West China Hospital, West China Medical School, Sichuan University, Chengdu 610041, People's Republic of China, and bDepartment of Pharmaceutical and Bioengineering, School of Chemical Engineering, Sichuan University, Chengdu 610065, People's Republic of China
*Correspondence e-mail: liujie2011@scu.edu.cn
The molecule of the title compound, C7H6ClNO2, is almost planar, with a dihedral angle of 3.34 (14)° between the COOMe group and the aromatic ring. In the crystal, the molecules are arranged into (12) layers by C—H⋯N hydrogen bonds and there are π–π stacking interactions between the aromatic rings in adjacent layers [centroid–centroid distance 3.8721 (4) Å]
Related literature
For background to the synthesis of methyl 6-chloronicotinate, see: González et al. (2009); Rekha et al. (2009). For a related structure, see: Ma & Liu (2008).
Experimental
Crystal data
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Refinement
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Data collection: CrysAlis PRO (Agilent, 2011); cell CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: OLEX2.
Supporting information
10.1107/S1600536811053517/gk2439sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811053517/gk2439Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536811053517/gk2439Isup3.cml
The title compound was prepared by the following method. A mixture of 6-chloronicotinic acid (5.67 g, 0.036 mol), dimethyl carbonate (10.95 mL, 0.131 mol) and concentrated H2SO4 (2.72 mL, 0.049 mol) was refluxed for 17 h. Then aqueous NaHCO3 solution (8.6 g in 86 mL water) was added, extracted with dichloromethane (150 mL), dried (Na2SO4), filtered and evaporated under reduced pressure to afford the title compound. Crystals suitable for X-ray analysis were obtained by slow evaporation from dichloromethane solution at room temperature over a period of one week.
H atoms were positioned geometrically and refined using a riding model approximation, with d(C—H) = 0.93 - 0.96 Å, and Uiso(H) =1.2Ueq(C) or 1.5Ueq(methyl C).
Data collection: CrysAlis PRO (Agilent, 2011); cell
CrysAlis PRO (Agilent, 2011); data reduction: CrysAlis PRO (Agilent, 2011); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).C7H6ClNO2 | Z = 2 |
Mr = 171.58 | F(000) = 176 |
Triclinic, P1 | Dx = 1.525 Mg m−3 |
a = 3.8721 (4) Å | Mo Kα radiation, λ = 0.7107 Å |
b = 5.8068 (6) Å | Cell parameters from 741 reflections |
c = 17.3721 (18) Å | θ = 3.6–26.3° |
α = 95.563 (9)° | µ = 0.45 mm−1 |
β = 94.918 (8)° | T = 293 K |
γ = 104.657 (9)° | Block, colourless |
V = 373.64 (7) Å3 | 0.30 × 0.30 × 0.12 mm |
Oxford Diffraction Xcalibur E diffractometer | 1527 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 855 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
Detector resolution: 16.0874 pixels mm-1 | θmax = 26.4°, θmin = 3.6° |
ω scans | h = −4→4 |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | k = −7→7 |
Tmin = 0.037, Tmax = 1.000 | l = −21→21 |
3068 measured reflections |
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)] = 0.055 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.119 | H-atom parameters constrained |
S = 0.99 | w = 1/[σ2(Fo2) + (0.041P)2] where P = (Fo2 + 2Fc2)/3 |
1527 reflections | (Δ/σ)max < 0.001 |
101 parameters | Δρmax = 0.23 e Å−3 |
0 restraints | Δρmin = −0.18 e Å−3 |
C7H6ClNO2 | γ = 104.657 (9)° |
Mr = 171.58 | V = 373.64 (7) Å3 |
Triclinic, P1 | Z = 2 |
a = 3.8721 (4) Å | Mo Kα radiation |
b = 5.8068 (6) Å | µ = 0.45 mm−1 |
c = 17.3721 (18) Å | T = 293 K |
α = 95.563 (9)° | 0.30 × 0.30 × 0.12 mm |
β = 94.918 (8)° |
Oxford Diffraction Xcalibur E diffractometer | 1527 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | 855 reflections with I > 2σ(I) |
Tmin = 0.037, Tmax = 1.000 | Rint = 0.029 |
3068 measured reflections |
R[F2 > 2σ(F2)] = 0.055 | 0 restraints |
wR(F2) = 0.119 | H-atom parameters constrained |
S = 0.99 | Δρmax = 0.23 e Å−3 |
1527 reflections | Δρmin = −0.18 e Å−3 |
101 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 | 0.3480 (2) | 1.23478 (16) | 0.44450 (4) | 0.0710 (4) | |
O1 | 0.4875 (6) | 0.7116 (4) | 0.10003 (12) | 0.0728 (8) | |
O2 | 0.1351 (5) | 0.3994 (4) | 0.14496 (10) | 0.0521 (6) | |
N1 | 0.5039 (6) | 1.1467 (5) | 0.30475 (15) | 0.0529 (7) | |
C1 | 0.3350 (8) | 1.0448 (6) | 0.36075 (16) | 0.0452 (8) | |
C2 | 0.1561 (7) | 0.8050 (6) | 0.35567 (17) | 0.0480 (8) | |
H2 | 0.0435 | 0.7421 | 0.3971 | 0.058* | |
C3 | 0.1498 (7) | 0.6630 (6) | 0.28773 (15) | 0.0443 (8) | |
H3 | 0.0331 | 0.5003 | 0.2823 | 0.053* | |
C4 | 0.3182 (7) | 0.7630 (5) | 0.22726 (15) | 0.0399 (7) | |
C5 | 0.4935 (7) | 1.0035 (5) | 0.23934 (17) | 0.0484 (8) | |
H5 | 0.6125 | 1.0704 | 0.1993 | 0.058* | |
C6 | 0.3266 (8) | 0.6273 (6) | 0.15097 (18) | 0.0464 (8) | |
C7 | 0.1289 (8) | 0.2550 (6) | 0.07211 (16) | 0.0618 (10) | |
H7A | −0.0050 | 0.3080 | 0.0315 | 0.093* | |
H7B | 0.0171 | 0.0899 | 0.0765 | 0.093* | |
H7C | 0.3703 | 0.2710 | 0.0599 | 0.093* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0898 (7) | 0.0583 (7) | 0.0610 (6) | 0.0171 (5) | 0.0109 (5) | −0.0070 (5) |
O1 | 0.0875 (17) | 0.0632 (18) | 0.0575 (14) | −0.0044 (13) | 0.0288 (13) | 0.0043 (13) |
O2 | 0.0669 (14) | 0.0379 (14) | 0.0472 (12) | 0.0064 (11) | 0.0127 (10) | −0.0011 (10) |
N1 | 0.0611 (17) | 0.0362 (17) | 0.0564 (16) | 0.0033 (13) | 0.0081 (13) | 0.0050 (14) |
C1 | 0.0451 (18) | 0.043 (2) | 0.0472 (17) | 0.0109 (16) | 0.0029 (14) | 0.0064 (16) |
C2 | 0.0517 (19) | 0.044 (2) | 0.0505 (18) | 0.0091 (16) | 0.0165 (15) | 0.0146 (16) |
C3 | 0.0457 (17) | 0.0346 (19) | 0.0485 (17) | 0.0021 (14) | 0.0071 (14) | 0.0060 (15) |
C4 | 0.0394 (17) | 0.042 (2) | 0.0400 (16) | 0.0105 (15) | 0.0059 (13) | 0.0138 (14) |
C5 | 0.0509 (19) | 0.042 (2) | 0.0496 (17) | 0.0048 (16) | 0.0110 (14) | 0.0112 (16) |
C6 | 0.0450 (18) | 0.046 (2) | 0.0489 (18) | 0.0112 (16) | 0.0075 (15) | 0.0093 (17) |
C7 | 0.071 (2) | 0.054 (2) | 0.0551 (19) | 0.0092 (18) | 0.0116 (17) | −0.0019 (18) |
Cl1—C1 | 1.728 (3) | C3—H3 | 0.9300 |
O1—C6 | 1.198 (4) | C3—C4 | 1.382 (4) |
O2—C6 | 1.333 (4) | C4—C5 | 1.376 (4) |
O2—C7 | 1.444 (3) | C4—C6 | 1.482 (4) |
N1—C1 | 1.322 (4) | C5—H5 | 0.9300 |
N1—C5 | 1.333 (3) | C7—H7A | 0.9600 |
C1—C2 | 1.380 (4) | C7—H7B | 0.9600 |
C2—H2 | 0.9300 | C7—H7C | 0.9600 |
C2—C3 | 1.367 (4) | ||
C6—O2—C7 | 116.0 (2) | C5—C4—C6 | 118.1 (3) |
C1—N1—C5 | 116.2 (3) | N1—C5—C4 | 124.2 (3) |
N1—C1—Cl1 | 115.3 (2) | N1—C5—H5 | 117.9 |
N1—C1—C2 | 124.6 (3) | C4—C5—H5 | 117.9 |
C2—C1—Cl1 | 120.1 (2) | O1—C6—O2 | 123.3 (3) |
C1—C2—H2 | 121.1 | O1—C6—C4 | 124.1 (3) |
C3—C2—C1 | 117.8 (3) | O2—C6—C4 | 112.6 (3) |
C3—C2—H2 | 121.1 | O2—C7—H7A | 109.5 |
C2—C3—H3 | 120.2 | O2—C7—H7B | 109.5 |
C2—C3—C4 | 119.5 (3) | O2—C7—H7C | 109.5 |
C4—C3—H3 | 120.2 | H7A—C7—H7B | 109.5 |
C3—C4—C6 | 124.3 (3) | H7A—C7—H7C | 109.5 |
C5—C4—C3 | 117.7 (3) | H7B—C7—H7C | 109.5 |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···N1i | 0.93 | 2.59 | 3.440 (4) | 151 |
C5—H5···O1 | 0.93 | 2.49 | 2.812 (3) | 101 |
Symmetry code: (i) x−1, y−1, z. |
Experimental details
Crystal data | |
Chemical formula | C7H6ClNO2 |
Mr | 171.58 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 293 |
a, b, c (Å) | 3.8721 (4), 5.8068 (6), 17.3721 (18) |
α, β, γ (°) | 95.563 (9), 94.918 (8), 104.657 (9) |
V (Å3) | 373.64 (7) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.45 |
Crystal size (mm) | 0.30 × 0.30 × 0.12 |
Data collection | |
Diffractometer | Oxford Diffraction Xcalibur E diffractometer |
Absorption correction | Multi-scan (CrysAlis PRO; Agilent, 2011) |
Tmin, Tmax | 0.037, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3068, 1527, 855 |
Rint | 0.029 |
(sin θ/λ)max (Å−1) | 0.625 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.055, 0.119, 0.99 |
No. of reflections | 1527 |
No. of parameters | 101 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.23, −0.18 |
Computer programs: CrysAlis PRO (Agilent, 2011), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), OLEX2 (Dolomanov et al., 2009) and Mercury (Macrae et al., 2006), OLEX2 (Dolomanov et al., 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···N1i | 0.93 | 2.59 | 3.440 (4) | 151 |
Symmetry code: (i) x−1, y−1, z. |
Acknowledgements
We thank the Analytical and Testing Center of Sichuan University for the X-ray measurements.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The title compound is one of the key intermediates in our synthetic investigations of GPCR(G-protein coupled receptor) modulators. We have synthesized the title compound and here we report its crystal structure.
As shown in Fig.1, the molecule is nearly planar, the dihedral angle formed by the pyridine ring and the ester group (C6/C7/O1/O2) being 3.34 (14)°. Weak C—H···O and C—H···N hydrogen bonds are present in the crystal structure linking molecules into (1 -1 2) layers. There are also π-π stacking interactions between the aromatic rings in adjacent layers [centroid-centroid distance 3.8721 (4) Å].