Abstract
In the title compound, C8H9ClN2O, the dihedral angle between the benzene ring and the methylamide substituent is 68.39 (11)°. In the crystal, molecules are linked by N—H⋯O hydrogen bonds, forming layers parallel to the ab plane.
Related literature
For background information on substituted anthranilamides, see: Bharate et al. (2013 ▶); Gnamm et al. (2012 ▶); Lahm et al. (2005 ▶); Norman et al. (1996 ▶); Roe et al. (1999 ▶). For the synthesis, see: Witt & Bergman (2000 ▶); Coppola (1980 ▶).
Experimental
Crystal data
C8H9ClN2O
M r = 184.62
Orthorhombic,
a = 9.2709 (19) Å
b = 11.812 (2) Å
c = 15.982 (3) Å
V = 1750.2 (6) Å3
Z = 8
Mo Kα radiation
μ = 0.39 mm−1
T = 173 K
0.43 × 0.25 × 0.18 mm
Data collection
Rigaku MM007-HF CCD (Saturn 724+) diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2007 ▶) T min = 0.609, T max = 1.000
3865 measured reflections
1528 independent reflections
1351 reflections with I > 2σ(I)
R int = 0.042
Refinement
R[F 2 > 2σ(F 2)] = 0.065
wR(F 2) = 0.139
S = 1.17
1528 reflections
110 parameters
H-atom parameters constrained
Δρmax = 0.26 e Å−3
Δρmin = −0.26 e Å−3
Data collection: CrystalClear (Rigaku, 2007 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536813027827/rz5085sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813027827/rz5085Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813027827/rz5085Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1B⋯O1i | 0.86 | 2.11 | 2.970 (3) | 175 |
| N2—H2⋯O1ii | 0.86 | 2.04 | 2.895 (4) | 172 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported by the National Natural Science Foundation of China (Nos. 31101448 and 31321004), the National Basic Research Program of China (2014CB932201 and 2012CB114104), the Public Service Sector R & D Project (200903033), the Open Fund of SKLBPI (SKL2012IP06), the National Key Technologies R & D Program of China (2011BAE06B03) and the Special Fund for Agro-Scientific Research in the Public Interest (No. 201003025) of the Chinese government.
supplementary crystallographic information
1. Comment
Anthranilamide-based derivatives exhibit interesting biological activities such as antibacterial, antifungal, antiviral, antimalarial and insecticidal activities (Bharate et al., 2013; Gnamm et al., 2012; Lahm et al., 2005; Norman et al., 1996; Roe et al., 1999). We report here the crystal structure of the title compound, 2-amino-6-chloro-N-methylbenzamide, an important organic intermediate in the synthesis of medicines, agricultural chemicals and animal drugs.
In the title compound (Fig. 1) the dihedral angle formed by the benzene ring and the methylamide substituent (r.m.s. deviation 0.0065 Å) is 68.39 (11)°. In the crystal structure, molecules are connected via N—H···O hydrogen bonds (Table 1) into layers running parallel to the ab plane.
2. Experimental
The title compound was prepared according to the literature method (Witt & Bergman, 2000) by stirring isatoic anhydride with aqueous methylamine. Isatoic anhydride was prepared by reaction of anthranilic acid with triphosgene in good yield (Coppola, 1980). The title compound (0.2 g) was dissolved in ethanol (50 ml) at room temperature. Colourless blocks were obtained through slow evaporation after two weeks.
3. Refinement
All H atoms were placed at calculated positions, with C—H = 0.93–0.98 Å, N—H = 0.86 Å, and refined as riding with Uiso(H) = 1.2Ueq(C, N) or 1.5Ueq(C) for methyl H atoms.
Figures
Fig. 1.
The molecular structure of the title compound showing 50% probability displacement ellipsoids.
Crystal data
| C8H9ClN2O | F(000) = 768 |
| Mr = 184.62 | Dx = 1.401 Mg m−3 |
| Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ac 2ab | Cell parameters from 3698 reflections |
| a = 9.2709 (19) Å | θ = 1.3–27.5° |
| b = 11.812 (2) Å | µ = 0.39 mm−1 |
| c = 15.982 (3) Å | T = 173 K |
| V = 1750.2 (6) Å3 | Block, colourless |
| Z = 8 | 0.43 × 0.25 × 0.18 mm |
Data collection
| Rigaku MM007-HF CCD (Saturn 724+) diffractometer | 1528 independent reflections |
| Radiation source: fine-focus sealed tube | 1351 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.042 |
| Detector resolution: 28.5714 pixels mm-1 | θmax = 25.0°, θmin = 2.6° |
| ω scans at fixed χ = 45° | h = −11→7 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2007) | k = −14→9 |
| Tmin = 0.609, Tmax = 1.000 | l = −10→19 |
| 3865 measured reflections |
Refinement
| 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)] = 0.065 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.139 | H-atom parameters constrained |
| S = 1.17 | w = 1/[σ2(Fo2) + (0.0417P)2 + 1.8852P] where P = (Fo2 + 2Fc2)/3 |
| 1528 reflections | (Δ/σ)max < 0.001 |
| 110 parameters | Δρmax = 0.26 e Å−3 |
| 0 restraints | Δρmin = −0.26 e Å−3 |
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 | ||
| Cl1 | 0.16414 (9) | 0.67224 (7) | 0.15558 (6) | 0.0435 (3) | |
| O1 | −0.2070 (2) | 0.70451 (18) | 0.04718 (16) | 0.0403 (6) | |
| C2 | −0.0247 (3) | 0.8296 (2) | 0.0969 (2) | 0.0298 (8) | |
| N1 | −0.1950 (3) | 0.9652 (2) | 0.0421 (2) | 0.0435 (8) | |
| H1A | −0.2129 | 0.9255 | −0.0017 | 0.052* | |
| H1B | −0.2227 | 1.0347 | 0.0402 | 0.052* | |
| C4 | −0.0826 (3) | 0.7415 (2) | 0.0382 (2) | 0.0302 (7) | |
| N2 | 0.0030 (3) | 0.7101 (2) | −0.02413 (17) | 0.0352 (7) | |
| H2 | 0.0870 | 0.7405 | −0.0280 | 0.042* | |
| C6 | 0.0854 (3) | 0.8068 (3) | 0.1541 (2) | 0.0332 (8) | |
| C7 | −0.0872 (3) | 0.9385 (3) | 0.0972 (2) | 0.0353 (8) | |
| C8 | −0.0390 (4) | 1.0177 (3) | 0.1558 (2) | 0.0398 (9) | |
| H8 | −0.0809 | 1.0911 | 0.1568 | 0.048* | |
| C9 | 0.1338 (4) | 0.8853 (3) | 0.2115 (2) | 0.0413 (9) | |
| H9 | 0.2095 | 0.8675 | 0.2493 | 0.050* | |
| C10 | 0.0685 (4) | 0.9910 (3) | 0.2123 (2) | 0.0443 (9) | |
| H10 | 0.0982 | 1.0458 | 0.2522 | 0.053* | |
| C11 | −0.0395 (4) | 0.6261 (3) | −0.0866 (3) | 0.0498 (10) | |
| H11C | −0.0103 | 0.6522 | −0.1423 | 0.075* | |
| H11B | −0.1443 | 0.6160 | −0.0851 | 0.075* | |
| H11A | 0.0079 | 0.5538 | −0.0742 | 0.075* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0438 (5) | 0.0390 (5) | 0.0476 (6) | 0.0069 (4) | −0.0035 (4) | 0.0071 (4) |
| O1 | 0.0297 (12) | 0.0267 (12) | 0.0646 (18) | −0.0043 (10) | 0.0029 (11) | −0.0057 (12) |
| C2 | 0.0266 (15) | 0.0251 (15) | 0.038 (2) | −0.0052 (13) | 0.0062 (14) | 0.0020 (14) |
| N1 | 0.0440 (16) | 0.0248 (14) | 0.062 (2) | 0.0047 (13) | −0.0059 (15) | −0.0056 (14) |
| C4 | 0.0281 (15) | 0.0200 (14) | 0.042 (2) | 0.0012 (13) | −0.0025 (15) | 0.0036 (14) |
| N2 | 0.0309 (13) | 0.0341 (14) | 0.0405 (17) | −0.0032 (12) | 0.0040 (13) | −0.0069 (13) |
| C6 | 0.0306 (16) | 0.0300 (17) | 0.039 (2) | −0.0008 (14) | 0.0073 (15) | 0.0012 (15) |
| C7 | 0.0326 (16) | 0.0270 (16) | 0.046 (2) | −0.0029 (14) | 0.0076 (16) | −0.0019 (15) |
| C8 | 0.048 (2) | 0.0262 (17) | 0.046 (2) | −0.0076 (16) | 0.0130 (18) | −0.0030 (16) |
| C9 | 0.0365 (18) | 0.051 (2) | 0.036 (2) | −0.0082 (18) | 0.0047 (16) | −0.0041 (18) |
| C10 | 0.0447 (19) | 0.045 (2) | 0.043 (2) | −0.0132 (18) | 0.0148 (18) | −0.0141 (18) |
| C11 | 0.042 (2) | 0.052 (2) | 0.056 (3) | 0.0000 (18) | −0.0020 (19) | −0.021 (2) |
Geometric parameters (Å, º)
| Cl1—C6 | 1.749 (3) | C6—C9 | 1.379 (5) |
| O1—C4 | 1.242 (3) | C7—C8 | 1.397 (5) |
| C2—C6 | 1.395 (4) | C8—C10 | 1.381 (5) |
| C2—C7 | 1.411 (4) | C8—H8 | 0.9500 |
| C2—C4 | 1.501 (4) | C9—C10 | 1.388 (5) |
| N1—C7 | 1.369 (4) | C9—H9 | 0.9500 |
| N1—H1A | 0.8601 | C10—H10 | 0.9500 |
| N1—H1B | 0.8600 | C11—H11C | 0.9800 |
| C4—N2 | 1.326 (4) | C11—H11B | 0.9800 |
| N2—C11 | 1.461 (4) | C11—H11A | 0.9800 |
| N2—H2 | 0.8600 | ||
| C6—C2—C7 | 118.4 (3) | C8—C7—C2 | 118.7 (3) |
| C6—C2—C4 | 122.5 (3) | C10—C8—C7 | 121.1 (3) |
| C7—C2—C4 | 119.1 (3) | C10—C8—H8 | 119.4 |
| C7—N1—H1A | 122.6 | C7—C8—H8 | 119.4 |
| C7—N1—H1B | 117.4 | C6—C9—C10 | 118.0 (3) |
| H1A—N1—H1B | 115.8 | C6—C9—H9 | 121.0 |
| O1—C4—N2 | 123.0 (3) | C10—C9—H9 | 121.0 |
| O1—C4—C2 | 120.2 (3) | C8—C10—C9 | 120.9 (3) |
| N2—C4—C2 | 116.7 (3) | C8—C10—H10 | 119.5 |
| C4—N2—C11 | 122.8 (3) | C9—C10—H10 | 119.5 |
| C4—N2—H2 | 118.6 | N2—C11—H11C | 109.5 |
| C11—N2—H2 | 118.6 | N2—C11—H11B | 109.5 |
| C9—C6—C2 | 122.9 (3) | H11C—C11—H11B | 109.5 |
| C9—C6—Cl1 | 117.7 (3) | N2—C11—H11A | 109.5 |
| C2—C6—Cl1 | 119.3 (2) | H11C—C11—H11A | 109.5 |
| N1—C7—C8 | 120.7 (3) | H11B—C11—H11A | 109.5 |
| N1—C7—C2 | 120.6 (3) | ||
| C6—C2—C4—O1 | 111.3 (4) | C6—C2—C7—N1 | 179.7 (3) |
| C7—C2—C4—O1 | −66.0 (4) | C4—C2—C7—N1 | −2.8 (5) |
| C6—C2—C4—N2 | −71.3 (4) | C6—C2—C7—C8 | −1.6 (5) |
| C7—C2—C4—N2 | 111.3 (3) | C4—C2—C7—C8 | 175.9 (3) |
| O1—C4—N2—C11 | −2.1 (5) | N1—C7—C8—C10 | 179.2 (3) |
| C2—C4—N2—C11 | −179.4 (3) | C2—C7—C8—C10 | 0.5 (5) |
| C7—C2—C6—C9 | 1.1 (5) | C2—C6—C9—C10 | 0.5 (5) |
| C4—C2—C6—C9 | −176.3 (3) | Cl1—C6—C9—C10 | −178.0 (3) |
| C7—C2—C6—Cl1 | 179.6 (2) | C7—C8—C10—C9 | 1.2 (5) |
| C4—C2—C6—Cl1 | 2.2 (4) | C6—C9—C10—C8 | −1.7 (5) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1B···O1i | 0.86 | 2.11 | 2.970 (3) | 175 |
| N2—H2···O1ii | 0.86 | 2.04 | 2.895 (4) | 172 |
Symmetry codes: (i) −x−1/2, y+1/2, z; (ii) x+1/2, −y+3/2, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ5085).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536813027827/rz5085sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813027827/rz5085Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813027827/rz5085Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

