organic compounds
2-Chloro-N-(2,3-dichlorophenyl)acetamide
aDepartment of Chemistry, Mangalore University, Mangalagangotri 574 199, Mangalore, India, and bInstitute of Materials Science, Darmstadt University of Technology, Petersenstrasse 23, D-64287, Darmstadt, Germany
*Correspondence e-mail: gowdabt@yahoo.com
The conformation of the N—H bond in the title compound (23DCPCA), C8H6Cl3NO, is syn to both the 2- and 3-chloro substituents in the aromatic ring, similar to the 2-chloro substituent in 2-chloro-N-(2-chlorophenyl)acetamide (2CPCA), the 2- and 3-chloro substituents in N-(2,3-dichlorophenyl)acetamide (23DCPA) and in 2,2-dichloro-N-(2,3-dichlorophenyl)acetamide (23DCPDCA). The bond parameters in 23DCPCA are similar to those in 2-chloro-N-(phenyl)acetamide, 2CPCA, 23DCPA, 23DCPDCA and other acetanilides. The molecules in 23DCPCA are linked into chains through N—H⋯O hydrogen bonding.
Experimental
Crystal data
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Refinement
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Data collection: CAD-4-PC (Enraf–Nonius, 1996); cell CAD-4-PC; data reduction: REDU4 (Stoe & Cie, 1987); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536808000408/om2201sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808000408/om2201Isup2.hkl
The title compound was prepared according to the literature method (Shilpa & Gowda, 2007). The purity of the compound was checked by determining its melting point. It was characterized by recording its infrared and NMR spectra (Shilpa & Gowda, 2007). Single crystals of the title compound were obtained from an ethanolic solution and used for X-ray diffraction studies at room temperature.
The CH atoms were positioned with idealized geometry using a riding model with C—H = 0.93–0.97 Å. The NH atom was located in difference map with N—H = 0.85 (5) Å. Uiso(H) values were set equal to 1.2 Ueq of the parent atom.
The residual electron-density features are located in the region of Cl1. The highest peak and deepest hole are 1.04 and 0.80%A from Cl1, respectively.
Data collection: CAD-4-PC (Enraf–Nonius, 1996); cell
CAD-4-PC (Enraf–Nonius, 1996); data reduction: REDU4 (Stoe & Cie, 1987); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C8H6Cl3NO | F(000) = 480 |
Mr = 238.49 | Dx = 1.665 Mg m−3 |
Monoclinic, P21/n | Cu Kα radiation, λ = 1.54180 Å |
Hall symbol: -P 2yn | Cell parameters from 25 reflections |
a = 11.704 (3) Å | θ = 4.3–23.9° |
b = 4.712 (1) Å | µ = 8.38 mm−1 |
c = 17.503 (4) Å | T = 299 K |
β = 99.76 (2)° | Prism, colourless |
V = 951.3 (4) Å3 | 0.50 × 0.35 × 0.28 mm |
Z = 4 |
Enraf–Nonius CAD-4 diffractometer | 1625 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.036 |
Graphite monochromator | θmax = 66.9°, θmin = 4.2° |
ω/2θ scans | h = −13→1 |
Absorption correction: ψ scan (North et al., 1968) | k = −5→0 |
Tmin = 0.014, Tmax = 0.096 | l = −20→20 |
1832 measured reflections | 3 standard reflections every 120 min |
1692 independent reflections | intensity decay: 2.0% |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.080 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.231 | w = 1/[σ2(Fo2) + (0.181P)2 + 0.9328P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max = 0.025 |
1692 reflections | Δρmax = 0.87 e Å−3 |
122 parameters | Δρmin = −1.04 e Å−3 |
0 restraints | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.018 (3) |
C8H6Cl3NO | V = 951.3 (4) Å3 |
Mr = 238.49 | Z = 4 |
Monoclinic, P21/n | Cu Kα radiation |
a = 11.704 (3) Å | µ = 8.38 mm−1 |
b = 4.712 (1) Å | T = 299 K |
c = 17.503 (4) Å | 0.50 × 0.35 × 0.28 mm |
β = 99.76 (2)° |
Enraf–Nonius CAD-4 diffractometer | 1625 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.036 |
Tmin = 0.014, Tmax = 0.096 | 3 standard reflections every 120 min |
1832 measured reflections | intensity decay: 2.0% |
1692 independent reflections |
R[F2 > 2σ(F2)] = 0.080 | 0 restraints |
wR(F2) = 0.231 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.07 | Δρmax = 0.87 e Å−3 |
1692 reflections | Δρmin = −1.04 e Å−3 |
122 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 | ||
C1 | 0.4488 (3) | 0.5307 (7) | 0.36495 (19) | 0.0315 (8) | |
C2 | 0.4556 (3) | 0.4122 (7) | 0.2935 (2) | 0.0316 (8) | |
C3 | 0.5442 (3) | 0.4955 (9) | 0.2544 (2) | 0.0395 (9) | |
C4 | 0.6240 (4) | 0.6936 (10) | 0.2854 (3) | 0.0502 (11) | |
H4 | 0.6825 | 0.7486 | 0.2586 | 0.060* | |
C5 | 0.6172 (4) | 0.8099 (9) | 0.3558 (3) | 0.0502 (11) | |
H5 | 0.6714 | 0.9453 | 0.3768 | 0.060* | |
C6 | 0.5313 (3) | 0.7298 (9) | 0.3964 (2) | 0.0416 (9) | |
H6 | 0.5284 | 0.8089 | 0.4447 | 0.050* | |
C7 | 0.2947 (4) | 0.6252 (8) | 0.4390 (2) | 0.0376 (9) | |
C8 | 0.1935 (4) | 0.4823 (8) | 0.4667 (2) | 0.0430 (10) | |
H8A | 0.2178 | 0.2983 | 0.4884 | 0.052* | |
H8B | 0.1320 | 0.4519 | 0.4228 | 0.052* | |
N1 | 0.3582 (3) | 0.4477 (7) | 0.40382 (17) | 0.0347 (8) | |
H1N | 0.346 (4) | 0.271 (11) | 0.405 (3) | 0.042* | |
O1 | 0.3132 (3) | 0.8774 (6) | 0.4466 (2) | 0.0556 (9) | |
Cl1 | 0.35541 (7) | 0.16288 (19) | 0.25447 (5) | 0.0389 (5) | |
Cl2 | 0.55325 (12) | 0.3482 (3) | 0.16544 (7) | 0.0653 (6) | |
Cl3 | 0.14026 (11) | 0.6855 (3) | 0.53663 (7) | 0.0602 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0320 (17) | 0.0313 (17) | 0.0342 (16) | −0.0005 (13) | 0.0143 (13) | 0.0009 (13) |
C2 | 0.0245 (16) | 0.0345 (17) | 0.0383 (18) | −0.0019 (13) | 0.0126 (13) | 0.0041 (14) |
C3 | 0.0316 (17) | 0.050 (2) | 0.0428 (19) | 0.0012 (16) | 0.0234 (14) | 0.0043 (16) |
C4 | 0.034 (2) | 0.056 (2) | 0.067 (3) | −0.0074 (17) | 0.0248 (19) | 0.006 (2) |
C5 | 0.033 (2) | 0.049 (2) | 0.070 (3) | −0.0125 (17) | 0.0109 (19) | −0.0012 (19) |
C6 | 0.040 (2) | 0.045 (2) | 0.042 (2) | −0.0058 (16) | 0.0097 (16) | −0.0031 (16) |
C7 | 0.050 (2) | 0.0314 (18) | 0.0354 (18) | −0.0010 (15) | 0.0188 (16) | 0.0010 (14) |
C8 | 0.048 (2) | 0.040 (2) | 0.049 (2) | −0.0055 (16) | 0.0304 (17) | −0.0054 (16) |
N1 | 0.0431 (16) | 0.0293 (15) | 0.0376 (16) | −0.0022 (12) | 0.0236 (13) | −0.0005 (12) |
O1 | 0.074 (2) | 0.0305 (15) | 0.076 (2) | −0.0035 (13) | 0.0499 (18) | −0.0054 (13) |
Cl1 | 0.0360 (7) | 0.0433 (7) | 0.0411 (7) | −0.0057 (3) | 0.0170 (4) | −0.0078 (3) |
Cl2 | 0.0670 (9) | 0.0878 (10) | 0.0529 (8) | −0.0123 (6) | 0.0438 (6) | −0.0074 (5) |
Cl3 | 0.0646 (9) | 0.0640 (9) | 0.0639 (8) | −0.0105 (5) | 0.0454 (6) | −0.0179 (5) |
C1—C2 | 1.384 (5) | C5—H5 | 0.9300 |
C1—C6 | 1.391 (5) | C6—H6 | 0.9300 |
C1—N1 | 1.409 (4) | C7—O1 | 1.211 (5) |
C2—C3 | 1.392 (5) | C7—N1 | 1.337 (5) |
C2—Cl1 | 1.718 (3) | C7—C8 | 1.512 (5) |
C3—C4 | 1.366 (6) | C8—Cl3 | 1.750 (4) |
C3—Cl2 | 1.725 (4) | C8—H8A | 0.9700 |
C4—C5 | 1.363 (7) | C8—H8B | 0.9700 |
C4—H4 | 0.9300 | N1—H1N | 0.85 (5) |
C5—C6 | 1.379 (6) | ||
C2—C1—C6 | 119.2 (3) | C5—C6—C1 | 119.9 (4) |
C2—C1—N1 | 119.2 (3) | C5—C6—H6 | 120.0 |
C6—C1—N1 | 121.7 (3) | C1—C6—H6 | 120.0 |
C1—C2—C3 | 119.5 (3) | O1—C7—N1 | 124.2 (4) |
C1—C2—Cl1 | 119.7 (3) | O1—C7—C8 | 122.5 (4) |
C3—C2—Cl1 | 120.8 (3) | N1—C7—C8 | 113.3 (3) |
C4—C3—C2 | 120.9 (4) | C7—C8—Cl3 | 111.8 (3) |
C4—C3—Cl2 | 119.4 (3) | C7—C8—H8A | 109.3 |
C2—C3—Cl2 | 119.7 (3) | Cl3—C8—H8A | 109.3 |
C5—C4—C3 | 119.5 (4) | C7—C8—H8B | 109.3 |
C5—C4—H4 | 120.2 | Cl3—C8—H8B | 109.3 |
C3—C4—H4 | 120.2 | H8A—C8—H8B | 107.9 |
C4—C5—C6 | 121.0 (4) | C7—N1—C1 | 124.9 (3) |
C4—C5—H5 | 119.5 | C7—N1—H1N | 119 (3) |
C6—C5—H5 | 119.5 | C1—N1—H1N | 116 (3) |
C6—C1—C2—C3 | −0.3 (5) | C3—C4—C5—C6 | 0.2 (7) |
N1—C1—C2—C3 | 179.3 (3) | C4—C5—C6—C1 | −1.0 (7) |
C6—C1—C2—Cl1 | 179.3 (3) | C2—C1—C6—C5 | 1.0 (6) |
N1—C1—C2—Cl1 | −1.1 (5) | N1—C1—C6—C5 | −178.6 (4) |
C1—C2—C3—C4 | −0.4 (6) | O1—C7—C8—Cl3 | −20.3 (5) |
Cl1—C2—C3—C4 | −180.0 (3) | N1—C7—C8—Cl3 | 161.7 (3) |
C1—C2—C3—Cl2 | 179.9 (3) | O1—C7—N1—C1 | −5.7 (6) |
Cl1—C2—C3—Cl2 | 0.3 (5) | C8—C7—N1—C1 | 172.3 (3) |
C2—C3—C4—C5 | 0.4 (6) | C2—C1—N1—C7 | −135.6 (4) |
Cl2—C3—C4—C5 | −179.9 (3) | C6—C1—N1—C7 | 44.0 (5) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.85 (5) | 2.05 (5) | 2.862 (4) | 161 (4) |
Symmetry code: (i) x, y−1, z. |
Experimental details
Crystal data | |
Chemical formula | C8H6Cl3NO |
Mr | 238.49 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 299 |
a, b, c (Å) | 11.704 (3), 4.712 (1), 17.503 (4) |
β (°) | 99.76 (2) |
V (Å3) | 951.3 (4) |
Z | 4 |
Radiation type | Cu Kα |
µ (mm−1) | 8.38 |
Crystal size (mm) | 0.50 × 0.35 × 0.28 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 diffractometer |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.014, 0.096 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 1832, 1692, 1625 |
Rint | 0.036 |
(sin θ/λ)max (Å−1) | 0.596 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.080, 0.231, 1.07 |
No. of reflections | 1692 |
No. of parameters | 122 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.87, −1.04 |
Computer programs: CAD-4-PC (Enraf–Nonius, 1996), REDU4 (Stoe & Cie, 1987), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2003).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.85 (5) | 2.05 (5) | 2.862 (4) | 161 (4) |
Symmetry code: (i) x, y−1, z. |
Acknowledgements
BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for extensions of his research fellowship.
References
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In the present work, the structure of 2-chloro-N-(2,3-dichlorophenyl)- acetamide (23DCPCA) has been determined to study the effect of substituents on the structures of N-aromatic amides (Gowda et al., 2007a, b, c). The conformation of the N—H bond in 23DCPCA is syn to both the 2-chloro and 3-chloro substituent (Fig. 1), similar to that of 2-chloro substituent in 2-chloro-N-(2-chlorophenyl)acetamide (2CPCA)(Gowda et al., 2007b), 2- and 3-chloro substituents in N-(2,3-dichlorophenyl)-acetamide (23DCPA) (Gowda et al., 2007a) and in 2,2-dichloro-N-(2,3-dichlorophenyl)acetamide (23DCPDCA)(Gowda et al., 2007c). The bond parameters in 23DCPCA are similar to those in 2-chloro-N-(phenyl)acetamide, 2CPCA, 23DCPA, 23DCPDCA and other acetanilides (Gowda et al., 2007a, b, c). The molecules in the structure of 23DCPCA are stabilized through N—H···O hydrogen bonding (Table 1 and Fig.2).