Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807041025/bt2485sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807041025/bt2485Isup2.hkl |
CCDC reference: 660338
The title compound was prepared according to the literature method (Shilpa and 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 and Gowda, 2007). Single crystals of the title compound were obtained from an ethanolic solution and used for X-ray diffraction studied at room temperature.
The amino H atom was located in difference map and was freely refined. The other H atoms were positioned with idealized geometry using a riding model (C—H = 0.93–0.98 Å). All H atoms bonded to C were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).
In the present work, the structure of N-(3,4-dichlorophenyl)-2,2- dichloroacetamide (34DCPDCA) has been determined to study the substituent effects on the structures of N-aromatic amides (Gowda et al., 2006; Gowda, Kozisek, Svoboda & Fuess, 2007; Gowda, Kožíšek, Tokarčík & Fuess, 2007). The conformation of the N—H bond in 34DCPDCA is syn to the 3-chloro substituent (Fig. 1), compared to the anti conformation observed in the chain unsubstituted N-(3,4-dichlorophenyl)- acetamide (34DCPA)(Jones et al., 1990), N-(3-chlorophenyl)- 2,2-dichloroacetamide (3CPDCA)(Gowda et al., 2006) and N-(3,4-dichlorophenyl)-2,2,2-trichloroacetamide (34DCPTCA)(Gowda, Kožíšek, Tokarčík & Fuess, 2007). The bond parameters in 34DCPDCA are similar to those in 34DCPA, 3CPDCA, 34DCPTCA and other acetanilides (Gowda et al., 2006; Gowda, Kozisek, Svoboda & Fuess, 2007; Gowda, Kožíšek, Tokarčík & Fuess, 2007). The molecules in 34DCPDCA are linked into chains via N—H···O hydrogen bonding (Fig.2).
For related literature, see: Gowda et al. (2006); Gowda, Kozisek, Svoboda & Fuess, (2007); Gowda, Kožíšek, Tokarčík & Fuess (2007); Jones et al. (1990); Shilpa & Gowda (2007).
Data collection: CAD-4-PC (Enraf–Nonius, 1996); cell refinement: CAD-4-PC (Enraf–Nonius, 1996); data reduction: REDU4 (Stoe & Cie, 1987); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).
C8H5Cl4NO | F(000) = 544 |
Mr = 272.93 | Dx = 1.721 Mg m−3 |
Monoclinic, P21/c | Cu Kα radiation, λ = 1.54180 Å |
Hall symbol: -P 2ybc | Cell parameters from 25 reflections |
a = 11.898 (5) Å | θ = 5.7–23.9° |
b = 10.310 (3) Å | µ = 9.93 mm−1 |
c = 9.212 (2) Å | T = 299 K |
β = 111.23 (3)° | Prism, colourless |
V = 1053.3 (6) Å3 | 0.25 × 0.23 × 0.20 mm |
Z = 4 |
Enraf–Nonius CAD-4 diffractometer | 1690 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.033 |
Graphite monochromator | θmax = 67.0°, θmin = 4.0° |
ω/2θ scans | h = −14→14 |
Absorption correction: ψ scan (North et al., 1968) | k = −12→0 |
Tmin = 0.120, Tmax = 0.138 | l = −10→4 |
2954 measured reflections | 3 standard reflections every 120 min |
1877 independent reflections | intensity decay: 1.0% |
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)] = 0.039 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.106 | w = 1/[σ2(Fo2) + (0.0454P)2 + 0.967P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max < 0.001 |
1877 reflections | Δρmax = 0.56 e Å−3 |
131 parameters | Δρmin = −0.37 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0037 (5) |
C8H5Cl4NO | V = 1053.3 (6) Å3 |
Mr = 272.93 | Z = 4 |
Monoclinic, P21/c | Cu Kα radiation |
a = 11.898 (5) Å | µ = 9.93 mm−1 |
b = 10.310 (3) Å | T = 299 K |
c = 9.212 (2) Å | 0.25 × 0.23 × 0.20 mm |
β = 111.23 (3)° |
Enraf–Nonius CAD-4 diffractometer | 1690 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.033 |
Tmin = 0.120, Tmax = 0.138 | 3 standard reflections every 120 min |
2954 measured reflections | intensity decay: 1.0% |
1877 independent reflections |
R[F2 > 2σ(F2)] = 0.039 | 0 restraints |
wR(F2) = 0.106 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.07 | Δρmax = 0.56 e Å−3 |
1877 reflections | Δρmin = −0.37 e Å−3 |
131 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 | 0.3114 (2) | 0.6392 (2) | 0.1238 (3) | 0.0323 (5) | |
C2 | 0.3922 (2) | 0.6851 (3) | 0.0593 (3) | 0.0357 (5) | |
H2 | 0.3670 | 0.7446 | −0.0220 | 0.043* | |
C3 | 0.5100 (2) | 0.6426 (3) | 0.1154 (3) | 0.0388 (6) | |
C4 | 0.5474 (2) | 0.5531 (3) | 0.2341 (3) | 0.0441 (6) | |
C5 | 0.4653 (3) | 0.5052 (3) | 0.2945 (3) | 0.0467 (7) | |
H5 | 0.4901 | 0.4433 | 0.3732 | 0.056* | |
C6 | 0.3476 (2) | 0.5471 (3) | 0.2409 (3) | 0.0400 (6) | |
H6 | 0.2932 | 0.5140 | 0.2828 | 0.048* | |
C7 | 0.1198 (2) | 0.7060 (2) | 0.1425 (3) | 0.0330 (5) | |
C8 | 0.0002 (2) | 0.7693 (3) | 0.0475 (3) | 0.0403 (6) | |
H8 | 0.0030 | 0.8002 | −0.0517 | 0.048* | |
N1 | 0.19265 (18) | 0.6887 (2) | 0.0630 (2) | 0.0339 (5) | |
H1N | 0.174 (3) | 0.720 (3) | −0.020 (4) | 0.041* | |
O1 | 0.14306 (18) | 0.6745 (2) | 0.2774 (2) | 0.0470 (5) | |
Cl1 | 0.60911 (7) | 0.70548 (8) | 0.03597 (11) | 0.0602 (3) | |
Cl2 | 0.69516 (7) | 0.50195 (9) | 0.30933 (12) | 0.0738 (3) | |
Cl3 | −0.11360 (7) | 0.65230 (11) | 0.01221 (13) | 0.0785 (3) | |
Cl4 | −0.02442 (9) | 0.90102 (9) | 0.15321 (10) | 0.0679 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0321 (12) | 0.0373 (13) | 0.0287 (11) | −0.0023 (10) | 0.0124 (9) | −0.0040 (9) |
C2 | 0.0330 (13) | 0.0393 (13) | 0.0371 (12) | 0.0025 (10) | 0.0155 (10) | 0.0017 (10) |
C3 | 0.0327 (13) | 0.0401 (14) | 0.0477 (14) | −0.0009 (10) | 0.0195 (11) | −0.0059 (11) |
C4 | 0.0361 (13) | 0.0401 (14) | 0.0497 (15) | 0.0074 (11) | 0.0079 (11) | −0.0067 (12) |
C5 | 0.0548 (17) | 0.0397 (15) | 0.0413 (14) | 0.0073 (12) | 0.0122 (12) | 0.0047 (11) |
C6 | 0.0460 (14) | 0.0402 (14) | 0.0370 (13) | −0.0021 (11) | 0.0188 (11) | 0.0008 (11) |
C7 | 0.0309 (12) | 0.0394 (13) | 0.0315 (12) | −0.0074 (10) | 0.0146 (9) | −0.0060 (10) |
C8 | 0.0336 (13) | 0.0530 (16) | 0.0383 (13) | −0.0014 (11) | 0.0177 (11) | −0.0040 (11) |
N1 | 0.0290 (10) | 0.0485 (13) | 0.0258 (9) | −0.0016 (9) | 0.0120 (8) | 0.0026 (9) |
O1 | 0.0481 (11) | 0.0659 (13) | 0.0317 (9) | 0.0038 (9) | 0.0201 (8) | 0.0024 (8) |
Cl1 | 0.0420 (4) | 0.0638 (5) | 0.0887 (6) | 0.0026 (3) | 0.0403 (4) | 0.0032 (4) |
Cl2 | 0.0412 (4) | 0.0708 (6) | 0.0955 (7) | 0.0202 (4) | 0.0081 (4) | 0.0067 (5) |
Cl3 | 0.0354 (4) | 0.0872 (7) | 0.1111 (8) | −0.0204 (4) | 0.0241 (4) | −0.0139 (6) |
Cl4 | 0.0855 (6) | 0.0608 (5) | 0.0616 (5) | 0.0230 (4) | 0.0318 (4) | −0.0043 (4) |
C1—C6 | 1.384 (4) | C5—H5 | 0.9300 |
C1—C2 | 1.384 (4) | C6—H6 | 0.9300 |
C1—N1 | 1.413 (3) | C7—O1 | 1.215 (3) |
C2—C3 | 1.378 (4) | C7—N1 | 1.334 (3) |
C2—H2 | 0.9300 | C7—C8 | 1.521 (4) |
C3—C4 | 1.376 (4) | C8—Cl3 | 1.754 (3) |
C3—Cl1 | 1.723 (3) | C8—Cl4 | 1.756 (3) |
C4—C5 | 1.378 (4) | C8—H8 | 0.9800 |
C4—Cl2 | 1.723 (3) | N1—H1N | 0.78 (3) |
C5—C6 | 1.375 (4) | ||
C6—C1—C2 | 120.0 (2) | C5—C6—C1 | 119.0 (2) |
C6—C1—N1 | 122.8 (2) | C5—C6—H6 | 120.5 |
C2—C1—N1 | 117.2 (2) | C1—C6—H6 | 120.5 |
C3—C2—C1 | 120.1 (2) | O1—C7—N1 | 125.0 (2) |
C3—C2—H2 | 120.0 | O1—C7—C8 | 121.4 (2) |
C1—C2—H2 | 120.0 | N1—C7—C8 | 113.6 (2) |
C4—C3—C2 | 120.2 (2) | C7—C8—Cl3 | 108.0 (2) |
C4—C3—Cl1 | 121.1 (2) | C7—C8—Cl4 | 108.81 (17) |
C2—C3—Cl1 | 118.7 (2) | Cl3—C8—Cl4 | 111.21 (14) |
C3—C4—C5 | 119.3 (2) | C7—C8—H8 | 109.6 |
C3—C4—Cl2 | 120.9 (2) | Cl3—C8—H8 | 109.6 |
C5—C4—Cl2 | 119.8 (2) | Cl4—C8—H8 | 109.6 |
C6—C5—C4 | 121.4 (3) | C7—N1—C1 | 125.8 (2) |
C6—C5—H5 | 119.3 | C7—N1—H1N | 118 (2) |
C4—C5—H5 | 119.3 | C1—N1—H1N | 115 (2) |
C6—C1—C2—C3 | −2.3 (4) | C2—C1—C6—C5 | 1.8 (4) |
N1—C1—C2—C3 | 178.7 (2) | N1—C1—C6—C5 | −179.3 (2) |
C1—C2—C3—C4 | 0.9 (4) | O1—C7—C8—Cl3 | −69.7 (3) |
C1—C2—C3—Cl1 | −178.1 (2) | N1—C7—C8—Cl3 | 109.7 (2) |
C2—C3—C4—C5 | 0.9 (4) | O1—C7—C8—Cl4 | 51.1 (3) |
Cl1—C3—C4—C5 | 180.0 (2) | N1—C7—C8—Cl4 | −129.4 (2) |
C2—C3—C4—Cl2 | −178.3 (2) | O1—C7—N1—C1 | −4.4 (4) |
Cl1—C3—C4—Cl2 | 0.7 (3) | C8—C7—N1—C1 | 176.2 (2) |
C3—C4—C5—C6 | −1.4 (4) | C6—C1—N1—C7 | 32.8 (4) |
Cl2—C4—C5—C6 | 177.8 (2) | C2—C1—N1—C7 | −148.3 (3) |
C4—C5—C6—C1 | 0.0 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.78 (3) | 2.08 (3) | 2.852 (3) | 171 (3) |
Symmetry code: (i) x, −y+3/2, z−1/2. |
Experimental details
Crystal data | |
Chemical formula | C8H5Cl4NO |
Mr | 272.93 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 299 |
a, b, c (Å) | 11.898 (5), 10.310 (3), 9.212 (2) |
β (°) | 111.23 (3) |
V (Å3) | 1053.3 (6) |
Z | 4 |
Radiation type | Cu Kα |
µ (mm−1) | 9.93 |
Crystal size (mm) | 0.25 × 0.23 × 0.20 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.120, 0.138 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2954, 1877, 1690 |
Rint | 0.033 |
(sin θ/λ)max (Å−1) | 0.597 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.039, 0.106, 1.07 |
No. of reflections | 1877 |
No. of parameters | 131 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.56, −0.37 |
Computer programs: CAD-4-PC (Enraf–Nonius, 1996), REDU4 (Stoe & Cie, 1987), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.78 (3) | 2.08 (3) | 2.852 (3) | 171 (3) |
Symmetry code: (i) x, −y+3/2, z−1/2. |
In the present work, the structure of N-(3,4-dichlorophenyl)-2,2- dichloroacetamide (34DCPDCA) has been determined to study the substituent effects on the structures of N-aromatic amides (Gowda et al., 2006; Gowda, Kozisek, Svoboda & Fuess, 2007; Gowda, Kožíšek, Tokarčík & Fuess, 2007). The conformation of the N—H bond in 34DCPDCA is syn to the 3-chloro substituent (Fig. 1), compared to the anti conformation observed in the chain unsubstituted N-(3,4-dichlorophenyl)- acetamide (34DCPA)(Jones et al., 1990), N-(3-chlorophenyl)- 2,2-dichloroacetamide (3CPDCA)(Gowda et al., 2006) and N-(3,4-dichlorophenyl)-2,2,2-trichloroacetamide (34DCPTCA)(Gowda, Kožíšek, Tokarčík & Fuess, 2007). The bond parameters in 34DCPDCA are similar to those in 34DCPA, 3CPDCA, 34DCPTCA and other acetanilides (Gowda et al., 2006; Gowda, Kozisek, Svoboda & Fuess, 2007; Gowda, Kožíšek, Tokarčík & Fuess, 2007). The molecules in 34DCPDCA are linked into chains via N—H···O hydrogen bonding (Fig.2).