Abstract
In the title compound, C9H10ClNO3S, the amide H atom is syn with respect to the ortho-methyl group in the benzene ring and the C—S—N—C torsion angle is −66.9 (2)°. An intramolecular N—H⋯Cl hydrogen bond occurs. The crystal structure features inversion-related dimers linked by pairs of N—H⋯O hydrogen bonds.
Related literature
For the sulfanilamide moiety in sulfonamide drugs, see; Maren (1976 ▶). For its ability to form hydrogen bonds in the solid state, see; Yang & Guillory (1972 ▶). For hydrogen-bonding preferences of sulfonamides, see; Adsmond & Grant (2001 ▶). For the effect of substituents on the crystal structures of sulfonoamides, see: Gowda et al. (2008a ▶,b
▶, 2010 ▶)
Experimental
Crystal data
C9H10ClNO3S
M r = 247.69
Triclinic,
a = 7.4439 (8) Å
b = 7.5195 (8) Å
c = 10.519 (1) Å
α = 93.64 (1)°
β = 109.72 (1)°
γ = 102.52 (1)°
V = 535.07 (10) Å3
Z = 2
Cu Kα radiation
μ = 4.90 mm−1
T = 299 K
0.50 × 0.40 × 0.18 mm
Data collection
Enraf–Nonius CAD-4 diffractometer
Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.193, T max = 0.473
3727 measured reflections
1891 independent reflections
1771 reflections with I > 2σ(I)
R int = 0.051
3 standard reflections every 120 min intensity decay: 0.5%
Refinement
R[F 2 > 2σ(F 2)] = 0.050
wR(F 2) = 0.137
S = 1.08
1891 reflections
141 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.52 e Å−3
Δρmin = −0.57 e Å−3
Data collection: CAD-4-PC (Enraf–Nonius, 1996 ▶); cell refinement: 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, 2009 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811003655/ds2090sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811003655/ds2090Isup2.hkl
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—H1N⋯O1i | 0.79 (2) | 2.32 (2) | 3.087 (3) | 166 (3) |
| N1—H1N⋯Cl1 | 0.79 (2) | 2.62 (3) | 2.978 (2) | 110 (2) |
Symmetry code: (i)
.
Acknowledgments
KS thanks the University Grants Commission, Government of India, New Delhi, for the award of a research fellowship under its faculty improvement program.
supplementary crystallographic information
Comment
The molecular structures of sulfonamide drugs contain the sulfanilamide moiety (Maren, 1976). The propensity for hydrogen bonding in the solid state, due to the presence of various hydrogen bond donors and acceptors can give rise to polymorphism (Yang & Guillory, 1972). The hydrogen bonding preferences of sulfonamides has also been investigated (Adsmond & Grant, 2001). The nature and position of substituents play a significant role on the crystal structures of N-(aryl)sulfonoamides (Gowda et al., 2008a,b, 2010). As a part of studying the substituent effects on the structures of this class of compounds, the structure of 2-chloro-N-(2-methylphenylsulfonyl)- acetamide (I) has been determined. The conformations of the N—H and C=O bonds of the SO2—NH—CO—C segment in the structure are anti to each other (Fig. 1), similar to that observed in N-(phenylsulfonyl)acetamide (II)(Gowda et al., 2010), N-(phenylsulfonyl)- 2,2-dichloroacetamide (III) (Gowda et al., 2008b) and N-(4-methylphenylsulfonyl)-2,2-dichloroacetamide (IV) (Gowda et al., 2008a).
The molecule in (I) is bent at the S-atom with a C1—S1—N1—C7 torsion angle of -67.0 (3)°, compared to the values of -58.8 (4)° in (II), -66.3 (3)° in (III) and -71.1 (2)° in (IV). Further, the dihedral angle between the benzene ring and the SO2—NH—CO—C group in (I) is 78.9 (1)°, compared to the values of 89.0 (2)° in (II), 79.8 (1)° in (III) and 81.0 (1)° in (IV),
The structure exhibits both the intramolecular N—H···Cl and the intermolecular N—H···O(S) hydrogen bonds.
In the crystal structure, the pairs of intermolecular N–H···O hydrogen bonds (Table 1) link the molecules through inversion-related dimers into zigzag chains running in the bc-plane. Part of the crystal structure is shown in Fig. 2.
Experimental
The title compound was prepared by refluxing 2-methylbenzenesulfonamide (0.10 mole) with an excess of chloroacetyl chloride (0.20 mole) for about an hour on a water bath. The reaction mixture was cooled and poured into ice cold water. The resulting solid was separated, washed thoroughly with water and dissolved in warm dilute sodium hydrogen carbonate solution. The title compound was reprecipitated by acidifying the filtered solution with glacial acetic acid. It was filtered, dried and recrystallized from ethanol. The purity of the compound was checked by determining its melting point. It was further characterized by recording its infrared spectra.
Prism like colorless single crystals of the title compound used in X-ray diffraction studies were obtained from a slow evaporation of an ethanolic solution of the compound.
Refinement
The H atom of the NH group was located in a difference map and later restrained to the distance N—H = 0.86 (3) Å. The other H atoms were positioned with idealized geometry using a riding model with C—H = 0.93–0.97 Å. All H atoms were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).
The Uij components of C3, C4 and C5 were restrained to approximate isotropic behavoir.
Figures
Fig. 1.
Molecular structure of the title compound, showing the atom- labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.
Molecular packing in the title compound. Hydrogen bonds are shown as dashed lines.
Crystal data
| C9H10ClNO3S | Z = 2 |
| Mr = 247.69 | F(000) = 256 |
| Triclinic, P1 | Dx = 1.537 Mg m−3 |
| Hall symbol: -P 1 | Cu Kα radiation, λ = 1.54180 Å |
| a = 7.4439 (8) Å | Cell parameters from 25 reflections |
| b = 7.5195 (8) Å | θ = 7.0–23.1° |
| c = 10.519 (1) Å | µ = 4.90 mm−1 |
| α = 93.64 (1)° | T = 299 K |
| β = 109.72 (1)° | Prism, colourless |
| γ = 102.52 (1)° | 0.50 × 0.40 × 0.18 mm |
| V = 535.07 (10) Å3 |
Data collection
| Enraf–Nonius CAD-4 diffractometer | 1771 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.051 |
| graphite | θmax = 66.9°, θmin = 4.5° |
| ω/2θ scans | h = −8→8 |
| Absorption correction: ψ scan (North et al., 1968) | k = −8→8 |
| Tmin = 0.193, Tmax = 0.473 | l = −12→12 |
| 3727 measured reflections | 3 standard reflections every 120 min |
| 1891 independent reflections | intensity decay: 0.5% |
Refinement
| 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)] = 0.050 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.137 | w = 1/[σ2(Fo2) + (0.0853P)2 + 0.2427P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.08 | (Δ/σ)max < 0.001 |
| 1891 reflections | Δρmax = 0.52 e Å−3 |
| 141 parameters | Δρmin = −0.57 e Å−3 |
| 1 restraint | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.028 (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 | ||
| C1 | 0.4813 (4) | 0.6426 (3) | 0.3198 (2) | 0.0356 (6) | |
| C2 | 0.6844 (5) | 0.7012 (3) | 0.3580 (3) | 0.0465 (7) | |
| C3 | 0.7891 (6) | 0.7927 (4) | 0.4905 (3) | 0.0674 (10) | |
| H3 | 0.9259 | 0.8321 | 0.5206 | 0.081* | |
| C4 | 0.6944 (8) | 0.8259 (5) | 0.5778 (3) | 0.0764 (13) | |
| H4 | 0.7682 | 0.8892 | 0.6653 | 0.092* | |
| C5 | 0.4938 (8) | 0.7680 (5) | 0.5388 (3) | 0.0754 (12) | |
| H5 | 0.4320 | 0.7916 | 0.5992 | 0.090* | |
| C6 | 0.3832 (6) | 0.6737 (4) | 0.4081 (3) | 0.0531 (8) | |
| H6 | 0.2468 | 0.6321 | 0.3800 | 0.064* | |
| C7 | 0.2227 (4) | 0.8123 (3) | 0.0563 (2) | 0.0336 (5) | |
| C8 | 0.1973 (4) | 0.9327 (3) | −0.0539 (3) | 0.0397 (6) | |
| H8A | 0.2593 | 1.0596 | −0.0110 | 0.048* | |
| H8B | 0.0574 | 0.9224 | −0.0984 | 0.048* | |
| C9 | 0.7974 (5) | 0.6716 (5) | 0.2685 (4) | 0.0622 (8) | |
| H9A | 0.7241 | 0.6847 | 0.1766 | 0.075* | |
| H9B | 0.8181 | 0.5500 | 0.2704 | 0.075* | |
| H9C | 0.9226 | 0.7610 | 0.3010 | 0.075* | |
| N1 | 0.3146 (3) | 0.6745 (3) | 0.05184 (19) | 0.0327 (5) | |
| H1N | 0.366 (4) | 0.660 (4) | −0.001 (3) | 0.039* | |
| O1 | 0.4251 (3) | 0.3986 (2) | 0.11017 (18) | 0.0450 (5) | |
| O2 | 0.1386 (3) | 0.4445 (3) | 0.1603 (2) | 0.0516 (5) | |
| O3 | 0.1615 (3) | 0.8425 (3) | 0.14615 (19) | 0.0504 (5) | |
| Cl1 | 0.29367 (12) | 0.88507 (9) | −0.18091 (7) | 0.0525 (3) | |
| S1 | 0.32891 (8) | 0.51904 (7) | 0.15752 (5) | 0.0320 (3) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0487 (16) | 0.0278 (10) | 0.0267 (11) | 0.0120 (10) | 0.0075 (10) | 0.0051 (8) |
| C2 | 0.0512 (18) | 0.0318 (12) | 0.0458 (14) | 0.0066 (11) | 0.0055 (12) | 0.0113 (10) |
| C3 | 0.076 (3) | 0.0459 (16) | 0.0511 (18) | 0.0051 (15) | −0.0078 (16) | 0.0068 (13) |
| C4 | 0.112 (4) | 0.0511 (18) | 0.0400 (17) | 0.017 (2) | −0.0020 (19) | −0.0004 (13) |
| C5 | 0.137 (4) | 0.070 (2) | 0.0381 (16) | 0.051 (2) | 0.039 (2) | 0.0132 (14) |
| C6 | 0.076 (2) | 0.0538 (16) | 0.0392 (14) | 0.0305 (15) | 0.0231 (14) | 0.0143 (11) |
| C7 | 0.0357 (13) | 0.0325 (11) | 0.0310 (11) | 0.0118 (9) | 0.0084 (9) | 0.0030 (8) |
| C8 | 0.0451 (16) | 0.0363 (12) | 0.0417 (13) | 0.0181 (11) | 0.0150 (11) | 0.0101 (10) |
| C9 | 0.0466 (19) | 0.0606 (18) | 0.076 (2) | 0.0087 (14) | 0.0209 (15) | 0.0130 (15) |
| N1 | 0.0407 (12) | 0.0335 (10) | 0.0287 (9) | 0.0161 (8) | 0.0141 (8) | 0.0063 (8) |
| O1 | 0.0661 (14) | 0.0323 (9) | 0.0412 (9) | 0.0231 (9) | 0.0185 (9) | 0.0057 (7) |
| O2 | 0.0432 (12) | 0.0498 (11) | 0.0537 (11) | −0.0001 (9) | 0.0134 (9) | 0.0151 (8) |
| O3 | 0.0648 (14) | 0.0597 (12) | 0.0438 (10) | 0.0355 (10) | 0.0277 (10) | 0.0130 (8) |
| Cl1 | 0.0744 (6) | 0.0547 (5) | 0.0462 (4) | 0.0325 (4) | 0.0314 (4) | 0.0216 (3) |
| S1 | 0.0384 (4) | 0.0259 (4) | 0.0298 (4) | 0.0087 (3) | 0.0093 (3) | 0.0049 (2) |
Geometric parameters (Å, °)
| C1—C2 | 1.386 (4) | C7—N1 | 1.367 (3) |
| C1—C6 | 1.398 (4) | C7—C8 | 1.502 (3) |
| C1—S1 | 1.760 (2) | C8—Cl1 | 1.768 (3) |
| C2—C3 | 1.392 (4) | C8—H8A | 0.9700 |
| C2—C9 | 1.494 (5) | C8—H8B | 0.9700 |
| C3—C4 | 1.374 (7) | C9—H9A | 0.9600 |
| C3—H3 | 0.9300 | C9—H9B | 0.9600 |
| C4—C5 | 1.367 (6) | C9—H9C | 0.9600 |
| C4—H4 | 0.9300 | N1—S1 | 1.6590 (19) |
| C5—C6 | 1.389 (5) | N1—H1N | 0.79 (2) |
| C5—H5 | 0.9300 | O1—S1 | 1.4303 (18) |
| C6—H6 | 0.9300 | O2—S1 | 1.417 (2) |
| C7—O3 | 1.208 (3) | ||
| C2—C1—C6 | 122.5 (2) | C7—C8—Cl1 | 116.35 (17) |
| C2—C1—S1 | 122.3 (2) | C7—C8—H8A | 108.2 |
| C6—C1—S1 | 115.3 (2) | Cl1—C8—H8A | 108.2 |
| C1—C2—C3 | 116.8 (3) | C7—C8—H8B | 108.2 |
| C1—C2—C9 | 124.9 (2) | Cl1—C8—H8B | 108.2 |
| C3—C2—C9 | 118.3 (3) | H8A—C8—H8B | 107.4 |
| C4—C3—C2 | 121.3 (4) | C2—C9—H9A | 109.5 |
| C4—C3—H3 | 119.4 | C2—C9—H9B | 109.5 |
| C2—C3—H3 | 119.4 | H9A—C9—H9B | 109.5 |
| C5—C4—C3 | 121.4 (3) | C2—C9—H9C | 109.5 |
| C5—C4—H4 | 119.3 | H9A—C9—H9C | 109.5 |
| C3—C4—H4 | 119.3 | H9B—C9—H9C | 109.5 |
| C4—C5—C6 | 119.4 (3) | C7—N1—S1 | 123.27 (17) |
| C4—C5—H5 | 120.3 | C7—N1—H1N | 124 (2) |
| C6—C5—H5 | 120.3 | S1—N1—H1N | 113 (2) |
| C5—C6—C1 | 118.7 (4) | O2—S1—O1 | 118.71 (12) |
| C5—C6—H6 | 120.7 | O2—S1—N1 | 108.92 (11) |
| C1—C6—H6 | 120.7 | O1—S1—N1 | 103.64 (10) |
| O3—C7—N1 | 122.6 (2) | O2—S1—C1 | 108.50 (12) |
| O3—C7—C8 | 118.3 (2) | O1—S1—C1 | 110.83 (12) |
| N1—C7—C8 | 119.1 (2) | N1—S1—C1 | 105.34 (10) |
| C6—C1—C2—C3 | 0.5 (4) | N1—C7—C8—Cl1 | −0.7 (3) |
| S1—C1—C2—C3 | −178.1 (2) | O3—C7—N1—S1 | 7.4 (4) |
| C6—C1—C2—C9 | 179.8 (3) | C8—C7—N1—S1 | −172.97 (18) |
| S1—C1—C2—C9 | 1.2 (4) | C7—N1—S1—O2 | 49.3 (2) |
| C1—C2—C3—C4 | −1.2 (4) | C7—N1—S1—O1 | 176.60 (19) |
| C9—C2—C3—C4 | 179.4 (3) | C7—N1—S1—C1 | −66.9 (2) |
| C2—C3—C4—C5 | 1.0 (5) | C2—C1—S1—O2 | 167.1 (2) |
| C3—C4—C5—C6 | 0.0 (5) | C6—C1—S1—O2 | −11.5 (2) |
| C4—C5—C6—C1 | −0.7 (5) | C2—C1—S1—O1 | 35.1 (2) |
| C2—C1—C6—C5 | 0.4 (4) | C6—C1—S1—O1 | −143.56 (19) |
| S1—C1—C6—C5 | 179.1 (2) | C2—C1—S1—N1 | −76.3 (2) |
| O3—C7—C8—Cl1 | 178.8 (2) | C6—C1—S1—N1 | 105.0 (2) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O1i | 0.79 (2) | 2.32 (2) | 3.087 (3) | 166 (3) |
| N1—H1N···Cl1 | 0.79 (2) | 2.62 (3) | 2.978 (2) | 110 (2) |
Symmetry codes: (i) −x+1, −y+1, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DS2090).
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 datablocks I, global. DOI: 10.1107/S1600536811003655/ds2090sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811003655/ds2090Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


