supplementary materials


Acta Cryst. (2009). E65, o2144    [ doi:10.1107/S1600536809031511 ]

2-Chlorobenzenesulfonamide

B. T. Gowda, S. Foro, K. Shakuntala and H. Fuess

Abstract top

In the crystal of the title compound, C6H6ClNO2S, N-H...O hydrogen bonds pack the molecules into sheets parallel to the ac plane.

Comment top

The chemistry of sulfonamides is of interest as they show distinct physical, chemical and biological properties. Many arylsulfonamides and their N-halo compounds exhibit pharmacological, fungicidal and herbicidal activities due to their oxidizing action in aqueous, partial aqueous and non-aqueous media. In the present work, the structure of 2-chlorobenzenesulfonamde has been determined to explore the substituent effects on the solid state structures of sulfonamides and N-halo arylsulfonamides (Gowda et al., 2003; Gowda, Babitha et al. 2007; Gowda, Nayak et al. 2007; Gowda, Srilatha et al. 2007). The structure of the title compound (Fig. 1) closely resembles those of the parent benzenesulfonamide (Gowda, Nayak et al., 2007) and other aryl sulfonamides (Gowda, Babitha et al., 2007; Gowda, Srilatha et al., 2007; Jones & Weinkauf, 1993; Kumar et al., 1992; O'Connor & Maslen, 1965). The title compound crystallizes in monoclinic space group Cc in contrast to the monoclinic Pc space group observed with the parent sulfonamide (Gowda et al., 2007b) and orthorhombic Pbca space group with 4-fluorobenzenesulfonamide (Jones & Weinkauf, 1993) and 4-aminobenzenesulfonamide (O'Connor & Maslen, 1965) and monoclinic P21/n space group with 4-chlorobenzenesulfonamide and 4-bromobenzenesulfonamide (Gowda et al., 2003), and 4-methylbenzenesulfonamide (Kumar et al., 1992). The molecules in the title compound are packed into infinite 3-D molecular network through N1—H11···O1 and N1—H12···O2 hydrogen bonding (Table 1 & Fig.2).

Related literature top

For our studies of the effect of substituents on the solid state structures of sulfonamides and N-halo arylsulfonamides, see: Gowda et al. (2003); Gowda, Babitha et al. (2007); Gowda, Nayak et al. (2007); Gowda, Srilatha et al. (2007). For the parent benzenesulfonamide, see: Gowda, Nayak et al. (2007). For other aryl sulfonamides, see: Gowda, Babitha et al. (2007); Gowda, Srilatha et al. (2007); Jones & Weinkauf (1993); Kumar et al. (1992); O'Connor & Maslen (1965).

Experimental top

The purity of the commmercial sample (TCI, Tokyo) was checked and characterized by its infrared spectra. The single crystals used in X-ray diffraction studies were grown in ethanol solution by a slow evaporation of the solvent at room temperature.

Refinement top

The H atoms of the NH2 group were located in difference map and refined with restrained geometry to 0.86 (2) Å. The other H atoms were positioned with idealized geometry using a riding model [C—H = 0.93 Å]. All H atoms were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2009); cell refinement: CrysAlis RED (Oxford Diffraction, 2009); data reduction: CrysAlis RED (Oxford Diffraction, 2009); 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 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Molecular structure of (I), showing the atom labelling scheme and displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. Molecular packing of (I) with hydrogen bonding shown as dashed lines.
2-Chlorobenzenesulfonamide top
Crystal data top
C6H6ClNO2SF(000) = 392
Mr = 191.63Dx = 1.591 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2ycCell parameters from 1188 reflections
a = 6.955 (1) Åθ = 2.6–27.8°
b = 14.848 (3) ŵ = 0.68 mm1
c = 7.751 (1) ÅT = 299 K
β = 91.51 (1)°Prism, colourless
V = 800.2 (2) Å30.48 × 0.48 × 0.26 mm
Z = 4
Data collection top
Oxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
1031 independent reflections
Radiation source: fine-focus sealed tube1004 reflections with I > 2σ(I)
graphiteRint = 0.008
Rotation method data acquisition using ω and phi scans.θmax = 26.4°, θmin = 2.7°
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2009)
h = 84
Tmin = 0.735, Tmax = 0.842k = 1815
1598 measured reflectionsl = 99
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.022H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.060 w = 1/[σ2(Fo2) + (0.0417P)2 + 0.2306P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.041
1031 reflectionsΔρmax = 0.14 e Å3
106 parametersΔρmin = 0.21 e Å3
4 restraintsAbsolute structure: Flack (1983), 215 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.04 (8)
Crystal data top
C6H6ClNO2SV = 800.2 (2) Å3
Mr = 191.63Z = 4
Monoclinic, CcMo Kα radiation
a = 6.955 (1) ŵ = 0.68 mm1
b = 14.848 (3) ÅT = 299 K
c = 7.751 (1) Å0.48 × 0.48 × 0.26 mm
β = 91.51 (1)°
Data collection top
Oxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
1031 independent reflections
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2009)
1004 reflections with I > 2σ(I)
Tmin = 0.735, Tmax = 0.842Rint = 0.008
1598 measured reflectionsθmax = 26.4°
Refinement top
R[F2 > 2σ(F2)] = 0.022H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.060Δρmax = 0.14 e Å3
S = 1.03Δρmin = 0.21 e Å3
1031 reflectionsAbsolute structure: Flack (1983), 215 Friedel pairs
106 parametersFlack parameter: 0.04 (8)
4 restraints
Special details top

Experimental. CrysAlis RED (Oxford Diffraction, 2009) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.

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) top
xyzUiso*/Ueq
Cl10.56409 (10)0.10747 (7)0.84733 (11)0.0700 (3)
S10.18379 (8)0.20974 (3)0.98884 (8)0.03276 (14)
O10.0067 (3)0.22742 (12)1.0448 (3)0.0486 (5)
O20.3434 (3)0.23916 (13)1.0939 (2)0.0535 (5)
N10.2010 (4)0.25747 (15)0.8048 (3)0.0396 (5)
H110.309 (3)0.251 (2)0.755 (4)0.048*
H120.105 (4)0.249 (2)0.740 (3)0.048*
C10.1995 (4)0.09052 (15)0.9649 (3)0.0335 (5)
C20.3626 (4)0.04740 (18)0.9082 (4)0.0443 (6)
C30.3663 (6)0.0459 (2)0.8966 (4)0.0588 (8)
H30.47550.07510.85820.071*
C40.2078 (7)0.0951 (2)0.9421 (4)0.0674 (10)
H40.21060.15760.93410.081*
C50.0464 (6)0.05329 (19)0.9990 (4)0.0590 (8)
H50.06000.08721.02920.071*
C60.0415 (4)0.04025 (18)1.0117 (4)0.0432 (6)
H60.06770.06891.05150.052*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0380 (4)0.0856 (6)0.0871 (6)0.0153 (4)0.0158 (4)0.0148 (5)
S10.0338 (3)0.0335 (2)0.0310 (2)0.0015 (3)0.00213 (18)0.0023 (2)
O10.0468 (11)0.0480 (9)0.0520 (11)0.0068 (9)0.0205 (9)0.0043 (9)
O20.0590 (14)0.0501 (11)0.0506 (11)0.0152 (10)0.0172 (10)0.0031 (9)
N10.0364 (11)0.0449 (11)0.0375 (11)0.0035 (10)0.0025 (8)0.0055 (9)
C10.0381 (12)0.0343 (10)0.0280 (11)0.0023 (11)0.0025 (9)0.0013 (8)
C20.0478 (16)0.0476 (13)0.0374 (13)0.0118 (13)0.0008 (12)0.0047 (11)
C30.078 (2)0.0498 (15)0.0485 (15)0.0276 (17)0.0026 (15)0.0016 (13)
C40.116 (3)0.0360 (14)0.0497 (18)0.0069 (19)0.0055 (19)0.0025 (12)
C50.079 (2)0.0399 (14)0.0574 (18)0.0158 (15)0.0058 (17)0.0052 (13)
C60.0445 (16)0.0412 (12)0.0436 (14)0.0049 (12)0.0026 (12)0.0022 (11)
Geometric parameters (Å, °) top
Cl1—C21.737 (3)C2—C31.389 (4)
S1—O11.429 (2)C3—C41.376 (5)
S1—O21.4275 (19)C3—H30.9300
S1—N11.600 (2)C4—C51.366 (5)
S1—C11.784 (2)C4—H40.9300
N1—H110.857 (19)C5—C61.393 (4)
N1—H120.835 (18)C5—H50.9300
C1—C61.385 (4)C6—H60.9300
C1—C21.384 (4)
O1—S1—O2118.92 (13)C3—C2—Cl1118.6 (2)
O1—S1—N1106.32 (13)C4—C3—C2119.8 (3)
O2—S1—N1107.32 (12)C4—C3—H3120.1
O1—S1—C1105.88 (12)C2—C3—H3120.1
O2—S1—C1108.31 (12)C5—C4—C3120.8 (3)
N1—S1—C1109.91 (11)C5—C4—H4119.6
S1—N1—H11116 (2)C3—C4—H4119.6
S1—N1—H12113 (2)C4—C5—C6119.8 (3)
H11—N1—H12114 (3)C4—C5—H5120.1
C6—C1—C2119.8 (2)C6—C5—H5120.1
C6—C1—S1117.2 (2)C1—C6—C5119.9 (3)
C2—C1—S1123.0 (2)C1—C6—H6120.1
C1—C2—C3119.9 (3)C5—C6—H6120.1
C1—C2—Cl1121.5 (2)
O1—S1—C1—C63.7 (2)S1—C1—C2—Cl12.5 (3)
O2—S1—C1—C6124.8 (2)C1—C2—C3—C40.2 (4)
N1—S1—C1—C6118.19 (19)Cl1—C2—C3—C4179.3 (2)
O1—S1—C1—C2178.5 (2)C2—C3—C4—C50.1 (4)
O2—S1—C1—C252.9 (2)C3—C4—C5—C60.1 (5)
N1—S1—C1—C264.0 (2)C2—C1—C6—C51.0 (4)
C6—C1—C2—C30.7 (4)S1—C1—C6—C5178.8 (2)
S1—C1—C2—C3178.4 (2)C4—C5—C6—C10.7 (4)
C6—C1—C2—Cl1179.77 (19)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H11···O1i0.86 (2)2.12 (2)2.908 (3)152 (3)
N1—H12···O2ii0.84 (2)2.12 (2)2.941 (3)166 (3)
Symmetry codes: (i) x+1/2, −y+1/2, z−1/2; (ii) x−1/2, −y+1/2, z−1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H11···O1i0.86 (2)2.12 (2)2.908 (3)152 (3)
N1—H12···O2ii0.84 (2)2.12 (2)2.941 (3)166 (3)
Symmetry codes: (i) x+1/2, −y+1/2, z−1/2; (ii) x−1/2, −y+1/2, z−1/2.
Acknowledgements top

BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for an extension of his research fellowship.

references
References top

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