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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 14;67(Pt 6):o1401. doi: 10.1107/S160053681101717X

4-Chloro-N-(2,6-dimethyl­phen­yl)benzene­sulfonamide

K Shakuntala a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3120512  PMID: 21754786

Abstract

In the title compound, C14H14ClNO2S, the amido H atom orients itself away from both the ortho-methyl groups in the adjacent aromatic ring. The mol­ecule is twisted at the S atom with an C—SO2—NH—C torsion angle of −69.9 (2)°. The two aromatic rings are tilted relative to each other by 31.9 (1)°. In the crystal, the mol­ecules are packed into zigzag chains along the b axis via inter­molecular N—H⋯O hydrogen bonds.

Related literature

For hydrogen-bonding modes of sulfonamides, see; Adsmond & Grant (2001 ▶). For our study of the effect of substituents on the structures of N-(ar­yl)methane­sulfonamides, see: Gowda et al. (2007 ▶), on the structures of N-(ar­yl)aryl­sulfonamides, see: Gowda et al. (2008 ▶); Shakuntala et al. (2011 ▶) and on the oxidative strengths of N-chloro,N-aryl­sulfonamides, see: Gowda & Kumar (2003 ▶).graphic file with name e-67-o1401-scheme1.jpg

Experimental

Crystal data

  • C14H14ClNO2S

  • M r = 295.77

  • Orthorhombic, Inline graphic

  • a = 7.3816 (4) Å

  • b = 10.2916 (7) Å

  • c = 18.312 (1) Å

  • V = 1391.13 (14) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.42 mm−1

  • T = 293 K

  • 0.40 × 0.28 × 0.24 mm

Data collection

  • Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.850, T max = 0.906

  • 5356 measured reflections

  • 2767 independent reflections

  • 2255 reflections with I > 2σ(I)

  • R int = 0.022

Refinement

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.079

  • S = 1.02

  • 2767 reflections

  • 177 parameters

  • 1 restraint

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.25 e Å−3

  • Absolute structure: Flack (1983 ▶), 1113 Friedel pairs

  • Flack parameter: 0.43 (7)

Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2009 ▶); data reduction: CrysAlis RED; 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/S160053681101717X/bq2299sup1.cif

e-67-o1401-sup1.cif (17.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681101717X/bq2299Isup2.hkl

e-67-o1401-Isup2.hkl (135.9KB, hkl)

Supplementary material file. DOI: 10.1107/S160053681101717X/bq2299Isup3.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—H1N⋯O1i 0.82 (2) 2.28 (2) 3.083 (3) 166 (3)

Symmetry code: (i) Inline graphic.

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 sulfonamide moieties are the constituents of many biologically important compounds. The hydrogen bonding preferences of sulfonamides has been investigated (Adsmond & Grant, 2001). As a part of studying the substituent effects on the structures and other aspects of this class of compounds (Gowda et al., 2003, 2007, 2008; Shakuntala et al., 2011), in the present work, the crystal structure of 4-chloro-N-(2,6-dimethylphenyl)-benzenesulfonamide (I) has been determined (Fig.1). In the structure, the amido H atom orients itself away from both the ortho-methyl groups in the adjacent aromatic ring. The molecule is twisted at the S atom with the C—SO2—NH—C torsion angle of -69.9 (2)°, compared to the values of -53.8 (3)° (molecule 1) and -63.4 (3)° (molecule 2) in 4-chloro-N-(phenyl)-benzenesulfonamide (II) (Shakuntala et al., 2011) and -78.7 (2)° in N-(2,6-dimethylphenyl)-benzenesulfonamide (III) (Gowda et al., 2008)

The sulfonyl and anilino benzene rings in (I) are tilted relative to each other by 31.9 (1)°, compared to the values of 69.1 (1)° in molecule 1 and 82.6 (1)° in molecule 2 of (II), and 44.9 (1)° in (III).

The packing of molecules in (I) into zigzag chains through N—H···O(S) hydrogen bonding (Table 1) is shown in Fig.2.

Experimental

The solution of chlorobenzene (10 ml) in chloroform (40 ml) was treated dropwise with chlorosulfonic acid (25 ml) at 0 ° C. After the initial evolution of hydrogen chloride subsided, the reaction mixture was brought to room temperature and poured into crushed ice in a beaker. The chloroform layer was separated, washed with cold water and allowed to evaporate slowly. The residual 4-chlorobenzenesulfonylchloride was treated with 2,6-dimethylaniline in the stoichiometric ratio and boiled for ten minutes. The reaction mixture was then cooled to room temperature and added to ice cold water (100 ml). The resultant 4-chloro-N-(2,6-dimethylphenyl)-benzenesulfonamide was filtered under suction and washed thoroughly with cold water. It was then recrystallized to constant melting point from dilute ethanol. The compound was characterized by recording its infrared and NMR spectra.

Prism like colorless single crystals used in X-ray diffraction studies were grown in ethanolic solution by slow evaporation at room temperature.

Refinement

The H atom of the NH group was located in a difference map and later restrained to the distance N—H = 0.86 (2) Å. The other H atoms were positioned with idealized geometry using a riding model with the aromatic C—H = 0.93 Å and the methyl C—H = 0.96 Å. All H atoms were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).

Figures

Fig. 1.

Fig. 1.

Molecular structure of (I), showing the atom labelling scheme and displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Molecular packing of (I) with hydrogen bonding shown as dashed lines.

Crystal data

C14H14ClNO2S F(000) = 616
Mr = 295.77 Dx = 1.412 Mg m−3
Orthorhombic, P212121 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2ab Cell parameters from 1775 reflections
a = 7.3816 (4) Å θ = 2.8–28.0°
b = 10.2916 (7) Å µ = 0.42 mm−1
c = 18.312 (1) Å T = 293 K
V = 1391.13 (14) Å3 Prism, colourless
Z = 4 0.40 × 0.28 × 0.24 mm

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 2767 independent reflections
Radiation source: fine-focus sealed tube 2255 reflections with I > 2σ(I)
graphite Rint = 0.022
Rotation method data acquisition using ω and φ scans θmax = 26.4°, θmin = 3.0°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −9→6
Tmin = 0.850, Tmax = 0.906 k = −12→10
5356 measured reflections l = −22→17

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)] = 0.036 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.079 w = 1/[σ2(Fo2) + (0.0326P)2 + 0.3144P] where P = (Fo2 + 2Fc2)/3
S = 1.02 (Δ/σ)max < 0.001
2767 reflections Δρmax = 0.19 e Å−3
177 parameters Δρmin = −0.25 e Å−3
1 restraint Absolute structure: Flack (1983), 1113 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.43 (7)

Special details

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)

x y z Uiso*/Ueq
Cl1 0.42735 (14) 0.03948 (8) −0.04544 (5) 0.0851 (3)
S1 0.96404 (8) 0.20494 (6) 0.19969 (4) 0.04077 (16)
O1 0.9231 (3) 0.33512 (15) 0.22176 (9) 0.0502 (5)
O2 1.1425 (2) 0.1712 (2) 0.17729 (11) 0.0606 (6)
N1 0.9167 (3) 0.11125 (19) 0.26858 (12) 0.0389 (5)
H1N 0.950 (3) 0.0356 (17) 0.2645 (14) 0.047*
C1 0.8156 (3) 0.1660 (2) 0.12743 (13) 0.0375 (6)
C2 0.8780 (4) 0.0962 (2) 0.06798 (14) 0.0479 (7)
H2 1.0000 0.0745 0.0642 0.057*
C3 0.7573 (4) 0.0591 (3) 0.01437 (15) 0.0568 (8)
H3 0.7974 0.0119 −0.0258 0.068*
C4 0.5788 (4) 0.0917 (3) 0.02047 (14) 0.0513 (7)
C5 0.5165 (4) 0.1648 (3) 0.07828 (15) 0.0524 (7)
H5 0.3949 0.1880 0.0811 0.063*
C6 0.6357 (3) 0.2032 (3) 0.13178 (14) 0.0450 (6)
H6 0.5958 0.2539 0.1706 0.054*
C7 0.7516 (3) 0.1254 (2) 0.30961 (13) 0.0357 (5)
C8 0.6035 (3) 0.0460 (2) 0.29430 (14) 0.0424 (6)
C9 0.4451 (4) 0.0670 (3) 0.33397 (15) 0.0560 (7)
H9 0.3433 0.0166 0.3244 0.067*
C10 0.4376 (4) 0.1614 (3) 0.38707 (17) 0.0620 (8)
H10 0.3302 0.1752 0.4124 0.074*
C11 0.5853 (4) 0.2345 (3) 0.40283 (14) 0.0555 (8)
H11 0.5782 0.2965 0.4397 0.067*
C12 0.7464 (4) 0.2189 (3) 0.36519 (13) 0.0433 (6)
C13 0.6103 (4) −0.0616 (3) 0.23877 (15) 0.0573 (7)
H13A 0.6806 −0.0340 0.1975 0.069*
H13B 0.4896 −0.0823 0.2232 0.069*
H13C 0.6652 −0.1371 0.2602 0.069*
C14 0.9069 (4) 0.2998 (3) 0.38620 (16) 0.0642 (8)
H14A 1.0162 0.2550 0.3730 0.077*
H14B 0.9055 0.3145 0.4380 0.077*
H14C 0.9017 0.3816 0.3611 0.077*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.1151 (8) 0.0671 (5) 0.0730 (6) −0.0104 (5) −0.0493 (5) 0.0049 (4)
S1 0.0373 (3) 0.0394 (3) 0.0457 (3) −0.0063 (3) 0.0044 (3) −0.0015 (3)
O1 0.0686 (12) 0.0340 (9) 0.0480 (10) −0.0116 (9) 0.0022 (9) 0.0000 (8)
O2 0.0365 (10) 0.0769 (15) 0.0684 (13) −0.0049 (9) 0.0078 (8) −0.0039 (11)
N1 0.0376 (12) 0.0320 (11) 0.0470 (12) 0.0027 (9) 0.0007 (9) 0.0018 (10)
C1 0.0416 (14) 0.0321 (13) 0.0389 (13) −0.0015 (11) 0.0030 (11) 0.0013 (11)
C2 0.0529 (16) 0.0410 (15) 0.0498 (16) 0.0081 (12) 0.0069 (13) −0.0040 (13)
C3 0.084 (2) 0.0459 (17) 0.0407 (15) 0.0074 (17) 0.0016 (15) −0.0071 (13)
C4 0.067 (2) 0.0398 (15) 0.0468 (16) −0.0057 (14) −0.0123 (14) 0.0078 (13)
C5 0.0452 (15) 0.0573 (17) 0.0548 (16) 0.0013 (13) −0.0048 (13) 0.0073 (14)
C6 0.0449 (15) 0.0453 (15) 0.0446 (14) 0.0040 (13) 0.0062 (12) −0.0026 (13)
C7 0.0363 (12) 0.0346 (13) 0.0360 (13) −0.0003 (10) −0.0034 (10) 0.0064 (11)
C8 0.0429 (13) 0.0386 (14) 0.0456 (14) −0.0053 (11) −0.0042 (12) 0.0092 (12)
C9 0.0406 (15) 0.0624 (19) 0.0651 (17) −0.0106 (15) −0.0001 (14) 0.0153 (16)
C10 0.0554 (18) 0.0652 (19) 0.0655 (19) 0.0109 (16) 0.0184 (15) 0.0144 (16)
C11 0.075 (2) 0.0508 (17) 0.0405 (15) 0.0094 (15) 0.0100 (14) 0.0007 (13)
C12 0.0569 (16) 0.0379 (14) 0.0353 (13) −0.0015 (13) −0.0050 (12) 0.0054 (11)
C13 0.0647 (18) 0.0464 (17) 0.0607 (17) −0.0199 (14) −0.0066 (15) −0.0008 (14)
C14 0.080 (2) 0.0604 (19) 0.0521 (16) −0.0142 (18) −0.0114 (15) −0.0103 (16)

Geometric parameters (Å, °)

Cl1—C4 1.731 (3) C7—C8 1.393 (3)
S1—O2 1.4228 (18) C7—C12 1.401 (3)
S1—O1 1.4316 (17) C8—C9 1.393 (4)
S1—N1 1.626 (2) C8—C13 1.504 (3)
S1—C1 1.764 (2) C9—C10 1.375 (4)
N1—C7 1.440 (3) C9—H9 0.9300
N1—H1N 0.818 (16) C10—C11 1.356 (4)
C1—C2 1.383 (3) C10—H10 0.9300
C1—C6 1.385 (3) C11—C12 1.383 (4)
C2—C3 1.380 (4) C11—H11 0.9300
C2—H2 0.9300 C12—C14 1.498 (4)
C3—C4 1.364 (4) C13—H13A 0.9600
C3—H3 0.9300 C13—H13B 0.9600
C4—C5 1.378 (4) C13—H13C 0.9600
C5—C6 1.375 (3) C14—H14A 0.9600
C5—H5 0.9300 C14—H14B 0.9600
C6—H6 0.9300 C14—H14C 0.9600
O2—S1—O1 120.37 (12) C12—C7—N1 118.2 (2)
O2—S1—N1 106.12 (12) C7—C8—C9 117.5 (2)
O1—S1—N1 106.90 (10) C7—C8—C13 122.8 (2)
O2—S1—C1 107.66 (12) C9—C8—C13 119.7 (2)
O1—S1—C1 107.05 (11) C10—C9—C8 120.8 (3)
N1—S1—C1 108.29 (11) C10—C9—H9 119.6
C7—N1—S1 121.78 (16) C8—C9—H9 119.6
C7—N1—H1N 113.2 (19) C11—C10—C9 120.7 (3)
S1—N1—H1N 115.5 (19) C11—C10—H10 119.7
C2—C1—C6 120.6 (2) C9—C10—H10 119.7
C2—C1—S1 120.11 (19) C10—C11—C12 121.4 (3)
C6—C1—S1 119.31 (19) C10—C11—H11 119.3
C3—C2—C1 119.3 (3) C12—C11—H11 119.3
C3—C2—H2 120.4 C11—C12—C7 117.7 (2)
C1—C2—H2 120.4 C11—C12—C14 119.1 (2)
C4—C3—C2 119.8 (3) C7—C12—C14 123.1 (2)
C4—C3—H3 120.1 C8—C13—H13A 109.5
C2—C3—H3 120.1 C8—C13—H13B 109.5
C3—C4—C5 121.3 (3) H13A—C13—H13B 109.5
C3—C4—Cl1 119.4 (2) C8—C13—H13C 109.5
C5—C4—Cl1 119.3 (2) H13A—C13—H13C 109.5
C6—C5—C4 119.4 (3) H13B—C13—H13C 109.5
C6—C5—H5 120.3 C12—C14—H14A 109.5
C4—C5—H5 120.3 C12—C14—H14B 109.5
C5—C6—C1 119.6 (2) H14A—C14—H14B 109.5
C5—C6—H6 120.2 C12—C14—H14C 109.5
C1—C6—H6 120.2 H14A—C14—H14C 109.5
C8—C7—C12 121.8 (2) H14B—C14—H14C 109.5
C8—C7—N1 120.0 (2)
O2—S1—N1—C7 174.71 (18) S1—C1—C6—C5 −175.2 (2)
O1—S1—N1—C7 45.1 (2) S1—N1—C7—C8 97.6 (2)
C1—S1—N1—C7 −69.9 (2) S1—N1—C7—C12 −83.4 (3)
O2—S1—C1—C2 9.0 (2) C12—C7—C8—C9 3.2 (4)
O1—S1—C1—C2 139.75 (19) N1—C7—C8—C9 −177.8 (2)
N1—S1—C1—C2 −105.3 (2) C12—C7—C8—C13 −175.3 (2)
O2—S1—C1—C6 −172.5 (2) N1—C7—C8—C13 3.7 (4)
O1—S1—C1—C6 −41.8 (2) C7—C8—C9—C10 −1.1 (4)
N1—S1—C1—C6 73.1 (2) C13—C8—C9—C10 177.4 (2)
C6—C1—C2—C3 −2.8 (4) C8—C9—C10—C11 −1.2 (4)
S1—C1—C2—C3 175.7 (2) C9—C10—C11—C12 1.5 (4)
C1—C2—C3—C4 0.2 (4) C10—C11—C12—C7 0.5 (4)
C2—C3—C4—C5 2.0 (4) C10—C11—C12—C14 −178.4 (3)
C2—C3—C4—Cl1 −177.7 (2) C8—C7—C12—C11 −2.9 (4)
C3—C4—C5—C6 −1.5 (4) N1—C7—C12—C11 178.1 (2)
Cl1—C4—C5—C6 178.1 (2) C8—C7—C12—C14 175.9 (2)
C4—C5—C6—C1 −1.1 (4) N1—C7—C12—C14 −3.1 (4)
C2—C1—C6—C5 3.3 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O1i 0.82 (2) 2.28 (2) 3.083 (3) 166 (3)

Symmetry codes: (i) −x+2, y−1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BQ2299).

References

  1. Adsmond, D. A. & Grant, D. J. W. (2001). J. Pharm. Sci. 90, 2058–2077. [DOI] [PubMed]
  2. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  3. Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2008). Acta Cryst. E64, o1691. [DOI] [PMC free article] [PubMed]
  4. Gowda, B. T., Foro, S. & Fuess, H. (2007). Acta Cryst. E63, o2570.
  5. Gowda, B. T. & Kumar, B. H. A. (2003). Oxid. Commun. 26, 403–425.
  6. Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
  7. Shakuntala, K., Foro, S. & Gowda, B. T. (2011). Acta Cryst. E67, o1252. [DOI] [PMC free article] [PubMed]
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]

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/S160053681101717X/bq2299sup1.cif

e-67-o1401-sup1.cif (17.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681101717X/bq2299Isup2.hkl

e-67-o1401-Isup2.hkl (135.9KB, hkl)

Supplementary material file. DOI: 10.1107/S160053681101717X/bq2299Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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