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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Oct 8;67(Pt 11):o2890. doi: 10.1107/S1600536811040888

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

Vinola Z Rodrigues a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3247307  PMID: 22219925

Abstract

In the title compound, C15H16ClNO2S, the C—SO2—NH—C torsion angle is −61.15 (16)°. The sulfonyl and aniline benzene rings are tilted relative to each other by 38.8 (1)°. The crystal structure features inversion-related dimers linked by pairs of N—H⋯O hydrogen bonds.

Related literature

For the preparation of the title compound, see: Savitha & Gowda (2006). For hydrogen-bonding modes of sulfonamides, see: Adsmond & Grant (2001). For studies on the effects of substituents on the structures and other aspects of N-(ar­yl)-amides, see: Gowda et al. (2000), on N-(ar­yl)-methane­sulfon­amides, see: Gowda et al. (2007), on N-(ar­yl)-aryl­sulfon­amides, see: Gelbrich et al. (2007); Perlovich et al. (2006); Rodrigues et al. (2011); Shetty & Gowda (2005) and on N-(chloro)-aryl­sulfonamides, see: Gowda et al. (2003).graphic file with name e-67-o2890-scheme1.jpg

Experimental

Crystal data

  • C15H16ClNO2S

  • M r = 309.80

  • Triclinic, Inline graphic

  • a = 8.275 (2) Å

  • b = 8.430 (2) Å

  • c = 11.195 (2) Å

  • α = 92.12 (1)°

  • β = 96.15 (1)°

  • γ = 109.58 (2)°

  • V = 729.3 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.41 mm−1

  • T = 293 K

  • 0.46 × 0.40 × 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 = 0.836, T max = 0.909

  • 4886 measured reflections

  • 2948 independent reflections

  • 2588 reflections with I > 2σ(I)

  • R int = 0.011

Refinement

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.096

  • S = 1.06

  • 2948 reflections

  • 187 parameters

  • 1 restraint

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

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.45 e Å−3

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 datablock(s) I, global. DOI: 10.1107/S1600536811040888/bt5663sup1.cif

e-67-o2890-sup1.cif (18.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811040888/bt5663Isup2.hkl

e-67-o2890-Isup2.hkl (144.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811040888/bt5663Isup3.cml

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1N⋯O2i 0.84 (2) 2.21 (2) 3.024 (2) 165 (2)

Symmetry code: (i) Inline graphic.

Acknowledgments

VZR thanks the University Grants Commission, Government of India, New Delhi, for the award of an RFSMS fellowship.

supplementary crystallographic information

Comment

The amide and sulfonamide moieties are the constituents of many biologically significant compounds. The hydrogen bonding preferences of sulfonamides have been investigated (Adsmond & Grant, 2001). As part of our studies on the substituent effects on the structures and other aspects of N-(aryl)-amides (Gowda et al., 2000), N-(aryl)-methanesulfonamides (Gowda et al., 2007), N-(aryl)-arylsulfonamides (Rodrigues et al., 2011; Shetty & Gowda, 2005) and N-(chloro)-arylsulfonamides (Gowda et al., 2003), in the present work, the crystal structure of 4-Chloro-2-methyl-N-(2,6-dimethylphenyl)benzenesulfonamide (I) has been determined (Fig. 1).

In (I), the conformation of the N—C bond in the C—SO2—NH—C segment has gauche torsions with respect to the S═O bonds. The molecule is bent at the S atom with the C—SO2—NH—C torsion angle of -61.2 (2)°, compared to the value of 67.5 (2)° in 4-Chloro-2-methyl-N-(2,4-dimethylphenyl)benzenesulfonamide (II) (Rodrigues et al., 2011).

The sulfonyl and the aniline benzene rings are tilted relative to each other by 38.8 (1)°, compared to the value of 44.5 (1)° in (II).

The other bond parameters in (I) are similar to those observed in (II), and other aryl sulfonamides (Perlovich et al., 2006; Gelbrich et al., 2007).

In the crystal, the intermolecular N–H···O hydrogen bonds (Table 1) link the molecules into dimeric chains. Part of the crystal structure is shown in Fig. 2.

Experimental

The solution of m-chlorotoluene (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 2-methyl-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 cc). The resultant solid 4-chloro-2-methyl-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 purity of the compound was checked and characterized by recording its infrared and NMR spectra (Savitha & Gowda, 2006).

Rod like colourless 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 wwa located in a difference map and its coordinates were refined with the N-H distance restrained to 0.86 (2) %A. The other H atoms were positioned with idealized geometry using a riding model with the aromatic C—H = 0.93Å and methyl C—H = 0.96 Å. All H atoms were refined with isotropic displacement parameters. The Uiso(H) values were set at 1.2Ueq(C-aromatic, N) and 1.5Ueq(C-methyl).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, 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

C15H16ClNO2S Z = 2
Mr = 309.80 F(000) = 324
Triclinic, P1 Dx = 1.411 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.275 (2) Å Cell parameters from 2916 reflections
b = 8.430 (2) Å θ = 2.6–27.8°
c = 11.195 (2) Å µ = 0.41 mm1
α = 92.12 (1)° T = 293 K
β = 96.15 (1)° Rod, colourless
γ = 109.58 (2)° 0.46 × 0.40 × 0.24 mm
V = 729.3 (3) Å3

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 2948 independent reflections
Radiation source: fine-focus sealed tube 2588 reflections with I > 2σ(I)
graphite Rint = 0.011
Rotation method data acquisition using ω scans θmax = 26.4°, θmin = 2.6°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −9→10
Tmin = 0.836, Tmax = 0.909 k = −10→10
4886 measured reflections l = −13→11

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096 H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0348P)2 + 0.4969P] where P = (Fo2 + 2Fc2)/3
2948 reflections (Δ/σ)max < 0.001
187 parameters Δρmax = 0.31 e Å3
1 restraint Δρmin = −0.45 e Å3

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 0.3930 (2) 0.4028 (2) 0.21423 (16) 0.0332 (4)
C2 0.2952 (3) 0.3124 (2) 0.10740 (17) 0.0394 (4)
C3 0.3843 (3) 0.2532 (3) 0.02725 (18) 0.0467 (5)
H3 0.3235 0.1908 −0.0436 0.056*
C4 0.5591 (3) 0.2846 (3) 0.05010 (19) 0.0462 (5)
C5 0.6547 (3) 0.3732 (3) 0.1545 (2) 0.0462 (5)
H5 0.7730 0.3938 0.1694 0.055*
C6 0.5698 (2) 0.4307 (2) 0.23665 (18) 0.0395 (4)
H6 0.6318 0.4892 0.3084 0.047*
C7 0.1102 (2) 0.1667 (2) 0.37777 (15) 0.0314 (4)
C8 0.1613 (3) 0.0322 (2) 0.34000 (17) 0.0379 (4)
C9 0.0315 (3) −0.1166 (3) 0.29221 (19) 0.0507 (6)
H9 0.0613 −0.2074 0.2649 0.061*
C10 −0.1402 (3) −0.1317 (3) 0.2847 (2) 0.0569 (6)
H10 −0.2246 −0.2313 0.2505 0.068*
C11 −0.1880 (3) −0.0012 (3) 0.3271 (2) 0.0514 (5)
H11 −0.3047 −0.0142 0.3226 0.062*
C12 −0.0641 (2) 0.1505 (2) 0.37689 (17) 0.0379 (4)
C13 0.1034 (3) 0.2753 (3) 0.0727 (2) 0.0559 (6)
H13A 0.0824 0.3789 0.0591 0.067*
H13B 0.0416 0.2222 0.1365 0.067*
H13C 0.0646 0.2012 0.0003 0.067*
C14 0.3469 (3) 0.0408 (3) 0.3529 (2) 0.0521 (5)
H14A 0.4067 0.1047 0.4268 0.063*
H14B 0.4007 0.0947 0.2862 0.063*
H14C 0.3516 −0.0714 0.3537 0.063*
C15 −0.1197 (3) 0.2859 (3) 0.4316 (2) 0.0492 (5)
H15A −0.0981 0.3784 0.3810 0.059*
H15B −0.0556 0.3249 0.5100 0.059*
H15C −0.2410 0.2411 0.4387 0.059*
N1 0.2397 (2) 0.32745 (19) 0.42256 (14) 0.0335 (3)
H1N 0.325 (2) 0.324 (3) 0.4680 (18) 0.040*
O1 0.15174 (18) 0.51087 (17) 0.27909 (13) 0.0433 (3)
O2 0.43786 (18) 0.61202 (16) 0.40162 (13) 0.0448 (3)
Cl1 0.66049 (10) 0.20864 (10) −0.05578 (6) 0.0746 (2)
S1 0.30108 (6) 0.47803 (5) 0.33118 (4) 0.03365 (13)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0364 (9) 0.0281 (8) 0.0340 (9) 0.0096 (7) 0.0053 (7) 0.0015 (7)
C2 0.0418 (10) 0.0407 (10) 0.0341 (9) 0.0137 (8) 0.0006 (8) 0.0003 (8)
C3 0.0544 (13) 0.0512 (12) 0.0328 (10) 0.0182 (10) 0.0011 (9) −0.0046 (9)
C4 0.0542 (12) 0.0479 (12) 0.0431 (11) 0.0229 (10) 0.0158 (9) 0.0044 (9)
C5 0.0382 (10) 0.0510 (12) 0.0497 (12) 0.0144 (9) 0.0093 (9) 0.0044 (9)
C6 0.0368 (10) 0.0360 (10) 0.0409 (10) 0.0071 (8) 0.0033 (8) 0.0000 (8)
C7 0.0365 (9) 0.0287 (9) 0.0253 (8) 0.0075 (7) 0.0003 (7) −0.0003 (7)
C8 0.0501 (11) 0.0325 (9) 0.0313 (9) 0.0153 (8) 0.0030 (8) 0.0012 (7)
C9 0.0784 (16) 0.0300 (10) 0.0391 (11) 0.0152 (10) 0.0001 (10) −0.0039 (8)
C10 0.0656 (15) 0.0368 (11) 0.0463 (12) −0.0050 (10) −0.0112 (11) −0.0026 (9)
C11 0.0385 (11) 0.0539 (13) 0.0487 (12) 0.0010 (10) −0.0030 (9) 0.0077 (10)
C12 0.0375 (10) 0.0398 (10) 0.0335 (9) 0.0096 (8) 0.0027 (8) 0.0055 (8)
C13 0.0439 (12) 0.0775 (16) 0.0412 (12) 0.0199 (11) −0.0082 (9) −0.0126 (11)
C14 0.0612 (14) 0.0455 (12) 0.0589 (14) 0.0290 (11) 0.0115 (11) 0.0042 (10)
C15 0.0445 (11) 0.0550 (13) 0.0540 (13) 0.0222 (10) 0.0133 (10) 0.0075 (10)
N1 0.0342 (8) 0.0305 (8) 0.0313 (8) 0.0078 (6) −0.0030 (6) −0.0029 (6)
O1 0.0454 (8) 0.0411 (8) 0.0487 (8) 0.0216 (6) 0.0057 (6) 0.0036 (6)
O2 0.0474 (8) 0.0298 (7) 0.0486 (8) 0.0042 (6) 0.0020 (6) −0.0089 (6)
Cl1 0.0795 (5) 0.0927 (5) 0.0632 (4) 0.0401 (4) 0.0278 (3) −0.0078 (4)
S1 0.0362 (2) 0.0266 (2) 0.0361 (2) 0.00905 (18) 0.00272 (18) −0.00301 (17)

Geometric parameters (Å, °)

C1—C6 1.394 (3) C10—C11 1.374 (4)
C1—C2 1.406 (3) C10—H10 0.9300
C1—S1 1.7805 (19) C11—C12 1.394 (3)
C2—C3 1.397 (3) C11—H11 0.9300
C2—C13 1.515 (3) C12—C15 1.500 (3)
C3—C4 1.374 (3) C13—H13A 0.9600
C3—H3 0.9300 C13—H13B 0.9600
C4—C5 1.375 (3) C13—H13C 0.9600
C4—Cl1 1.742 (2) C14—H14A 0.9600
C5—C6 1.381 (3) C14—H14B 0.9600
C5—H5 0.9300 C14—H14C 0.9600
C6—H6 0.9300 C15—H15A 0.9600
C7—C12 1.401 (3) C15—H15B 0.9600
C7—C8 1.403 (3) C15—H15C 0.9600
C7—N1 1.448 (2) N1—S1 1.6405 (16)
C8—C9 1.392 (3) N1—H1N 0.835 (15)
C8—C14 1.503 (3) O1—S1 1.4250 (14)
C9—C10 1.377 (4) O2—S1 1.4369 (14)
C9—H9 0.9300
C6—C1—C2 120.62 (17) C12—C11—H11 119.6
C6—C1—S1 115.99 (14) C11—C12—C7 117.58 (19)
C2—C1—S1 123.31 (14) C11—C12—C15 119.85 (19)
C3—C2—C1 116.59 (18) C7—C12—C15 122.52 (18)
C3—C2—C13 117.95 (18) C2—C13—H13A 109.5
C1—C2—C13 125.46 (18) C2—C13—H13B 109.5
C4—C3—C2 121.87 (19) H13A—C13—H13B 109.5
C4—C3—H3 119.1 C2—C13—H13C 109.5
C2—C3—H3 119.1 H13A—C13—H13C 109.5
C3—C4—C5 121.49 (19) H13B—C13—H13C 109.5
C3—C4—Cl1 118.87 (17) C8—C14—H14A 109.5
C5—C4—Cl1 119.64 (17) C8—C14—H14B 109.5
C4—C5—C6 118.02 (19) H14A—C14—H14B 109.5
C4—C5—H5 121.0 C8—C14—H14C 109.5
C6—C5—H5 121.0 H14A—C14—H14C 109.5
C5—C6—C1 121.38 (19) H14B—C14—H14C 109.5
C5—C6—H6 119.3 C12—C15—H15A 109.5
C1—C6—H6 119.3 C12—C15—H15B 109.5
C12—C7—C8 122.19 (17) H15A—C15—H15B 109.5
C12—C7—N1 117.89 (16) C12—C15—H15C 109.5
C8—C7—N1 119.90 (16) H15A—C15—H15C 109.5
C9—C8—C7 117.36 (19) H15B—C15—H15C 109.5
C9—C8—C14 119.58 (19) C7—N1—S1 119.87 (12)
C7—C8—C14 123.02 (17) C7—N1—H1N 116.8 (15)
C10—C9—C8 121.1 (2) S1—N1—H1N 109.8 (15)
C10—C9—H9 119.4 O1—S1—O2 118.97 (9)
C8—C9—H9 119.4 O1—S1—N1 108.26 (9)
C11—C10—C9 120.7 (2) O2—S1—N1 105.13 (8)
C11—C10—H10 119.7 O1—S1—C1 108.66 (9)
C9—C10—H10 119.7 O2—S1—C1 107.46 (9)
C10—C11—C12 120.9 (2) N1—S1—C1 107.89 (8)
C10—C11—H11 119.6
C6—C1—C2—C3 0.2 (3) C8—C9—C10—C11 −1.7 (3)
S1—C1—C2—C3 −176.35 (15) C9—C10—C11—C12 1.1 (3)
C6—C1—C2—C13 −179.5 (2) C10—C11—C12—C7 2.3 (3)
S1—C1—C2—C13 3.9 (3) C10—C11—C12—C15 −175.1 (2)
C1—C2—C3—C4 −1.4 (3) C8—C7—C12—C11 −5.4 (3)
C13—C2—C3—C4 178.4 (2) N1—C7—C12—C11 176.31 (16)
C2—C3—C4—C5 1.3 (3) C8—C7—C12—C15 171.99 (18)
C2—C3—C4—Cl1 −179.08 (17) N1—C7—C12—C15 −6.3 (3)
C3—C4—C5—C6 −0.1 (3) C12—C7—N1—S1 −86.30 (19)
Cl1—C4—C5—C6 −179.66 (16) C8—C7—N1—S1 95.34 (18)
C4—C5—C6—C1 −1.1 (3) C7—N1—S1—O1 56.27 (16)
C2—C1—C6—C5 1.0 (3) C7—N1—S1—O2 −175.60 (13)
S1—C1—C6—C5 177.81 (16) C7—N1—S1—C1 −61.15 (16)
C12—C7—C8—C9 4.8 (3) C6—C1—S1—O1 154.04 (14)
N1—C7—C8—C9 −176.88 (16) C2—C1—S1—O1 −29.23 (18)
C12—C7—C8—C14 −173.08 (18) C6—C1—S1—O2 24.10 (17)
N1—C7—C8—C14 5.2 (3) C2—C1—S1—O2 −159.17 (16)
C7—C8—C9—C10 −1.2 (3) C6—C1—S1—N1 −88.80 (15)
C14—C8—C9—C10 176.7 (2) C2—C1—S1—N1 87.93 (17)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O2i 0.84 (2) 2.21 (2) 3.024 (2) 165 (2)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5663).

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 datablock(s) I, global. DOI: 10.1107/S1600536811040888/bt5663sup1.cif

e-67-o2890-sup1.cif (18.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811040888/bt5663Isup2.hkl

e-67-o2890-Isup2.hkl (144.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811040888/bt5663Isup3.cml

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


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