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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 6;67(Pt 9):o2258. doi: 10.1107/S1600536811031102

N-(2,6-Dimethyl­phen­yl)-2,4-dimethyl­benzene­sulfonamide

P G Nirmala a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3200847  PMID: 22058917

Abstract

Mol­ecules of the title compound, C16H19NO2S, are bent at the S atom with a C—SO2—NH—C torsion angle of −60.0 (2)°. The dihedral angle between the phenyl­sulfonyl and aniline rings is 41.7 (1)°. In the crystal, mol­ecules are packed into centrosymmetric dimers through pairs of N—H⋯O(S) 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: Arjunan et al. (2004); Gowda et al. (2000), on N-(ar­yl)-methane­sulfonamides, see: Gowda et al. (2007), on N-(ar­yl)-aryl­sulfonamides, see: Gelbrich et al. (2007); Nirmala et al. (2010); Perlovich et al. (2006), and on N-chloro-aryl­sulfonamides, see: Gowda et al. (2003).graphic file with name e-67-o2258-scheme1.jpg

Experimental

Crystal data

  • C16H19NO2S

  • M r = 289.38

  • Monoclinic, Inline graphic

  • a = 11.119 (2) Å

  • b = 8.312 (1) Å

  • c = 16.043 (2) Å

  • β = 97.27 (1)°

  • V = 1470.8 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.22 mm−1

  • T = 293 K

  • 0.48 × 0.36 × 0.20 mm

Data collection

  • Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) T min = 0.901, T max = 0.957

  • 5256 measured reflections

  • 2685 independent reflections

  • 2107 reflections with I > 2σ(I)

  • R int = 0.021

Refinement

  • R[F 2 > 2σ(F 2)] = 0.043

  • wR(F 2) = 0.125

  • S = 1.04

  • 2685 reflections

  • 188 parameters

  • 1 restraint

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

  • Δρmax = 0.28 e Å−3

  • Δρmin = −0.28 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/S1600536811031102/bt5591sup1.cif

e-67-o2258-sup1.cif (18.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031102/bt5591Isup2.hkl

e-67-o2258-Isup2.hkl (131.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811031102/bt5591Isup3.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 0.83 (2) 2.20 (2) 3.024 (3) 168 (2)

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 amide and sulfonamide moieties are the constituents of many biologically important compounds. The hydrogen bonding preferences of sulfonamides have been studied (Adsmond & Grant, 2001). As part of our work on the effects of substituents on the structures and other aspects of N-(aryl)-amides (Arjunan et al., 2004; Gowda et al., 2000), N-(aryl)-methanesulfonamides (Gowda et al., 2007), N-(aryl)-arylsulfonamides (Nirmala et al., 2010) and N-chloro-arylsulfonamides (Gowda et al., 2003), in the present work, the crystal structure of 2,4-dimethyl-N-(2,6-dimethylphenyl)benzenesulfonamide (I) has been determined (Fig. 1).

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 C1—SO2—NH—C7 torsion angle of -60.0 (2)°, compared to the values of 70.1 (2) and -66.0 (2)° in the two independent molecules of 2,4-dimethyl-N-(2,3-dimethylphenyl)benzenesulfonamide (II), 66.5 (2)° in 2,4-dimethyl-N-(2,4-dimethylphenyl)-benzenesulfonamide (III), 53.9 (2)° in 2,4-dimethyl-N-(3,5-dimethylphenyl)- benzenesulfonamide (IV) and 46.1 (3)° (molecule 1) and 47.7 (3)° (molecule 2) in the two independent molecules of 2,4-dimethyl-N-(phenyl)- benzenesulfonamide (V)(Nirmala et al., 2010).

The sulfonyl and the anilino benzene rings in (I) are tilted relative to each other by 41.7 (1)°, compared to the values of 41.5 (1) and 43.8 (1)° in the two molecules of (II), 41.0 (1)° in (III), 82.1 (1)° in (IV) and 67.5 (1)° (molecule 1) and 72.9 (1)° (molecule 2) in (V),

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

In the crystal, packing of molecules into chains through of N—H···O(S) hydrogen bonds (Table 1) is shown in Fig.2.

Experimental

The solution of m-xylene (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 2,4-dimethylbenzenesulfonylchloride 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 solid 2,4-dimethyl-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).

The prism like colourless single crystals used in X-ray diffraction studies were grown in ethanolic solution by a 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 = 0.93Å and methyl C—H = 0.96 Å. 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

C16H19NO2S F(000) = 616
Mr = 289.38 Dx = 1.307 Mg m3
Monoclinic, P2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yc Cell parameters from 922 reflections
a = 11.119 (2) Å θ = 2.5–27.7°
b = 8.312 (1) Å µ = 0.22 mm1
c = 16.043 (2) Å T = 293 K
β = 97.27 (1)° Prism, colourless
V = 1470.8 (4) Å3 0.48 × 0.36 × 0.20 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 2685 independent reflections
Radiation source: fine-focus sealed tube 2107 reflections with I > 2σ(I)
graphite Rint = 0.021
Rotation method data acquisition using ω and φ scans θmax = 25.4°, θmin = 3.0°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −12→13
Tmin = 0.901, Tmax = 0.957 k = −6→10
5256 measured reflections l = −19→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)] = 0.043 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.125 H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0674P)2 + 0.5567P] where P = (Fo2 + 2Fc2)/3
2685 reflections (Δ/σ)max = 0.005
188 parameters Δρmax = 0.28 e Å3
1 restraint Δρmin = −0.28 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 0.21154 (19) 0.9601 (3) 0.45025 (12) 0.0397 (5)
C2 0.1037 (2) 0.9068 (3) 0.40278 (14) 0.0461 (6)
C3 0.0200 (2) 1.0252 (3) 0.37507 (17) 0.0566 (7)
H3 −0.0520 0.9933 0.3435 0.068*
C4 0.0369 (2) 1.1871 (3) 0.39137 (16) 0.0541 (6)
C5 0.1448 (2) 1.2349 (3) 0.43770 (15) 0.0529 (6)
H5 0.1590 1.3434 0.4493 0.063*
C6 0.2309 (2) 1.1225 (3) 0.46654 (14) 0.0444 (5)
H6 0.3030 1.1559 0.4974 0.053*
C7 0.37589 (17) 0.7507 (3) 0.33206 (12) 0.0355 (5)
C8 0.37653 (19) 0.5848 (3) 0.31960 (14) 0.0432 (5)
C9 0.3293 (2) 0.5267 (3) 0.24105 (15) 0.0540 (6)
H9 0.3260 0.4163 0.2317 0.065*
C10 0.2874 (2) 0.6298 (3) 0.17701 (15) 0.0563 (7)
H10 0.2551 0.5888 0.1250 0.068*
C11 0.2929 (2) 0.7931 (3) 0.18931 (14) 0.0484 (6)
H11 0.2665 0.8615 0.1449 0.058*
C12 0.33732 (19) 0.8582 (3) 0.26703 (13) 0.0400 (5)
C13 0.0733 (2) 0.7344 (3) 0.38090 (19) 0.0631 (7)
H13A 0.0683 0.6743 0.4315 0.076*
H13B 0.1354 0.6892 0.3515 0.076*
H13C −0.0032 0.7295 0.3457 0.076*
C14 −0.0588 (3) 1.3083 (4) 0.3596 (2) 0.0775 (9)
H14A −0.1099 1.3288 0.4024 0.093*
H14B −0.1068 1.2668 0.3104 0.093*
H14C −0.0205 1.4067 0.3458 0.093*
C15 0.4295 (2) 0.4694 (3) 0.38653 (16) 0.0560 (6)
H15A 0.3750 0.4581 0.4280 0.067*
H15B 0.5060 0.5099 0.4126 0.067*
H15C 0.4414 0.3665 0.3616 0.067*
C16 0.3431 (2) 1.0378 (3) 0.27633 (15) 0.0517 (6)
H16A 0.4105 1.0663 0.3171 0.062*
H16B 0.2694 1.0761 0.2946 0.062*
H16C 0.3532 1.0857 0.2232 0.062*
N1 0.42138 (16) 0.8124 (2) 0.41422 (10) 0.0386 (4)
H1N 0.466 (2) 0.894 (2) 0.4152 (15) 0.046*
O1 0.28375 (16) 0.6738 (2) 0.50137 (10) 0.0517 (4)
O2 0.40451 (14) 0.9080 (2) 0.55574 (9) 0.0496 (4)
S1 0.33235 (5) 0.82853 (7) 0.48727 (3) 0.04002 (19)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0382 (11) 0.0462 (13) 0.0339 (11) −0.0007 (10) 0.0014 (9) 0.0020 (9)
C2 0.0381 (12) 0.0505 (14) 0.0486 (13) −0.0031 (11) 0.0011 (10) 0.0001 (11)
C3 0.0361 (12) 0.0683 (18) 0.0624 (15) −0.0012 (12) −0.0053 (11) 0.0030 (13)
C4 0.0458 (14) 0.0574 (16) 0.0592 (15) 0.0104 (12) 0.0067 (12) 0.0063 (12)
C5 0.0579 (15) 0.0475 (14) 0.0533 (14) 0.0033 (12) 0.0070 (12) −0.0027 (11)
C6 0.0447 (12) 0.0478 (14) 0.0396 (12) −0.0007 (11) 0.0006 (10) −0.0038 (10)
C7 0.0288 (10) 0.0451 (12) 0.0306 (10) 0.0006 (9) −0.0037 (8) −0.0007 (9)
C8 0.0362 (11) 0.0452 (14) 0.0464 (12) 0.0010 (10) −0.0016 (9) −0.0017 (10)
C9 0.0522 (14) 0.0509 (15) 0.0562 (15) −0.0032 (12) −0.0036 (12) −0.0148 (12)
C10 0.0496 (14) 0.0730 (18) 0.0425 (13) −0.0029 (13) −0.0091 (11) −0.0152 (12)
C11 0.0434 (13) 0.0666 (17) 0.0327 (11) 0.0052 (12) −0.0049 (10) 0.0016 (11)
C12 0.0347 (11) 0.0502 (14) 0.0341 (11) 0.0022 (10) 0.0004 (9) 0.0002 (9)
C13 0.0477 (14) 0.0585 (16) 0.0784 (18) −0.0082 (13) −0.0109 (13) −0.0060 (14)
C14 0.0596 (17) 0.075 (2) 0.096 (2) 0.0187 (16) 0.0015 (16) 0.0111 (17)
C15 0.0622 (15) 0.0474 (14) 0.0562 (15) 0.0072 (13) −0.0008 (12) 0.0045 (11)
C16 0.0613 (15) 0.0502 (15) 0.0425 (12) 0.0019 (12) 0.0027 (11) 0.0079 (11)
N1 0.0387 (10) 0.0431 (11) 0.0317 (9) −0.0037 (8) −0.0039 (7) −0.0021 (8)
O1 0.0561 (10) 0.0492 (10) 0.0493 (9) −0.0023 (8) 0.0044 (8) 0.0109 (7)
O2 0.0516 (9) 0.0622 (11) 0.0313 (8) 0.0006 (8) −0.0089 (7) −0.0041 (7)
S1 0.0414 (3) 0.0467 (3) 0.0300 (3) −0.0006 (2) −0.0033 (2) 0.0015 (2)

Geometric parameters (Å, °)

C1—C6 1.387 (3) C10—H10 0.9300
C1—C2 1.408 (3) C11—C12 1.391 (3)
C1—S1 1.775 (2) C11—H11 0.9300
C2—C3 1.388 (3) C12—C16 1.500 (3)
C2—C13 1.504 (4) C13—H13A 0.9600
C3—C4 1.379 (4) C13—H13B 0.9600
C3—H3 0.9300 C13—H13C 0.9600
C4—C5 1.387 (4) C14—H14A 0.9600
C4—C14 1.506 (4) C14—H14B 0.9600
C5—C6 1.375 (3) C14—H14C 0.9600
C5—H5 0.9300 C15—H15A 0.9600
C6—H6 0.9300 C15—H15B 0.9600
C7—C8 1.394 (3) C15—H15C 0.9600
C7—C12 1.399 (3) C16—H16A 0.9600
C7—N1 1.445 (2) C16—H16B 0.9600
C8—C9 1.389 (3) C16—H16C 0.9600
C8—C15 1.503 (3) N1—S1 1.6325 (19)
C9—C10 1.373 (4) N1—H1N 0.834 (16)
C9—H9 0.9300 O1—S1 1.4242 (17)
C10—C11 1.372 (4) O2—S1 1.4364 (15)
C6—C1—C2 120.6 (2) C7—C12—C16 123.77 (19)
C6—C1—S1 116.35 (17) C2—C13—H13A 109.5
C2—C1—S1 122.97 (18) C2—C13—H13B 109.5
C3—C2—C1 116.1 (2) H13A—C13—H13B 109.5
C3—C2—C13 118.7 (2) C2—C13—H13C 109.5
C1—C2—C13 125.2 (2) H13A—C13—H13C 109.5
C4—C3—C2 124.2 (2) H13B—C13—H13C 109.5
C4—C3—H3 117.9 C4—C14—H14A 109.5
C2—C3—H3 117.9 C4—C14—H14B 109.5
C3—C4—C5 117.9 (2) H14A—C14—H14B 109.5
C3—C4—C14 121.0 (3) C4—C14—H14C 109.5
C5—C4—C14 121.0 (3) H14A—C14—H14C 109.5
C6—C5—C4 120.3 (2) H14B—C14—H14C 109.5
C6—C5—H5 119.9 C8—C15—H15A 109.5
C4—C5—H5 119.9 C8—C15—H15B 109.5
C5—C6—C1 120.9 (2) H15A—C15—H15B 109.5
C5—C6—H6 119.6 C8—C15—H15C 109.5
C1—C6—H6 119.6 H15A—C15—H15C 109.5
C8—C7—C12 122.12 (19) H15B—C15—H15C 109.5
C8—C7—N1 118.32 (18) C12—C16—H16A 109.5
C12—C7—N1 119.50 (19) C12—C16—H16B 109.5
C9—C8—C7 117.8 (2) H16A—C16—H16B 109.5
C9—C8—C15 119.7 (2) C12—C16—H16C 109.5
C7—C8—C15 122.5 (2) H16A—C16—H16C 109.5
C10—C9—C8 121.0 (2) H16B—C16—H16C 109.5
C10—C9—H9 119.5 C7—N1—S1 120.67 (14)
C8—C9—H9 119.5 C7—N1—H1N 116.2 (16)
C11—C10—C9 120.3 (2) S1—N1—H1N 109.3 (17)
C11—C10—H10 119.8 O1—S1—O2 118.69 (10)
C9—C10—H10 119.8 O1—S1—N1 108.46 (10)
C10—C11—C12 121.2 (2) O2—S1—N1 104.84 (9)
C10—C11—H11 119.4 O1—S1—C1 108.85 (10)
C12—C11—H11 119.4 O2—S1—C1 107.37 (10)
C11—C12—C7 117.4 (2) N1—S1—C1 108.20 (9)
C11—C12—C16 118.8 (2)
C6—C1—C2—C3 −0.6 (3) C8—C9—C10—C11 0.8 (4)
S1—C1—C2—C3 −177.08 (18) C9—C10—C11—C12 −2.0 (4)
C6—C1—C2—C13 179.7 (2) C10—C11—C12—C7 −0.1 (3)
S1—C1—C2—C13 3.2 (3) C10—C11—C12—C16 179.0 (2)
C1—C2—C3—C4 −0.1 (4) C8—C7—C12—C11 3.3 (3)
C13—C2—C3—C4 179.6 (3) N1—C7—C12—C11 −179.25 (19)
C2—C3—C4—C5 0.7 (4) C8—C7—C12—C16 −175.7 (2)
C2—C3—C4—C14 −179.5 (3) N1—C7—C12—C16 1.7 (3)
C3—C4—C5—C6 −0.5 (4) C8—C7—N1—S1 −86.7 (2)
C14—C4—C5—C6 179.7 (2) C12—C7—N1—S1 95.8 (2)
C4—C5—C6—C1 −0.2 (4) C7—N1—S1—O1 57.93 (19)
C2—C1—C6—C5 0.8 (3) C7—N1—S1—O2 −174.33 (16)
S1—C1—C6—C5 177.48 (18) C7—N1—S1—C1 −59.99 (19)
C12—C7—C8—C9 −4.4 (3) C6—C1—S1—O1 153.48 (17)
N1—C7—C8—C9 178.15 (19) C2—C1—S1—O1 −29.9 (2)
C12—C7—C8—C15 173.6 (2) C6—C1—S1—O2 23.8 (2)
N1—C7—C8—C15 −3.8 (3) C2—C1—S1—O2 −159.61 (18)
C7—C8—C9—C10 2.3 (4) C6—C1—S1—N1 −88.85 (18)
C15—C8—C9—C10 −175.8 (2) C2—C1—S1—N1 87.7 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O2i 0.83 (2) 2.20 (2) 3.024 (3) 168 (2)

Symmetry codes: (i) −x+1, −y+2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5591).

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/S1600536811031102/bt5591sup1.cif

e-67-o2258-sup1.cif (18.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031102/bt5591Isup2.hkl

e-67-o2258-Isup2.hkl (131.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811031102/bt5591Isup3.cml

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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