organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

N-(3,5-Di­methyl­phen­yl)benzene­sulfonamide

aDepartment of Chemistry, Mangalore University, Mangalagangotri 574 199, Mangalore, India, and bInstitute of Materials Science, Darmstadt University of Technology, Petersenstrasse 23, D-64287 Darmstadt, Germany
*Correspondence e-mail: gowdabt@yahoo.com

(Received 15 November 2009; accepted 21 November 2009; online 28 November 2009)

In the crystal structure of the title compound, C14H15NO2S, the mol­ecule is bent at the S atom with a C—SO2—NH—C torsion angle of 67.9 (2)°. The two benzene rings are tilted by 54.6 (1)° relative to each other. In the crystal, inter­molecular N—H⋯O hydrogen bonds pack the mol­ecules into a supra­molecular structure.

Related literature

For preparation of the title compound, see: Gowda et al. (2005[Gowda, B. T., Shetty, M. & Jayalakshmi, K. L. (2005). Z. Naturforsch. Teil A, 60, 106-112.]). For our study of the effects of substituents on the structures of N-(ar­yl)-aryl­sulfonamides, see: Gowda et al. (2008[Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2008). Acta Cryst. E64, o1691.]; 2009a[Gowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2009a). Acta Cryst. E65, o366.],b[Gowda, B. T., Foro, S., Nirmala, P. G. & Fuess, H. (2009b). Acta Cryst. E65, o2763.]). For related structures, see: Gelbrich et al. (2007[Gelbrich, T., Hursthouse, M. B. & Threlfall, T. L. (2007). Acta Cryst. B63, 621-632.]); Perlovich et al. (2006[Perlovich, G. L., Tkachev, V. V., Schaper, K.-J. & Raevsky, O. A. (2006). Acta Cryst. E62, o780-o782.]).

[Scheme 1]

Experimental

Crystal data
  • C14H15NO2S

  • Mr = 261.33

  • Monoclinic, P 21 /c

  • a = 11.192 (1) Å

  • b = 7.3543 (7) Å

  • c = 16.672 (2) Å

  • β = 101.62 (1)°

  • V = 1344.1 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.23 mm−1

  • T = 299 K

  • 0.48 × 0.40 × 0.18 mm

Data collection
  • Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009[Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED. Oxford Diffraction Ltd, Yarnton, England.]) Tmin = 0.896, Tmax = 0.959

  • 5063 measured reflections

  • 2742 independent reflections

  • 2187 reflections with I > 2σ(I)

  • Rint = 0.015

Refinement
  • R[F2 > 2σ(F2)] = 0.038

  • wR(F2) = 0.111

  • S = 1.05

  • 2742 reflections

  • 169 parameters

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

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.31 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1N⋯O1i 0.81 (2) 2.14 (2) 2.942 (2) 176 (2)
Symmetry code: (i) [-x+1, y+{\script{1\over 2}}, -z+{\script{3\over 2}}].

Data collection: CrysAlis CCD (Oxford Diffraction, 2009[Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED. Oxford Diffraction Ltd, Yarnton, England.]); cell refinement: CrysAlis RED (Oxford Diffraction, 2009[Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED. Oxford Diffraction Ltd, Yarnton, England.]); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: PLATON (Spek, 2009[Spek, A. L. (2009). Acta Cryst. D65, 148-155.]); software used to prepare material for publication: SHELXL97.

Supporting information


Comment top

As part of a study of substituent effects on the structures of N-(aryl)-arylsulfonamides (Gowda et al., 2008; 2009a,b), in the present work, the structure of N-(3,5-dimethylphenyl)benzenesulfonamide (I) has been determined (Fig. 1). The molecule is bent at the S atom with the C1—SO2—NH—C7 torsion angle of 67.9 (2)°, compared to the values of 71.0 (2)° in N-(2,3-dimethylphenyl)benzenesulfonamide (II)(Gowda et al., 2009a), 62.7 (2)° in N-(2,5-dimethylphenyl)benzenesulfonamide (III) (Gowda et al., 2009b) and -78.7 (2)° in N-(2,6-dimethylphenyl)benzenesulfonamide (IV)(Gowda et al., 2008). The two benzene rings in (I) are tilted relative to each other by 54.6 (1)°, compared to the values of 64.8 (1)° in (II), 40.4 (1)° in (III) and 44.9 (1)° in (IV). The other bond parameters in (I) are similar to those observed in (II), (III), (IV) and other aryl sulfonamides (Perlovich et al., 2006; Gelbrich et al., 2007). The crystal packing of molecules in (I) via N—H···O(S) hydrogen bonds (Table 1) is shown in Fig.2.

Related literature top

For preparation of the title compound, see: Gowda et al. (2005). For our study of the effects of substituents on the structures of N-(aryl)-arylsulfonamides, see: Gowda et al. (2008; 2009a,b). For related structures, see: Gelbrich et al. (2007); Perlovich et al. (2006)

Experimental top

The solution of benzene (10 cc) in chloroform (40 cc) was treated dropwise with chlorosulfonic acid (25 cc) 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 benzenesulfonylchloride was treated with 3,5-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 N-(3,5-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 (Gowda et al., 2005). The single crystals used in X-ray diffraction studies were grown in ethanolic solution by a slow evaporation at room temperature.

Refinement top

The H atom of the NH was located in difference map and its positional parameters were refined freely [N—H = 0.81 (2) Å]. The other H atoms were positioned with idealized geometry using a riding model [C—H = 0.93—0.96 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.
N-(3,5-Dimethylphenyl)benzenesulfonamide top
Crystal data top
C14H15NO2SF(000) = 552
Mr = 261.33Dx = 1.291 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 11.192 (1) Åθ = 2.5–27.8°
b = 7.3543 (7) ŵ = 0.23 mm1
c = 16.672 (2) ÅT = 299 K
β = 101.62 (1)°Prism, colourless
V = 1344.1 (2) Å30.48 × 0.40 × 0.18 mm
Z = 4
Data collection top
Oxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
2742 independent reflections
Radiation source: fine-focus sealed tube2187 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.015
Rotation method data acquisition using ω and phi scansθmax = 26.4°, θmin = 2.5°
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2009)
h = 1313
Tmin = 0.896, Tmax = 0.959k = 69
5063 measured reflectionsl = 920
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)] = 0.038H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.111 w = 1/[σ2(Fo2) + (0.0575P)2 + 0.3783P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.004
2742 reflectionsΔρmax = 0.31 e Å3
169 parametersΔρmin = 0.31 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0115 (18)
Crystal data top
C14H15NO2SV = 1344.1 (2) Å3
Mr = 261.33Z = 4
Monoclinic, P21/cMo Kα radiation
a = 11.192 (1) ŵ = 0.23 mm1
b = 7.3543 (7) ÅT = 299 K
c = 16.672 (2) Å0.48 × 0.40 × 0.18 mm
β = 101.62 (1)°
Data collection top
Oxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
2742 independent reflections
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2009)
2187 reflections with I > 2σ(I)
Tmin = 0.896, Tmax = 0.959Rint = 0.015
5063 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0380 restraints
wR(F2) = 0.111H atoms treated by a mixture of independent and constrained refinement
S = 1.05Δρmax = 0.31 e Å3
2742 reflectionsΔρmin = 0.31 e Å3
169 parameters
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
C10.41245 (16)0.1889 (3)0.59746 (11)0.0434 (4)
C20.52681 (19)0.2478 (3)0.59053 (14)0.0618 (6)
H20.58730.26680.63690.074*
C30.5495 (3)0.2780 (4)0.51321 (17)0.0816 (8)
H30.62660.31610.50740.098*
C40.4597 (3)0.2524 (4)0.44490 (15)0.0790 (8)
H40.47640.27160.39310.095*
C50.3458 (3)0.1986 (4)0.45274 (14)0.0805 (8)
H50.28460.18460.40630.097*
C60.3209 (2)0.1650 (3)0.52926 (13)0.0620 (6)
H60.24380.12680.53470.074*
C70.20322 (14)0.3865 (2)0.68610 (10)0.0354 (4)
C80.18940 (16)0.5491 (2)0.64340 (10)0.0410 (4)
H80.25780.61620.63810.049*
C90.07428 (18)0.6121 (3)0.60856 (12)0.0479 (5)
C100.02579 (17)0.5069 (3)0.61670 (12)0.0514 (5)
H100.10350.54770.59290.062*
C110.01416 (16)0.3444 (3)0.65873 (12)0.0489 (5)
C120.10215 (16)0.2850 (3)0.69465 (11)0.0430 (4)
H120.11220.17720.72440.052*
C130.0577 (2)0.7909 (3)0.56388 (16)0.0733 (7)
H13A0.13230.82390.54760.088*
H13B0.03640.88300.59930.088*
H13C0.00630.77990.51620.088*
C140.12452 (19)0.2338 (4)0.66755 (16)0.0755 (7)
H14A0.17170.20580.61420.091*
H14B0.17350.30230.69780.091*
H14C0.09850.12290.69620.091*
N10.32271 (13)0.3272 (2)0.72571 (9)0.0395 (4)
H1N0.3739 (18)0.406 (3)0.7338 (12)0.047*
O10.49861 (12)0.12569 (19)0.75071 (8)0.0526 (4)
O20.29563 (13)0.00239 (19)0.68847 (10)0.0590 (4)
S10.38310 (4)0.14444 (6)0.69537 (3)0.04071 (17)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0437 (10)0.0417 (10)0.0431 (9)0.0098 (8)0.0043 (8)0.0040 (8)
C20.0500 (12)0.0781 (15)0.0577 (13)0.0046 (11)0.0119 (10)0.0035 (11)
C30.0782 (18)0.100 (2)0.0758 (17)0.0074 (16)0.0366 (14)0.0110 (16)
C40.110 (2)0.0806 (18)0.0512 (14)0.0199 (16)0.0283 (15)0.0035 (12)
C50.104 (2)0.0826 (18)0.0466 (13)0.0137 (16)0.0035 (13)0.0090 (12)
C60.0616 (14)0.0681 (14)0.0509 (12)0.0016 (11)0.0019 (10)0.0081 (10)
C70.0323 (8)0.0407 (9)0.0330 (8)0.0014 (7)0.0063 (6)0.0033 (7)
C80.0411 (9)0.0395 (9)0.0419 (9)0.0038 (8)0.0074 (7)0.0010 (7)
C90.0507 (11)0.0427 (10)0.0458 (10)0.0040 (8)0.0008 (8)0.0007 (8)
C100.0365 (10)0.0596 (12)0.0539 (11)0.0079 (9)0.0012 (8)0.0014 (10)
C110.0354 (9)0.0621 (12)0.0495 (11)0.0036 (8)0.0093 (8)0.0006 (9)
C120.0393 (9)0.0463 (10)0.0441 (10)0.0018 (8)0.0101 (7)0.0058 (8)
C130.0773 (16)0.0504 (13)0.0804 (17)0.0035 (12)0.0119 (13)0.0119 (12)
C140.0411 (12)0.100 (2)0.0858 (17)0.0124 (12)0.0142 (11)0.0160 (15)
N10.0326 (8)0.0392 (8)0.0450 (8)0.0012 (6)0.0038 (6)0.0030 (6)
O10.0436 (7)0.0577 (8)0.0510 (7)0.0142 (6)0.0032 (6)0.0062 (6)
O20.0556 (8)0.0410 (7)0.0798 (10)0.0062 (6)0.0123 (7)0.0002 (7)
S10.0367 (3)0.0373 (3)0.0457 (3)0.00433 (18)0.00246 (18)0.00225 (18)
Geometric parameters (Å, º) top
C1—C21.378 (3)C9—C101.390 (3)
C1—C61.380 (3)C9—C131.505 (3)
C1—S11.7594 (19)C10—C111.378 (3)
C2—C31.381 (3)C10—H100.9300
C2—H20.9300C11—C121.389 (2)
C3—C41.372 (4)C11—C141.511 (3)
C3—H30.9300C12—H120.9300
C4—C51.366 (4)C13—H13A0.9600
C4—H40.9300C13—H13B0.9600
C5—C61.382 (3)C13—H13C0.9600
C5—H50.9300C14—H14A0.9600
C6—H60.9300C14—H14B0.9600
C7—C81.384 (2)C14—H14C0.9600
C7—C121.386 (2)N1—S11.6302 (15)
C7—N11.435 (2)N1—H1N0.81 (2)
C8—C91.382 (2)O1—S11.4356 (13)
C8—H80.9300O2—S11.4204 (14)
C2—C1—C6121.3 (2)C9—C10—H10118.8
C2—C1—S1119.10 (15)C10—C11—C12118.44 (17)
C6—C1—S1119.64 (16)C10—C11—C14121.40 (19)
C1—C2—C3118.5 (2)C12—C11—C14120.15 (19)
C1—C2—H2120.7C7—C12—C11119.97 (17)
C3—C2—H2120.7C7—C12—H12120.0
C4—C3—C2120.7 (2)C11—C12—H12120.0
C4—C3—H3119.6C9—C13—H13A109.5
C2—C3—H3119.6C9—C13—H13B109.5
C5—C4—C3120.2 (2)H13A—C13—H13B109.5
C5—C4—H4119.9C9—C13—H13C109.5
C3—C4—H4119.9H13A—C13—H13C109.5
C4—C5—C6120.4 (2)H13B—C13—H13C109.5
C4—C5—H5119.8C11—C14—H14A109.5
C6—C5—H5119.8C11—C14—H14B109.5
C1—C6—C5118.9 (2)H14A—C14—H14B109.5
C1—C6—H6120.5C11—C14—H14C109.5
C5—C6—H6120.5H14A—C14—H14C109.5
C8—C7—C12120.60 (16)H14B—C14—H14C109.5
C8—C7—N1119.75 (15)C7—N1—S1120.92 (12)
C12—C7—N1119.56 (16)C7—N1—H1N115.0 (15)
C9—C8—C7120.24 (16)S1—N1—H1N108.7 (15)
C9—C8—H8119.9O2—S1—O1119.88 (9)
C7—C8—H8119.9O2—S1—N1108.03 (8)
C8—C9—C10118.28 (18)O1—S1—N1104.82 (8)
C8—C9—C13120.85 (19)O2—S1—C1108.42 (9)
C10—C9—C13120.87 (18)O1—S1—C1107.56 (9)
C11—C10—C9122.46 (17)N1—S1—C1107.53 (8)
C11—C10—H10118.8
C6—C1—C2—C31.8 (3)C8—C7—C12—C111.4 (3)
S1—C1—C2—C3178.45 (19)N1—C7—C12—C11177.90 (16)
C1—C2—C3—C40.9 (4)C10—C11—C12—C71.5 (3)
C2—C3—C4—C50.8 (4)C14—C11—C12—C7179.70 (19)
C3—C4—C5—C61.7 (4)C8—C7—N1—S1114.44 (16)
C2—C1—C6—C50.9 (3)C12—C7—N1—S169.0 (2)
S1—C1—C6—C5179.33 (19)C7—N1—S1—O248.89 (16)
C4—C5—C6—C10.9 (4)C7—N1—S1—O1177.81 (13)
C12—C7—C8—C90.1 (3)C7—N1—S1—C167.93 (15)
N1—C7—C8—C9176.67 (16)C2—C1—S1—O2148.57 (17)
C7—C8—C9—C100.9 (3)C6—C1—S1—O231.65 (19)
C7—C8—C9—C13178.38 (19)C2—C1—S1—O117.56 (19)
C8—C9—C10—C110.7 (3)C6—C1—S1—O1162.66 (16)
C13—C9—C10—C11178.5 (2)C2—C1—S1—N194.86 (17)
C9—C10—C11—C120.5 (3)C6—C1—S1—N184.93 (18)
C9—C10—C11—C14179.3 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O1i0.81 (2)2.14 (2)2.942 (2)176 (2)
Symmetry code: (i) x+1, y+1/2, z+3/2.

Experimental details

Crystal data
Chemical formulaC14H15NO2S
Mr261.33
Crystal system, space groupMonoclinic, P21/c
Temperature (K)299
a, b, c (Å)11.192 (1), 7.3543 (7), 16.672 (2)
β (°) 101.62 (1)
V3)1344.1 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.23
Crystal size (mm)0.48 × 0.40 × 0.18
Data collection
DiffractometerOxford Diffraction Xcalibur
diffractometer with a Sapphire CCD detector
Absorption correctionMulti-scan
(CrysAlis RED; Oxford Diffraction, 2009)
Tmin, Tmax0.896, 0.959
No. of measured, independent and
observed [I > 2σ(I)] reflections
5063, 2742, 2187
Rint0.015
(sin θ/λ)max1)0.625
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.038, 0.111, 1.05
No. of reflections2742
No. of parameters169
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.31, 0.31

Computer programs: CrysAlis CCD (Oxford Diffraction, 2009), CrysAlis RED (Oxford Diffraction, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O1i0.81 (2)2.14 (2)2.942 (2)176 (2)
Symmetry code: (i) x+1, y+1/2, z+3/2.
 

References

First citationGelbrich, T., Hursthouse, M. B. & Threlfall, T. L. (2007). Acta Cryst. B63, 621–632.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationGowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2008). Acta Cryst. E64, o1691.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationGowda, B. T., Foro, S., Babitha, K. S. & Fuess, H. (2009a). Acta Cryst. E65, o366.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationGowda, B. T., Foro, S., Nirmala, P. G. & Fuess, H. (2009b). Acta Cryst. E65, o2763.  Web of Science CrossRef IUCr Journals Google Scholar
First citationGowda, B. T., Shetty, M. & Jayalakshmi, K. L. (2005). Z. Naturforsch. Teil A, 60, 106–112.  CAS Google Scholar
First citationOxford Diffraction (2009). CrysAlis CCD and CrysAlis RED. Oxford Diffraction Ltd, Yarnton, England.  Google Scholar
First citationPerlovich, G. L., Tkachev, V. V., Schaper, K.-J. & Raevsky, O. A. (2006). Acta Cryst. E62, o780–o782.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSpek, A. L. (2009). Acta Cryst. D65, 148–155.  Web of Science CrossRef CAS IUCr Journals Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds