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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Apr 18;68(Pt 5):o1403. doi: 10.1107/S1600536812015681

N-(2-Chloro­benzo­yl)-4-methyl­benzene­sulfonamide

P A Suchetan a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3344529  PMID: 22590291

Abstract

In the title compound, C14H12ClNO3S, the C=O bond is syn to the Cl substituent in the adjacent benzene ring. The C—S—N—C torsion angle is −80.6 (6)°. The chloro­benzoyl ring is disordered and was refined using a split model [occupancy ratio 0.537 (3):0.463 (3)]. In the crystal, mol­ecules are linked by pairs of N—H⋯O(S) hydrogen bonds, forming inversion dimers.

Related literature  

For our studies on the effects of substituents on the structures and other aspects of N-(ar­yl)-amides, see: Gowda et al. (2000, 2007), of N-(substitutedbenzo­yl)-aryl­sulfonamides, see: Gowda et al. (2010), of N-chloro­aryl­amides, see: Jyothi & Gowda (2004) and of N-bromo­aryl­sulfonamides, see: Usha & Gowda (2006).graphic file with name e-68-o1403-scheme1.jpg

Experimental  

Crystal data  

  • C14H12ClNO3S

  • M r = 309.76

  • Monoclinic, Inline graphic

  • a = 25.079 (4) Å

  • b = 8.1963 (7) Å

  • c = 18.397 (3) Å

  • β = 131.77 (1)°

  • V = 2820.4 (7) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.42 mm−1

  • T = 293 K

  • 0.48 × 0.20 × 0.16 mm

Data collection  

  • Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) T min = 0.822, T max = 0.935

  • 5253 measured reflections

  • 2432 independent reflections

  • 1623 reflections with I > 2σ(I)

  • R int = 0.033

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.071

  • wR(F 2) = 0.115

  • S = 1.16

  • 2432 reflections

  • 216 parameters

  • 15 restraints

  • H-atom parameters constrained

  • Δρmax = 0.30 e Å−3

  • Δρmin = −0.31 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/S1600536812015681/nc2273sup1.cif

e-68-o1403-sup1.cif (17.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812015681/nc2273Isup2.hkl

e-68-o1403-Isup2.hkl (119.6KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812015681/nc2273Isup3.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 0.86 2.02 2.867 (4) 169

Symmetry code: (i) Inline graphic.

Acknowledgments

BTG thanks the University Grants Commission, Government of India, New Delhi, for a special grant under the UGC–BSR one-time grant to faculty.

supplementary crystallographic information

Comment

As part of our studies on the substituent effects on the structures and other aspects of N-(aryl)-amides (Gowda et al., 2000, 2007), N-(substitutedbenzoyl)-arylsulfonamides (Gowda et al., 2010), N-chloroarylsulfonamides (Jyothi & Gowda, 2004) and N-bromoarylsulfonamides (Usha & Gowda, 2006), in the present work, the crystal structure of N-(2-chlorobenzoyl)-4-methylbenzenesulfonamide (I) has been determined. The conformation of the N—H bond in the C—SO2—NH—C(O) segment is anti to the C=O bond (Fig. 1), similar to that observed in i>N-(2-chlorobenzoyl)-4-chlorobenzenesulfonamide (II)(Gowda et al., 2010). Further, the conformation of the C=O bond in the C—SO2—NH—C(O) segment of (I) is syn to the ortho-Cl in the benzoyl ring, similar to that observed between in (II).

The molecules are twisted at the S atom with the torsional angle of -80.6 (6)°, compared to that of 65.7 (2)° in (II).

The dihedral angle between the sulfonyl benzene ring and the —SO2—NH—C—O segment is 65.0 (5)°, compared to the value of 88.5 (1)° in (II).

Furthermore, the dihedral angle between the sulfonyl and the benzoyl benzene rings is 66.1 (2)°, compared to the value of 58.2 (1)° in (II).

The packing of molecules linked by of N—H···O(S) hydrogen bonds(Table 1) is shown in Fig. 2.

Experimental

The title compound was prepared by refluxing a mixture of 2-chlorobenzoic acid, 4-methylbenzenesulfonamide and phosphorous oxy chloride for 3 h on a water bath. The resultant mixture was cooled and poured into ice cold water. The solid obtained was filtered, washed thoroughly with water and then dissolved in sodium bicarbonate solution. The compound was later reprecipitated by acidifying the filtered solution with dilute HCl. It was filtered, dried and recrystallized.

Prism like colourless single crystals of the title compound used in X-ray diffraction studies were obtained by slow evaporation of the solvent in its toluene solution at room temperature.

Refinement

The H atoms were positioned with idealized geometry using a riding model with C—H distances of 0.93 Å (C-aromatic) and 0.96 Å (C-methyl) and N—H = 0.86 (2) %A.

Uiso(H) values were set at 1.2 Ueq(C-aromatic, N) and 1.5 Ueq(C-methyl).

The chlorobenzyol ring with atoms C8, C9, C10, C11, C12, C13 and CL1 is disordered and was refined using a split model. The corresponding site-occupation factors were refined so that their sum was unity [0.536 (4)–0.464 (4)]. The corresponding bond distances in the disordered groups were restrained to be equal. The C atoms of lower occupancy were refined isotropic.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, showing the atom- labelling scheme. Displacement ellipsoids are drawn at the 50% probability level and disordering is shown as full and dashed lines.

Fig. 2.

Fig. 2.

Molecular packing in the title compound. Hydrogen bonds are shown as dashed lines and the disordering is not shown for clarity.

Crystal data

C14H12ClNO3S F(000) = 1280
Mr = 309.76 Dx = 1.459 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 2528 reflections
a = 25.079 (4) Å θ = 2.5–27.9°
b = 8.1963 (7) Å µ = 0.42 mm1
c = 18.397 (3) Å T = 293 K
β = 131.77 (1)° Prism, colourless
V = 2820.4 (7) Å3 0.48 × 0.20 × 0.16 mm
Z = 8

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 2432 independent reflections
Radiation source: fine-focus sealed tube 1623 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.033
Rotation method data acquisition using ω and phi scans θmax = 25.0°, θmin = 2.7°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −23→29
Tmin = 0.822, Tmax = 0.935 k = −9→7
5253 measured reflections l = −21→19

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)] = 0.071 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.115 H-atom parameters constrained
S = 1.16 w = 1/[σ2(Fo2) + (0.0079P)2 + 10.754P] where P = (Fo2 + 2Fc2)/3
2432 reflections (Δ/σ)max = 0.002
216 parameters Δρmax = 0.30 e Å3
15 restraints Δρmin = −0.31 e Å3

Special details

Experimental. Absorption correction: 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 Occ. (<1)
S1 0.46756 (6) 0.21314 (14) 0.84045 (8) 0.0370 (3)
O1 0.47071 (16) 0.0832 (4) 0.8932 (2) 0.0501 (8)
O2 0.53214 (14) 0.2614 (4) 0.8617 (2) 0.0451 (8)
O3 0.31747 (17) 0.0536 (4) 0.7036 (2) 0.0606 (10)
N1 0.41113 (17) 0.1593 (4) 0.7243 (2) 0.0392 (9)
H1N 0.4221 0.1892 0.6909 0.047*
C1 0.4310 (2) 0.3870 (5) 0.8486 (3) 0.0331 (10)
C2 0.4617 (2) 0.5370 (5) 0.8639 (3) 0.0453 (12)
H2 0.5004 0.5468 0.8677 0.054*
C3 0.4343 (2) 0.6723 (6) 0.8737 (3) 0.0494 (12)
H3 0.4547 0.7741 0.8840 0.059*
C4 0.3767 (2) 0.6586 (6) 0.8682 (3) 0.0408 (11)
C5 0.3469 (2) 0.5060 (6) 0.8526 (3) 0.0475 (12)
H5 0.3079 0.4957 0.8481 0.057*
C6 0.3739 (2) 0.3701 (6) 0.8436 (3) 0.0452 (12)
H6 0.3540 0.2680 0.8343 0.054*
C7 0.3475 (2) 0.0709 (5) 0.6741 (3) 0.0406 (11)
C8 0.3257 (5) −0.0153 (13) 0.5801 (7) 0.030 (3) 0.537 (3)
C9 0.2525 (4) −0.0070 (12) 0.4939 (6) 0.031 (2) 0.537 (3)
C10 0.2260 (5) −0.0831 (12) 0.4066 (6) 0.031 (2) 0.537 (3)
H10 0.1780 −0.0830 0.3496 0.037* 0.537 (3)
C11 0.2799 (5) −0.1586 (11) 0.4153 (6) 0.037 (2) 0.537 (3)
H11 0.2667 −0.2112 0.3605 0.044* 0.537 (3)
C12 0.3534 (6) −0.1611 (11) 0.5014 (7) 0.043 (2) 0.537 (3)
H12 0.3859 −0.2151 0.5011 0.052* 0.537 (3)
C13 0.3767 (6) −0.0868 (14) 0.5831 (8) 0.040 (3) 0.537 (3)
H13 0.4249 −0.0839 0.6389 0.048* 0.537 (3)
Cl1 0.18345 (12) 0.0821 (3) 0.48116 (17) 0.0546 (8) 0.537 (3)
C8' 0.3105 (7) 0.0155 (17) 0.5785 (9) 0.024 (4)* 0.463 (3)
C9' 0.3503 (7) −0.090 (2) 0.5695 (10) 0.041 (5)* 0.463 (3)
C10' 0.3175 (8) −0.158 (2) 0.4767 (11) 0.075 (6)* 0.463 (3)
H10' 0.3420 −0.2235 0.4663 0.089* 0.463 (3)
C11' 0.2470 (8) −0.118 (2) 0.4041 (11) 0.061 (6)* 0.463 (3)
H11' 0.2244 −0.1571 0.3421 0.073* 0.463 (3)
C12' 0.2056 (8) −0.0234 (18) 0.4137 (11) 0.083 (5)* 0.463 (3)
H12' 0.1573 −0.0046 0.3610 0.099* 0.463 (3)
C13' 0.2385 (8) 0.0399 (19) 0.5032 (11) 0.066 (5)* 0.463 (3)
H13' 0.2124 0.0995 0.5134 0.079* 0.463 (3)
Cl1' 0.43803 (18) −0.1591 (4) 0.6657 (3) 0.0793 (13) 0.463 (3)
C14 0.3471 (3) 0.8079 (6) 0.8782 (3) 0.0576 (14)
H14A 0.3478 0.8981 0.8457 0.086*
H14B 0.3757 0.8334 0.9460 0.086*
H14C 0.2987 0.7872 0.8494 0.086*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0378 (6) 0.0369 (6) 0.0381 (6) −0.0007 (6) 0.0260 (5) −0.0026 (5)
O1 0.068 (2) 0.0397 (19) 0.0475 (19) 0.0079 (17) 0.0404 (19) 0.0108 (15)
O2 0.0334 (17) 0.054 (2) 0.0472 (18) −0.0044 (15) 0.0267 (15) −0.0123 (15)
O3 0.055 (2) 0.079 (3) 0.064 (2) −0.0214 (19) 0.046 (2) −0.0109 (19)
N1 0.045 (2) 0.041 (2) 0.038 (2) −0.0101 (18) 0.0304 (19) −0.0067 (17)
C1 0.036 (2) 0.033 (3) 0.034 (2) 0.001 (2) 0.024 (2) 0.0004 (19)
C2 0.046 (3) 0.041 (3) 0.061 (3) −0.008 (2) 0.040 (3) −0.005 (2)
C3 0.058 (3) 0.035 (3) 0.067 (3) −0.009 (2) 0.046 (3) −0.006 (2)
C4 0.045 (3) 0.042 (3) 0.034 (2) 0.009 (2) 0.026 (2) 0.002 (2)
C5 0.048 (3) 0.052 (3) 0.062 (3) −0.004 (3) 0.045 (3) −0.005 (3)
C6 0.053 (3) 0.037 (3) 0.063 (3) −0.006 (2) 0.046 (3) −0.008 (2)
C7 0.036 (3) 0.038 (3) 0.045 (3) −0.007 (2) 0.026 (2) −0.002 (2)
C8 0.024 (5) 0.017 (5) 0.056 (6) 0.010 (4) 0.030 (5) 0.005 (4)
C9 0.034 (5) 0.032 (6) 0.035 (5) 0.001 (4) 0.026 (5) 0.001 (4)
C10 0.024 (5) 0.038 (6) 0.041 (5) 0.007 (4) 0.026 (5) 0.000 (4)
C11 0.028 (5) 0.036 (5) 0.036 (6) 0.006 (4) 0.018 (5) 0.002 (4)
C12 0.050 (7) 0.035 (5) 0.063 (7) 0.006 (5) 0.046 (6) −0.006 (4)
C13 0.041 (7) 0.047 (6) 0.043 (6) −0.006 (6) 0.032 (6) −0.011 (5)
Cl1 0.0510 (16) 0.0559 (16) 0.0613 (16) 0.0102 (12) 0.0392 (14) 0.0080 (12)
Cl1' 0.078 (2) 0.065 (2) 0.110 (3) −0.0042 (18) 0.069 (2) −0.0242 (19)
C14 0.066 (3) 0.054 (3) 0.055 (3) 0.017 (3) 0.041 (3) 0.005 (3)

Geometric parameters (Å, º)

S1—O1 1.407 (3) C9—Cl1 1.745 (9)
S1—O2 1.446 (3) C10—C11 1.397 (12)
S1—N1 1.654 (3) C10—H10 0.9300
S1—C1 1.754 (4) C11—C12 1.420 (12)
O3—C7 1.195 (5) C11—H11 0.9300
N1—C7 1.400 (5) C12—C13 1.342 (11)
N1—H1N 0.8600 C12—H12 0.9300
C1—C2 1.377 (5) C13—H13 0.9300
C1—C6 1.380 (5) C8'—C13' 1.373 (17)
C2—C3 1.378 (6) C8'—C9' 1.412 (15)
C2—H2 0.9300 C9'—C10' 1.423 (16)
C3—C4 1.384 (6) C9'—Cl1' 1.762 (13)
C3—H3 0.9300 C10'—C11' 1.368 (15)
C4—C5 1.385 (6) C10'—H10' 0.9300
C4—C14 1.506 (6) C11'—C12' 1.398 (14)
C5—C6 1.369 (6) C11'—H11' 0.9300
C5—H5 0.9300 C12'—C13' 1.360 (16)
C6—H6 0.9300 C12'—H12' 0.9300
C7—C8' 1.408 (12) C13'—H13' 0.9300
C7—C8 1.589 (11) C14—H14A 0.9600
C8—C13 1.374 (14) C14—H14B 0.9600
C8—C9 1.419 (12) C14—H14C 0.9600
C9—C10 1.410 (12)
O1—S1—O2 118.86 (19) C8—C9—Cl1 126.8 (7)
O1—S1—N1 107.20 (18) C11—C10—C9 112.3 (8)
O2—S1—N1 105.20 (17) C11—C10—H10 123.8
O1—S1—C1 110.41 (19) C9—C10—H10 123.8
O2—S1—C1 108.09 (19) C10—C11—C12 124.9 (7)
N1—S1—C1 106.31 (18) C10—C11—H11 117.5
C7—N1—S1 127.5 (3) C12—C11—H11 117.5
C7—N1—H1N 116.2 C13—C12—C11 121.1 (9)
S1—N1—H1N 116.2 C13—C12—H12 119.5
C2—C1—C6 121.2 (4) C11—C12—H12 119.5
C2—C1—S1 119.3 (3) C12—C13—C8 116.7 (11)
C6—C1—S1 119.5 (3) C12—C13—H13 121.6
C1—C2—C3 119.0 (4) C8—C13—H13 121.6
C1—C2—H2 120.5 C13'—C8'—C7 122.9 (11)
C3—C2—H2 120.5 C13'—C8'—C9' 121.9 (12)
C2—C3—C4 120.8 (4) C7—C8'—C9' 114.5 (10)
C2—C3—H3 119.6 C8'—C9'—C10' 119.3 (12)
C4—C3—H3 119.6 C8'—C9'—Cl1' 125.9 (10)
C3—C4—C5 118.7 (4) C10'—C9'—Cl1' 114.7 (12)
C3—C4—C14 120.1 (4) C11'—C10'—C9' 114.7 (13)
C5—C4—C14 121.1 (4) C11'—C10'—H10' 122.7
C6—C5—C4 121.2 (4) C9'—C10'—H10' 122.7
C6—C5—H5 119.4 C10'—C11'—C12' 126.5 (15)
C4—C5—H5 119.4 C10'—C11'—H11' 116.8
C5—C6—C1 119.0 (4) C12'—C11'—H11' 116.8
C5—C6—H6 120.5 C13'—C12'—C11' 117.5 (15)
C1—C6—H6 120.5 C13'—C12'—H12' 121.3
O3—C7—N1 123.2 (4) C11'—C12'—H12' 121.3
O3—C7—C8' 115.9 (7) C12'—C13'—C8' 119.7 (13)
N1—C7—C8' 120.3 (7) C12'—C13'—H13' 120.1
O3—C7—C8 125.2 (5) C8'—C13'—H13' 120.1
N1—C7—C8 111.3 (5) C4—C14—H14A 109.5
C8'—C7—C8 15.5 (7) C4—C14—H14B 109.5
C13—C8—C9 122.8 (9) H14A—C14—H14B 109.5
C13—C8—C7 120.6 (8) C4—C14—H14C 109.5
C9—C8—C7 116.5 (8) H14A—C14—H14C 109.5
C10—C9—C8 122.0 (8) H14B—C14—H14C 109.5
C10—C9—Cl1 111.1 (6)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O2i 0.86 2.02 2.867 (4) 169

Symmetry code: (i) −x+1, y, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NC2273).

References

  1. Gowda, B. T., Foro, S. & Fuess, H. (2007). Acta Cryst. E63, o1975–o1976.
  2. Gowda, B. T., Foro, S., Suchetan, P. A. & Fuess, H. (2010). Acta Cryst. E66, o1467. [DOI] [PMC free article] [PubMed]
  3. Gowda, B. T., Svoboda, I. & Fuess, H. (2000). Z. Naturforsch. Teil A, 55, 779–790.
  4. Jyothi, K. & Gowda, B. T. (2004). Z. Naturforsch. Teil A, 59, 64–68.
  5. Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  8. Usha, K. M. & Gowda, B. T. (2006). J. Chem. Sci. 118, 351–359.

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/S1600536812015681/nc2273sup1.cif

e-68-o1403-sup1.cif (17.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812015681/nc2273Isup2.hkl

e-68-o1403-Isup2.hkl (119.6KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812015681/nc2273Isup3.cml

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


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