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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Mar 15;67(Pt 4):o884. doi: 10.1107/S1600536811009196

N,N′-Bis(2-chloro­phenyl­sulfon­yl)suberamide

Vinola Z Rodrigues a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3099798  PMID: 21754161

Abstract

In the crystal of the title compound, C20H22Cl2N2O6S2, the asymmetric unit comprises half of a mol­ecule, the remaining portion is generated via an inversion centre. The conformation of the N—H and C=O bonds in the SO2–NH–C(O)–C segment is anti. The mol­ecule is bent at the S atom with the C–SO2–NH–C(O) torsion angle being 68.16 (19)°. The dihedral angle between the plane of the benzene ring and the SO2–NH–C(O)–C segment is 77.5 (1)°. Hydrogen bonds of the type N—H⋯O(C) link mol­ecules into supra­molecular chains along the b axis.

Related literature

For the study of the effect of substituents on the structures of N-(ar­yl)-amides, see: Gowda et al. (2000 ▶). For the effect of substituents in N-(ar­yl)-aryl­sulfonamides, see: Gowda et al. (2005 ▶). For the effect of substituents on the structures of N-(aryl­sulfon­yl)-amides, see: Rodrigues et al. (2011 ▶).graphic file with name e-67-0o884-scheme1.jpg

Experimental

Crystal data

  • C20H22Cl2N2O6S2

  • M r = 521.42

  • Monoclinic, Inline graphic

  • a = 7.8737 (9) Å

  • b = 9.717 (1) Å

  • c = 14.616 (2) Å

  • β = 94.575 (9)°

  • V = 1114.7 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.52 mm−1

  • T = 293 K

  • 0.36 × 0.22 × 0.10 mm

Data collection

  • Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.835, T max = 0.950

  • 4126 measured reflections

  • 2276 independent reflections

  • 1744 reflections with I > 2σ(I)

  • R int = 0.018

Refinement

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.104

  • S = 1.05

  • 2276 reflections

  • 148 parameters

  • 1 restraint

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

  • Δρmax = 0.32 e Å−3

  • Δρmin = −0.33 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 datablocks I, global. DOI: 10.1107/S1600536811009196/tk2727sup1.cif

e-67-0o884-sup1.cif (16.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009196/tk2727Isup2.hkl

e-67-0o884-Isup2.hkl (111.9KB, hkl)

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⋯O3i 0.83 (2) 2.20 (2) 3.020 (2) 172 (2)

Symmetry code: (i) Inline graphic.

Acknowledgments

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

supplementary crystallographic information

Comment

The amide and sulfonamide moieties are important constituents of many biologically significant compounds. As part of an investigation studying the effect of substituents on the structures of this class of compounds (Gowda et al., 2000, 2005; Rodrigues et al., 2011), in the present work, the structure of N,N-bis(2-chlorophenylsulfonyl)-suberamide (I) has been determined (Fig. 1). The asymmetric unit comprises half of a molecule, the remaining portion is generated through an inversion centre, similar to that observed in N,N-bis(2-chlorophenylsulfonyl)-adipamide (II) (Rodrigues et al., 2011). The conformation of the N—H and C═O bonds in the SO2—NH—C(═O)—C segment is anti. The molecule is bent at the S atom with the C—SO2—NH—C(═O) torsion angle being 68.16 (19) °, compared to the value of -65.1 (6)° in (II). The torsion angles C2—C1—S1—N1 and C6—C1—S1—N1 are, respectively, 70.6 (2)° and -113.32 (17)°. The corresponding values in (II) are -69.5 (6) ° and 108.8 (5) °, respectively. The dihedral angle between the planes of the benzene ring and the SO2—NH—C(═O)—C segment in (I) is 77.5 (1) °, compared to the value of 89.6 (2) ° in (II).

A series of N—H···O(C) intermolecular hydrogen bonds (Table 1) link the molecules into chains running along the b axis (Fig. 2).

Experimental

Compound (I) was prepared by refluxing a mixture of suberic acid (0.01 mol) with 2-chlorobenzenesulfonamide (0.02 mol) and POCl3 for 1 h on a water bath. The reaction mixture was allowed to cool and diethyl ether added. The solid product obtained was filtered, washed thoroughly with ether and hot ethanol. The compound was recrystallized to a constant melting point. Colourless prisms were grown by the slow evaporation of its ethanol solution 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±0.02 Å. The other H atoms were positioned with idealized geometry using a riding model with aromati-C—H distance = 0.93 Å, and methylene-C—H = 0.97 Å. All H atoms were refined with Uiso(H) = 1.2Ueq(N,C).

Figures

Fig. 1.

Fig. 1.

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

Fig. 2.

Fig. 2.

Molecular packing of (I) viewed in projection down the a axis and with hydrogen bonding shown as dashed lines.

Crystal data

C20H22Cl2N2O6S2 F(000) = 540
Mr = 521.42 Dx = 1.553 Mg m−3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 1476 reflections
a = 7.8737 (9) Å θ = 2.6–27.7°
b = 9.717 (1) Å µ = 0.52 mm−1
c = 14.616 (2) Å T = 293 K
β = 94.575 (9)° Prism, colourless
V = 1114.7 (2) Å3 0.36 × 0.22 × 0.10 mm
Z = 2

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 2276 independent reflections
Radiation source: fine-focus sealed tube 1744 reflections with I > 2σ(I)
graphite Rint = 0.018
Rotation method data acquisition using ω scans θmax = 26.4°, θmin = 2.6°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −9→9
Tmin = 0.835, Tmax = 0.950 k = −11→12
4126 measured reflections l = −18→8

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) = 0.104 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0588P)2 + 0.1117P] where P = (Fo2 + 2Fc2)/3
2276 reflections (Δ/σ)max = 0.001
148 parameters Δρmax = 0.32 e Å−3
1 restraint Δρmin = −0.33 e Å−3

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
C1 0.3294 (3) −0.0856 (2) 0.61075 (13) 0.0301 (5)
C2 0.2763 (3) −0.0520 (2) 0.52035 (14) 0.0329 (5)
C3 0.3042 (3) −0.1437 (3) 0.45110 (15) 0.0449 (6)
H3 0.2664 −0.1228 0.3908 0.054*
C4 0.3873 (4) −0.2654 (3) 0.47050 (17) 0.0499 (7)
H4 0.4073 −0.3258 0.4232 0.060*
C5 0.4412 (3) −0.2986 (3) 0.55920 (18) 0.0479 (6)
H5 0.4977 −0.3813 0.5719 0.057*
C6 0.4118 (3) −0.2096 (2) 0.62958 (16) 0.0381 (5)
H6 0.4473 −0.2327 0.6898 0.046*
C7 0.0104 (3) −0.0734 (2) 0.75061 (14) 0.0306 (5)
C8 −0.1521 (3) −0.0352 (2) 0.79001 (14) 0.0347 (5)
H8A −0.2460 −0.0863 0.7594 0.042*
H8B −0.1743 0.0622 0.7808 0.042*
C9 −0.1371 (3) −0.0685 (2) 0.89303 (14) 0.0385 (6)
H9A −0.2477 −0.0554 0.9167 0.046*
H9B −0.1066 −0.1647 0.9011 0.046*
C10 −0.0071 (3) 0.0185 (3) 0.94906 (14) 0.0394 (6)
H10A −0.0384 0.1147 0.9422 0.047*
H10B 0.1034 0.0065 0.9252 0.047*
N1 0.1046 (2) 0.03505 (19) 0.72033 (12) 0.0316 (4)
H1N 0.066 (3) 0.1134 (18) 0.7259 (16) 0.038*
O1 0.3959 (2) −0.03761 (18) 0.78343 (10) 0.0456 (4)
O2 0.3555 (2) 0.16371 (17) 0.68236 (10) 0.0415 (4)
O3 0.0630 (2) −0.19135 (16) 0.74794 (11) 0.0437 (4)
Cl1 0.17624 (9) 0.10214 (7) 0.49044 (4) 0.0505 (2)
S1 0.31012 (7) 0.02626 (6) 0.70503 (3) 0.03155 (17)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0299 (11) 0.0338 (12) 0.0268 (10) −0.0019 (9) 0.0051 (8) −0.0017 (9)
C2 0.0336 (12) 0.0347 (12) 0.0305 (11) −0.0013 (10) 0.0026 (9) 0.0015 (9)
C3 0.0513 (15) 0.0557 (16) 0.0275 (11) −0.0037 (13) 0.0025 (11) −0.0034 (11)
C4 0.0576 (17) 0.0482 (16) 0.0459 (14) −0.0019 (13) 0.0167 (12) −0.0152 (12)
C5 0.0488 (16) 0.0374 (14) 0.0586 (16) 0.0075 (11) 0.0113 (13) −0.0039 (12)
C6 0.0377 (13) 0.0377 (13) 0.0390 (12) 0.0018 (10) 0.0038 (10) 0.0024 (10)
C7 0.0389 (12) 0.0300 (12) 0.0232 (9) −0.0026 (10) 0.0040 (9) −0.0009 (9)
C8 0.0356 (12) 0.0334 (12) 0.0353 (12) −0.0025 (10) 0.0045 (9) 0.0021 (10)
C9 0.0441 (14) 0.0399 (14) 0.0329 (12) −0.0059 (11) 0.0123 (10) −0.0002 (10)
C10 0.0453 (14) 0.0409 (14) 0.0335 (12) −0.0062 (11) 0.0125 (10) −0.0010 (10)
N1 0.0384 (11) 0.0264 (10) 0.0310 (9) 0.0014 (8) 0.0092 (8) 0.0012 (8)
O1 0.0493 (11) 0.0561 (11) 0.0298 (8) 0.0067 (8) −0.0074 (7) −0.0001 (8)
O2 0.0447 (10) 0.0362 (9) 0.0440 (9) −0.0111 (7) 0.0068 (7) −0.0030 (7)
O3 0.0529 (11) 0.0277 (9) 0.0527 (10) 0.0006 (8) 0.0187 (8) −0.0006 (7)
Cl1 0.0632 (4) 0.0445 (4) 0.0418 (3) 0.0062 (3) −0.0077 (3) 0.0065 (3)
S1 0.0340 (3) 0.0352 (3) 0.0253 (3) −0.0016 (2) 0.0016 (2) −0.0017 (2)

Geometric parameters (Å, °)

C1—C6 1.385 (3) C7—C8 1.492 (3)
C1—C2 1.393 (3) C8—C9 1.535 (3)
C1—S1 1.771 (2) C8—H8A 0.9700
C2—C3 1.379 (3) C8—H8B 0.9700
C2—Cl1 1.732 (2) C9—C10 1.516 (3)
C3—C4 1.370 (4) C9—H9A 0.9700
C3—H3 0.9300 C9—H9B 0.9700
C4—C5 1.370 (4) C10—C10i 1.527 (4)
C4—H4 0.9300 C10—H10A 0.9700
C5—C6 1.378 (3) C10—H10B 0.9700
C5—H5 0.9300 N1—S1 1.6532 (19)
C6—H6 0.9300 N1—H1N 0.826 (16)
C7—O3 1.221 (3) O1—S1 1.4250 (16)
C7—N1 1.381 (3) O2—S1 1.4282 (17)
C6—C1—C2 119.5 (2) C7—C8—H8B 109.9
C6—C1—S1 116.55 (16) C9—C8—H8B 109.9
C2—C1—S1 123.79 (17) H8A—C8—H8B 108.3
C3—C2—C1 119.4 (2) C10—C9—C8 114.08 (18)
C3—C2—Cl1 118.01 (18) C10—C9—H9A 108.7
C1—C2—Cl1 122.59 (17) C8—C9—H9A 108.7
C4—C3—C2 120.5 (2) C10—C9—H9B 108.7
C4—C3—H3 119.8 C8—C9—H9B 108.7
C2—C3—H3 119.8 H9A—C9—H9B 107.6
C5—C4—C3 120.4 (2) C9—C10—C10i 112.9 (2)
C5—C4—H4 119.8 C9—C10—H10A 109.0
C3—C4—H4 119.8 C10i—C10—H10A 109.0
C4—C5—C6 120.1 (2) C9—C10—H10B 109.0
C4—C5—H5 120.0 C10i—C10—H10B 109.0
C6—C5—H5 120.0 H10A—C10—H10B 107.8
C5—C6—C1 120.1 (2) C7—N1—S1 124.07 (16)
C5—C6—H6 119.9 C7—N1—H1N 117.4 (17)
C1—C6—H6 119.9 S1—N1—H1N 115.6 (17)
O3—C7—N1 120.9 (2) O1—S1—O2 118.86 (10)
O3—C7—C8 123.3 (2) O1—S1—N1 108.65 (10)
N1—C7—C8 115.66 (19) O2—S1—N1 104.39 (10)
C7—C8—C9 108.97 (18) O1—S1—C1 107.08 (11)
C7—C8—H8A 109.9 O2—S1—C1 110.79 (10)
C9—C8—H8A 109.9 N1—S1—C1 106.41 (10)
C6—C1—C2—C3 1.0 (3) C7—C8—C9—C10 66.2 (3)
S1—C1—C2—C3 176.93 (18) C8—C9—C10—C10i −179.1 (2)
C6—C1—C2—Cl1 −178.69 (17) O3—C7—N1—S1 −17.2 (3)
S1—C1—C2—Cl1 −2.8 (3) C8—C7—N1—S1 160.00 (15)
C1—C2—C3—C4 −1.7 (4) C7—N1—S1—O1 −46.8 (2)
Cl1—C2—C3—C4 178.1 (2) C7—N1—S1—O2 −174.61 (16)
C2—C3—C4—C5 1.1 (4) C7—N1—S1—C1 68.16 (19)
C3—C4—C5—C6 0.1 (4) C6—C1—S1—O1 2.7 (2)
C4—C5—C6—C1 −0.7 (4) C2—C1—S1—O1 −173.29 (18)
C2—C1—C6—C5 0.2 (3) C6—C1—S1—O2 133.79 (17)
S1—C1—C6—C5 −176.03 (19) C2—C1—S1—O2 −42.2 (2)
O3—C7—C8—C9 64.1 (3) C6—C1—S1—N1 −113.32 (17)
N1—C7—C8—C9 −113.0 (2) C2—C1—S1—N1 70.6 (2)

Symmetry codes: (i) −x, −y, −z+2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O3ii 0.83 (2) 2.20 (2) 3.020 (2) 172 (2)

Symmetry codes: (ii) −x, y+1/2, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: TK2727).

References

  1. Gowda, B. T., Paulus, H. & Fuess, H. (2000). Z. Naturforsch. Teil A, 55, 791–800.
  2. Gowda, B. T., Shetty, M. & Jayalakshmi, K. L. (2005). Z. Naturforsch. Teil A, 60, 106–112.
  3. Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, Oxfordshire, England.
  4. Rodrigues, V. Z., Foro, S. & Gowda, B. T. (2011). Acta Cryst. E67, o837. [DOI] [PMC free article] [PubMed]
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. 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/S1600536811009196/tk2727sup1.cif

e-67-0o884-sup1.cif (16.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009196/tk2727Isup2.hkl

e-67-0o884-Isup2.hkl (111.9KB, hkl)

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


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