Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Mar 26;67(Pt 4):o967. doi: 10.1107/S1600536811010518

2,5-Dichloro­anilinium 4-chloro­benzene­sulfonate

K Shakuntala a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3099771  PMID: 21754230

Abstract

In the crystal of the title compound, C6H6Cl2N+·C6H4ClO3S−, the 2,5-dichloroanilinium cations and 4-chlorobenzenesulfonate anions are located on a crystallographic mirror plane and are connected by N—H⋯O hydrogen bonds. In the crystal, the connectivity of the hydrogen bonds leads to double chains propagating in [010].

Related literature

For the effect of substituents on the oxidative strengths of N-chloro, N-aryl­sulfonamides, see: Gowda et al. (2004a ▶). For their effect on the structures of N-(ar­yl)-amides, see: Gowda et al. (2004b ▶) and of N-(ar­yl)-methane­sulfonamides, see: Gowda et al. (2007 ▶).graphic file with name e-67-0o967-scheme1.jpg

Experimental

Crystal data

  • C6H6Cl2N+·C6H4ClO3S−

  • M r = 354.62

  • Monoclinic, Inline graphic

  • a = 9.792 (1) Å

  • b = 6.802 (1) Å

  • c = 10.879 (1) Å

  • β = 94.26 (1)°

  • V = 722.60 (15) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.78 mm−1

  • T = 293 K

  • 0.40 × 0.34 × 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 = 0.745, T max = 0.834

  • 2700 measured reflections

  • 1603 independent reflections

  • 1439 reflections with I > 2σ(I)

  • R int = 0.012

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.107

  • S = 1.02

  • 1603 reflections

  • 124 parameters

  • 2 restraints

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

  • Δρmax = 0.39 e Å−3

  • Δρmin = −0.39 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/S1600536811010518/bt5496sup1.cif

e-67-0o967-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010518/bt5496Isup2.hkl

e-67-0o967-Isup2.hkl (79KB, 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—H11N⋯O1i 0.88 (2) 1.85 (2) 2.730 (2) 176 (2)
N1—H12N⋯O2ii 0.89 (2) 1.88 (2) 2.753 (3) 170 (3)

Symmetry codes: (i) Inline graphic; (ii) 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 amine and sulfonate moieties are important constituents of many important compounds. As a part of studying the substituent effects on the structures of this class of compounds (Gowda et al., 2004a, 2004b, 2007), in the present work, the crystal structure of 2,5-dichloroanilinium, 4-chlorobenzenesulfonate (I) has been determined (Fig. 1). The title compound showed interesting H-bonding in its crystal structure (Fig. 2). It forms the structure through N—H···O(S) hydrogen bonding. Three H-atoms of the positively charged NH3 group have three O atoms of the negatively charged sulfonate anion as acceptors, with each oxygen forming H-bonding with three H-atoms, one each from three positively charged NH3 groups.

The crystal packing of (I) through N1—H11N···O1, N1—H11aN···O1a and N1—H12N···O2 hydrogen bonding (Table 1) is shown in Fig.2.

Experimental

The solution of chlorobenzene (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 4-chlorobenzenesulfonylchloride was treated with 2,5-dichloroaniline 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 title compound (I) was filtered under suction and washed thoroughly with cold water. It was then recrystallized to constant melting point from dilute ethanol.

Prism like colorless single crystals used in X-ray diffraction studies were grown in ethanolic solution by slow evaporation at room temperature.

Refinement

The N bounded H atoms were 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 C—H = 0.93 Å. All H atoms were refined with isotropic displacement parameters set to 1.2 times of the Ueq of the parent atom.

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.

Fig. 2.

Fig. 2.

Molecular packing in the title compound. Hydrogen bonds are shown as dashed lines.

Crystal data

C6H6Cl2N+·C6H4ClO3S− F(000) = 360
Mr = 354.62 Dx = 1.630 Mg m−3
Monoclinic, P21/m Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yb Cell parameters from 1811 reflections
a = 9.792 (1) Å θ = 2.7–27.8°
b = 6.802 (1) Å µ = 0.78 mm−1
c = 10.879 (1) Å T = 293 K
β = 94.26 (1)° Prism, colourless
V = 722.60 (15) Å3 0.40 × 0.34 × 0.24 mm
Z = 2

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 1603 independent reflections
Radiation source: fine-focus sealed tube 1439 reflections with I > 2σ(I)
graphite Rint = 0.012
Rotation method data acquisition using ω scans θmax = 26.4°, θmin = 2.7°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −12→12
Tmin = 0.745, Tmax = 0.834 k = −8→6
2700 measured reflections l = −13→10

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.107 w = 1/[σ2(Fo2) + (0.0626P)2 + 0.4408P] where P = (Fo2 + 2Fc2)/3
S = 1.02 (Δ/σ)max = 0.023
1603 reflections Δρmax = 0.39 e Å−3
124 parameters Δρmin = −0.39 e Å−3
2 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.036 (4)

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
Cl1 0.87369 (7) 0.7500 0.13209 (9) 0.0577 (3)
S1 0.23468 (6) 0.7500 0.11153 (5) 0.0274 (2)
O1 0.19906 (14) 0.5759 (2) 0.17720 (16) 0.0519 (4)
O2 0.1854 (2) 0.7500 −0.01564 (19) 0.0575 (7)
C1 0.4152 (2) 0.7500 0.1146 (2) 0.0277 (5)
C2 0.4901 (3) 0.7500 0.2257 (3) 0.0740 (15)
H2 0.4454 0.7500 0.2982 0.089*
C3 0.6311 (3) 0.7500 0.2313 (3) 0.0833 (17)
H3 0.6818 0.7500 0.3071 0.100*
C4 0.6952 (3) 0.7500 0.1251 (3) 0.0398 (7)
C5 0.6231 (3) 0.7500 0.0130 (3) 0.0406 (7)
H5 0.6684 0.7500 −0.0592 0.049*
C6 0.4811 (3) 0.7500 0.0082 (3) 0.0372 (6)
H6 0.4307 0.7500 −0.0677 0.045*
Cl2 −0.23538 (8) 0.7500 0.58953 (8) 0.0540 (3)
Cl3 0.39589 (11) 0.7500 0.57932 (12) 0.0947 (5)
N1 −0.0373 (2) 0.7500 0.8143 (2) 0.0293 (5)
H11N −0.0933 (19) 0.852 (3) 0.8172 (19) 0.035*
H12N 0.027 (3) 0.7500 0.876 (2) 0.035*
C7 0.0232 (3) 0.7500 0.6963 (2) 0.0298 (5)
C8 −0.0594 (3) 0.7500 0.5875 (3) 0.0365 (6)
C9 0.0000 (4) 0.7500 0.4767 (3) 0.0487 (8)
H9 −0.0552 0.7500 0.4033 0.058*
C10 0.1392 (4) 0.7500 0.4734 (3) 0.0530 (9)
H10 0.1790 0.7500 0.3984 0.064*
C11 0.2195 (4) 0.7500 0.5822 (3) 0.0504 (8)
C12 0.1633 (3) 0.7500 0.6941 (3) 0.0425 (7)
H12 0.2190 0.7500 0.7672 0.051*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0194 (3) 0.0852 (7) 0.0683 (6) 0.000 0.0028 (3) 0.000
S1 0.0183 (3) 0.0362 (4) 0.0279 (3) 0.000 0.0028 (2) 0.000
O1 0.0376 (8) 0.0493 (9) 0.0692 (10) −0.0112 (7) 0.0078 (7) 0.0157 (8)
O2 0.0271 (10) 0.114 (2) 0.0306 (10) 0.000 −0.0029 (8) 0.000
C1 0.0217 (11) 0.0327 (13) 0.0290 (12) 0.000 0.0029 (9) 0.000
C2 0.0256 (15) 0.167 (5) 0.0293 (14) 0.000 0.0043 (12) 0.000
C3 0.0268 (15) 0.187 (5) 0.0349 (16) 0.000 −0.0058 (13) 0.000
C4 0.0198 (12) 0.0510 (17) 0.0487 (16) 0.000 0.0037 (11) 0.000
C5 0.0269 (13) 0.0555 (18) 0.0406 (15) 0.000 0.0113 (11) 0.000
C6 0.0257 (13) 0.0556 (17) 0.0304 (12) 0.000 0.0033 (10) 0.000
Cl2 0.0422 (4) 0.0676 (6) 0.0495 (5) 0.000 −0.0150 (3) 0.000
Cl3 0.0499 (6) 0.1572 (13) 0.0820 (7) 0.000 0.0370 (5) 0.000
N1 0.0267 (10) 0.0344 (12) 0.0268 (10) 0.000 0.0009 (8) 0.000
C7 0.0338 (13) 0.0290 (13) 0.0267 (12) 0.000 0.0040 (10) 0.000
C8 0.0450 (16) 0.0314 (14) 0.0323 (13) 0.000 −0.0029 (11) 0.000
C9 0.072 (2) 0.0452 (17) 0.0279 (14) 0.000 −0.0037 (14) 0.000
C10 0.078 (2) 0.0502 (19) 0.0336 (15) 0.000 0.0208 (15) 0.000
C11 0.0479 (18) 0.057 (2) 0.0484 (17) 0.000 0.0202 (14) 0.000
C12 0.0368 (15) 0.0563 (19) 0.0348 (14) 0.000 0.0054 (11) 0.000

Geometric parameters (Å, °)

Cl1—C4 1.744 (3) Cl2—C8 1.725 (3)
S1—O2 1.431 (2) Cl3—C11 1.730 (4)
S1—O1i 1.4390 (16) N1—C7 1.453 (3)
S1—O1 1.4390 (16) N1—H11N 0.884 (15)
S1—C1 1.766 (2) N1—H12N 0.886 (18)
C1—C6 1.367 (4) C7—C12 1.373 (4)
C1—C2 1.366 (4) C7—C8 1.383 (4)
C2—C3 1.378 (4) C8—C9 1.377 (4)
C2—H2 0.9300 C9—C10 1.367 (5)
C3—C4 1.355 (5) C9—H9 0.9300
C3—H3 0.9300 C10—C11 1.371 (5)
C4—C5 1.363 (4) C10—H10 0.9300
C5—C6 1.387 (4) C11—C12 1.374 (4)
C5—H5 0.9300 C12—H12 0.9300
C6—H6 0.9300
O2—S1—O1i 113.77 (8) C5—C6—H6 119.9
O2—S1—O1 113.77 (8) C7—N1—H11N 109.0 (14)
O1i—S1—O1 110.72 (14) C7—N1—H12N 111 (2)
O2—S1—C1 106.49 (12) H11N—N1—H12N 112.4 (18)
O1i—S1—C1 105.65 (8) C12—C7—C8 120.5 (3)
O1—S1—C1 105.65 (8) C12—C7—N1 119.2 (2)
C6—C1—C2 119.6 (2) C8—C7—N1 120.3 (2)
C6—C1—S1 121.2 (2) C9—C8—C7 119.4 (3)
C2—C1—S1 119.2 (2) C9—C8—Cl2 119.9 (2)
C1—C2—C3 120.6 (3) C7—C8—Cl2 120.7 (2)
C1—C2—H2 119.7 C10—C9—C8 120.6 (3)
C3—C2—H2 119.7 C10—C9—H9 119.7
C4—C3—C2 119.2 (3) C8—C9—H9 119.7
C4—C3—H3 120.4 C11—C10—C9 119.1 (3)
C2—C3—H3 120.4 C11—C10—H10 120.4
C3—C4—C5 121.4 (3) C9—C10—H10 120.4
C3—C4—Cl1 119.3 (2) C10—C11—C12 121.6 (3)
C5—C4—Cl1 119.3 (2) C10—C11—Cl3 119.6 (3)
C4—C5—C6 119.0 (3) C12—C11—Cl3 118.9 (3)
C4—C5—H5 120.5 C11—C12—C7 118.8 (3)
C6—C5—H5 120.5 C11—C12—H12 120.6
C1—C6—C5 120.2 (3) C7—C12—H12 120.6
C1—C6—H6 119.9
O2—S1—C1—C6 0.0 C4—C5—C6—C1 0.0
O1i—S1—C1—C6 −121.30 (8) C12—C7—C8—C9 0.000 (1)
O1—S1—C1—C6 121.30 (8) N1—C7—C8—C9 180.0
O2—S1—C1—C2 180.0 C12—C7—C8—Cl2 180.0
O1i—S1—C1—C2 58.70 (8) N1—C7—C8—Cl2 0.0
O1—S1—C1—C2 −58.70 (8) C7—C8—C9—C10 0.000 (1)
C6—C1—C2—C3 0.0 Cl2—C8—C9—C10 180.0
S1—C1—C2—C3 180.0 C8—C9—C10—C11 0.0
C1—C2—C3—C4 0.0 C9—C10—C11—C12 0.000 (1)
C2—C3—C4—C5 0.0 C9—C10—C11—Cl3 180.0
C2—C3—C4—Cl1 180.0 C10—C11—C12—C7 0.000 (1)
C3—C4—C5—C6 0.0 Cl3—C11—C12—C7 180.0
Cl1—C4—C5—C6 180.0 C8—C7—C12—C11 0.0
C2—C1—C6—C5 0.0 N1—C7—C12—C11 180.0
S1—C1—C6—C5 180.0

Symmetry codes: (i) x, −y+3/2, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H11N···O1ii 0.88 (2) 1.85 (2) 2.730 (2) 176 (2)
N1—H12N···O2iii 0.89 (2) 1.88 (2) 2.753 (3) 170 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5496).

References

  1. Gowda, B. T., Foro, S. & Fuess, H. (2007). Acta Cryst. E63, o2570.
  2. Gowda, B. T. & Shetty, M. (2004a). J. Phys. Org. Chem. 17, 848–864.
  3. Gowda, B. T., Svoboda, I. & Fuess, H. (2004b). Z. Naturforsch. Teil A, 55, 845–852.
  4. Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
  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/S1600536811010518/bt5496sup1.cif

e-67-0o967-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010518/bt5496Isup2.hkl

e-67-0o967-Isup2.hkl (79KB, hkl)

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

RESOURCES