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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 18;67(Pt 7):m926. doi: 10.1107/S1600536811022136

Potassium N-bromo-2-chloro­benzene­sulfonamidate sesquihydrate

B Thimme Gowda a,*, Sabine Foro b, K Shakuntala a
PMCID: PMC3151922  PMID: 21836910

Abstract

In the structure of the title compound, K+·C6H4BrClNO2S·1.5H2O, the K+ ion is hepta­coordinated by three O atoms from water mol­ecules and by four sulfonyl O atoms of N-bromo-2-chloro­benzene­sulfonamidate anions. The S—N distance of 1.582 (4) Å is consistent with an S=N double bond. The crystal structure is stabilized by inter­molecular O—H⋯Br and O—H⋯N hydrogen bonds. The asymmetric unit consits of one potassium cation, one N-bromo-2-chloro­benzene­sulfonamidate anion and one water mol­ecule in general positions and one water mol­ecule located on a twofold rotation axis.

Related literature

For preparation of N-haloaryl­sulfonamides, see: Usha & Gowda (2006). For our study of the effect of substituents on the structures of N-haloaryl­sulfonamides, see: Gowda et al. (2010, 2011a ,b ). For related structures, see: George et al. (2000); Olmstead & Power (1986).graphic file with name e-67-0m926-scheme1.jpg

Experimental

Crystal data

  • K+·C6H4BrClNO2S·1.5H2O

  • M r = 335.65

  • Orthorhombic, Inline graphic

  • a = 12.343 (2) Å

  • b = 52.066 (6) Å

  • c = 6.942 (1) Å

  • V = 4461.3 (11) Å3

  • Z = 16

  • Mo Kα radiation

  • μ = 4.47 mm−1

  • T = 293 K

  • 0.44 × 0.40 × 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 = 0.244, T max = 0.468

  • 4075 measured reflections

  • 1909 independent reflections

  • 1841 reflections with I > 2σ(I)

  • R int = 0.026

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.067

  • S = 1.06

  • 1909 reflections

  • 141 parameters

  • 4 restraints

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

  • Δρmax = 0.42 e Å−3

  • Δρmin = −0.52 e Å−3

  • Absolute structure: Flack (1983), 671 Friedel pairs

  • Flack parameter: 0.019 (9)

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/S1600536811022136/nc2232sup1.cif

e-67-0m926-sup1.cif (19.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022136/nc2232Isup2.hkl

e-67-0m926-Isup2.hkl (94.2KB, hkl)

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
O3—H31⋯N1i 0.80 (2) 2.16 (2) 2.937 (4) 164 (5)
O3—H32⋯Br1ii 0.80 (2) 2.83 (3) 3.574 (3) 156 (4)
O4—H41⋯N1iii 0.82 (2) 2.13 (3) 2.905 (4) 157 (5)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

BTG thanks the University Grants Commission, Government of India, New Delhi, for a UGC-BSR one-time grant to Faculty/Professors.

supplementary crystallographic information

Comment

To explore the effect of replacing sodium by potassium on the solid state structures of N-haloarylsulfonamidates (Gowda et al., 2011a,b), the structure of potassium N-bromo-2-chloro-benzenesulfonamidate sesquihydrate (I) has been determined (Fig. 1). The structure of I resembles those of sodium N-bromo-2-chloro-benzenesulfonamidate sesquihydrate (II) (Gowda et al., 2011b), sodium N-chloro-2-chloro- benzenesulfonamidate sesquihydrate (III)(Gowda et al., 2010), potassium N-chloro-4-chloro-benzenesulfonamidate monohydrate (IV)(Gowda et al., 2011a), and other sodium N-chloro- arylsulfonamidates (George et al., 2000; Olmstead & Power, 1986).

In the structure of the title compound the K+ ion is hepta coordinated by three O atoms from water molecules and by four sulfonyl O atoms of N-bromo-2-chloro-benzenesulfonamide anions. The replacement of Na+ by K+ changes the coordination from hexa to hepta coordination (Gowda et al., 2011b).

The S—N distance of 1.582 (4)Å is consistent with an S—N double bond and is in agreement with the observed values of 1.579 (6) Å in (II), 1.588 (2) Å in (III) and 1.588 (2) Å in (IV)

In the crystal structure two-dimensional polymeric layer are found that are located parallel to the ac plane (Fig. 2). The molecular packing is stabilized by O3—H31···N1, O3—H32···Br1 and O4—H41···N1 hydrogen bonds (Table 1).

Experimental

The title compound was prepared according to the literature method (Usha & Gowda, 2006). The purity of the compound was checked by determining its melting point (176 °). It was characterized by recording its infrared and NMR spectra. Yellow prisms of the title compound used in X-ray diffraction studies were obtained from its aqueous solution at room temperature.

Refinement

The H atoms bound to O atoms were located in difference map and later restrained to O—H = 0.82 (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).

The absolute structure was determined on the basis of 671 Friedel pairs pairs.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, showing the atom labelling scheme for the asymmetric unit and extended to show the coordination geometry for the K+. The displacement ellipsoids are drawn at the 50% probability level. The H atoms are represented as small spheres of arbitrary radii. Symmetry codes: (i) x +1/2, y , z -1/2; (ii) - x +1/2, - y , z -1/2".

Fig. 2.

Fig. 2.

Molecular packing of the title compound with hydrogen bonding shown as dashed lines.

Crystal data

K+·C6H4BrClNO2S·1.5H2O F(000) = 2640
Mr = 335.65 Dx = 1.999 Mg m3
Orthorhombic, Fdd2 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: F 2 -2d Cell parameters from 2515 reflections
a = 12.343 (2) Å θ = 2.9–27.9°
b = 52.066 (6) Å µ = 4.47 mm1
c = 6.942 (1) Å T = 293 K
V = 4461.3 (11) Å3 Prism, yellow
Z = 16 0.44 × 0.40 × 0.20 mm

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 1909 independent reflections
Radiation source: fine-focus sealed tube 1841 reflections with I > 2σ(I)
graphite Rint = 0.026
Rotation method data acquisition using ω scans. θmax = 26.4°, θmin = 3.1°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −8→15
Tmin = 0.244, Tmax = 0.468 k = −56→64
4075 measured reflections l = −8→6

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)] = 0.026 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.067 w = 1/[σ2(Fo2) + (0.0419P)2 + 7.9401P] where P = (Fo2 + 2Fc2)/3
S = 1.06 (Δ/σ)max = 0.002
1909 reflections Δρmax = 0.42 e Å3
141 parameters Δρmin = −0.52 e Å3
4 restraints Absolute structure: Flack (1983), 671 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.019 (9)

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 0.1277 (3) 0.07221 (6) 0.8359 (5) 0.0279 (7)
C2 0.2039 (3) 0.08804 (7) 0.7551 (6) 0.0366 (8)
C3 0.2302 (4) 0.11022 (8) 0.8473 (8) 0.0527 (12)
H3 0.2811 0.1213 0.7935 0.063*
C4 0.1824 (4) 0.11628 (8) 1.0178 (9) 0.0620 (14)
H4 0.2017 0.1315 1.0788 0.074*
C5 0.1081 (4) 0.10099 (9) 1.1015 (8) 0.0568 (13)
H5 0.0766 0.1055 1.2184 0.068*
C6 0.0802 (3) 0.07872 (7) 1.0103 (7) 0.0383 (8)
H6 0.0291 0.0678 1.0655 0.046*
Br1 −0.06844 (3) 0.067404 (8) 0.49856 (7) 0.04826 (13)
Cl1 0.26996 (9) 0.08136 (2) 0.54056 (16) 0.0559 (3)
K1 0.34639 (6) 0.007514 (14) 0.52051 (13) 0.03396 (18)
N1 0.0549 (2) 0.04684 (5) 0.5150 (5) 0.0326 (6)
O1 0.0081 (2) 0.03366 (5) 0.8608 (4) 0.0389 (6)
O2 0.1870 (2) 0.02816 (5) 0.7239 (5) 0.0386 (6)
O3 0.2768 (2) −0.03195 (5) 0.7376 (5) 0.0412 (6)
H31 0.315 (3) −0.0386 (9) 0.817 (6) 0.049*
H32 0.247 (4) −0.0416 (8) 0.666 (6) 0.049*
O4 0.5000 0.0000 0.8095 (6) 0.0466 (10)
H41 0.505 (4) 0.0112 (7) 0.892 (6) 0.056*
S1 0.09016 (6) 0.043209 (13) 0.73226 (12) 0.02646 (17)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0302 (16) 0.0232 (15) 0.0302 (17) 0.0029 (13) −0.0063 (14) 0.0003 (13)
C2 0.0397 (18) 0.0328 (16) 0.037 (2) −0.0047 (13) −0.0093 (19) 0.0048 (18)
C3 0.060 (3) 0.030 (2) 0.068 (3) −0.0135 (19) −0.023 (2) 0.004 (2)
C4 0.078 (3) 0.032 (2) 0.075 (4) 0.001 (2) −0.028 (3) −0.019 (2)
C5 0.073 (3) 0.044 (2) 0.053 (3) 0.019 (2) −0.013 (2) −0.022 (2)
C6 0.048 (2) 0.0327 (17) 0.035 (2) 0.0119 (15) −0.0027 (19) −0.0056 (18)
Br1 0.0399 (2) 0.0498 (2) 0.0551 (3) 0.00658 (16) −0.0060 (2) 0.0135 (2)
Cl1 0.0568 (6) 0.0659 (7) 0.0449 (6) −0.0265 (5) 0.0108 (5) 0.0044 (5)
K1 0.0342 (4) 0.0329 (4) 0.0348 (4) 0.0038 (3) 0.0060 (3) 0.0016 (3)
N1 0.0353 (14) 0.0298 (13) 0.0328 (16) 0.0011 (11) 0.0023 (14) −0.0036 (14)
O1 0.0466 (15) 0.0280 (12) 0.0421 (16) −0.0063 (11) 0.0119 (12) 0.0061 (11)
O2 0.0422 (13) 0.0306 (11) 0.0429 (16) 0.0119 (10) 0.0037 (12) 0.0029 (12)
O3 0.0528 (16) 0.0311 (13) 0.0396 (16) −0.0014 (11) −0.0041 (15) −0.0001 (13)
O4 0.070 (3) 0.038 (2) 0.031 (2) −0.0152 (19) 0.000 0.000
S1 0.0315 (4) 0.0186 (3) 0.0293 (4) 0.0007 (3) 0.0042 (3) 0.0006 (3)

Geometric parameters (Å, °)

C1—C2 1.371 (5) K1—O3ii 2.790 (3)
C1—C6 1.387 (6) K1—O2ii 2.803 (3)
C1—S1 1.736 (3) K1—O1ii 3.008 (3)
C2—C3 1.360 (6) K1—S1ii 3.4047 (11)
C2—Cl1 1.733 (5) K1—H32 3.01 (4)
C3—C4 1.360 (8) N1—S1 1.582 (4)
C3—H3 0.9300 O1—S1 1.438 (3)
C4—C5 1.346 (8) O1—K1iii 2.659 (3)
C4—H4 0.9300 O1—K1iv 3.008 (3)
C5—C6 1.365 (6) O2—S1 1.431 (3)
C5—H5 0.9300 O2—K1iv 2.803 (3)
C6—H6 0.9300 O3—K1iv 2.790 (3)
Br1—N1 1.864 (3) O3—H31 0.804 (19)
K1—O2 2.649 (3) O3—H32 0.796 (19)
K1—O1i 2.659 (3) O4—K1v 2.788 (3)
K1—O3 2.689 (3) O4—H41 0.819 (19)
K1—O4 2.788 (3) S1—K1iv 3.4047 (11)
C2—C1—C6 120.0 (3) O1i—K1—S1ii 88.82 (6)
C2—C1—S1 122.4 (3) O3—K1—S1ii 79.06 (7)
C6—C1—S1 117.5 (3) O4—K1—S1ii 99.07 (5)
C3—C2—C1 118.8 (4) O3ii—K1—S1ii 93.74 (7)
C3—C2—Cl1 117.5 (3) O2ii—K1—S1ii 24.26 (5)
C1—C2—Cl1 123.6 (3) O1ii—K1—S1ii 24.95 (5)
C2—C3—C4 120.2 (4) O2—K1—H32 82.2 (9)
C2—C3—H3 119.9 O1i—K1—H32 151.7 (9)
C4—C3—H3 119.9 O3—K1—H32 14.7 (6)
C5—C4—C3 122.3 (4) O4—K1—H32 85.2 (7)
C5—C4—H4 118.9 O3ii—K1—H32 113.7 (7)
C3—C4—H4 118.9 O2ii—K1—H32 67.9 (6)
C4—C5—C6 118.3 (5) O1ii—K1—H32 76.2 (9)
C4—C5—H5 120.9 S1ii—K1—H32 68.4 (8)
C6—C5—H5 120.9 S1—N1—Br1 110.60 (17)
C5—C6—C1 120.4 (4) S1—O1—K1iii 164.64 (17)
C5—C6—H6 119.8 S1—O1—K1iv 93.13 (13)
C1—C6—H6 119.8 K1iii—O1—K1iv 85.96 (7)
O2—K1—O1i 124.89 (9) S1—O2—K1 149.8 (2)
O2—K1—O3 76.94 (8) S1—O2—K1iv 102.12 (15)
O1i—K1—O3 149.87 (9) K1—O2—K1iv 103.41 (8)
O2—K1—O4 100.27 (10) K1—O3—K1iv 102.72 (8)
O1i—K1—O4 82.02 (8) K1—O3—H31 122 (4)
O3—K1—O4 72.95 (7) K1iv—O3—H31 92 (4)
O2—K1—O3ii 77.62 (10) K1—O3—H32 106 (4)
O1i—K1—O3ii 83.23 (9) K1iv—O3—H32 118 (4)
O3—K1—O3ii 124.66 (5) H31—O3—H32 116 (5)
O4—K1—O3ii 160.21 (6) K1—O4—K1v 87.96 (13)
O2—K1—O2ii 123.44 (5) K1—O4—H41 117 (4)
O1i—K1—O2ii 98.26 (9) K1v—O4—H41 123 (4)
O3—K1—O2ii 81.86 (9) O2—S1—O1 115.10 (17)
O4—K1—O2ii 122.39 (7) O2—S1—N1 104.89 (17)
O3ii—K1—O2ii 72.84 (8) O1—S1—N1 116.06 (16)
O2—K1—O1ii 158.24 (8) O2—S1—C1 105.67 (17)
O1i—K1—O1ii 76.30 (9) O1—S1—C1 103.37 (17)
O3—K1—O1ii 81.53 (9) N1—S1—C1 111.42 (15)
O4—K1—O1ii 76.07 (7) O2—S1—K1iv 53.61 (12)
O3ii—K1—O1ii 113.00 (8) O1—S1—K1iv 61.92 (11)
O2ii—K1—O1ii 49.09 (7) N1—S1—K1iv 135.78 (10)
O2—K1—S1ii 143.01 (7) C1—S1—K1iv 111.69 (11)
C6—C1—C2—C3 −1.1 (5) O1i—K1—O4—K1v −41.28 (6)
S1—C1—C2—C3 −178.8 (3) O3—K1—O4—K1v 121.76 (7)
C6—C1—C2—Cl1 178.7 (3) O3ii—K1—O4—K1v −83.5 (3)
S1—C1—C2—Cl1 0.9 (5) O2ii—K1—O4—K1v 53.47 (8)
C1—C2—C3—C4 0.8 (6) O1ii—K1—O4—K1v 36.50 (6)
Cl1—C2—C3—C4 −178.9 (3) S1ii—K1—O4—K1v 46.24 (2)
C2—C3—C4—C5 −0.2 (7) K1—O2—S1—O1 139.5 (3)
C3—C4—C5—C6 −0.2 (7) K1iv—O2—S1—O1 −7.7 (2)
C4—C5—C6—C1 0.0 (6) K1—O2—S1—N1 10.7 (4)
C2—C1—C6—C5 0.7 (6) K1iv—O2—S1—N1 −136.49 (13)
S1—C1—C6—C5 178.5 (3) K1—O2—S1—C1 −107.1 (3)
O1i—K1—O2—S1 71.6 (4) K1iv—O2—S1—C1 105.67 (15)
O3—K1—O2—S1 −131.4 (3) K1—O2—S1—K1iv 147.2 (4)
O4—K1—O2—S1 159.0 (3) K1iii—O1—S1—O2 −79.1 (7)
O3ii—K1—O2—S1 −1.0 (3) K1iv—O1—S1—O2 7.01 (19)
O2ii—K1—O2—S1 −60.5 (3) K1iii—O1—S1—N1 43.9 (7)
O1ii—K1—O2—S1 −122.9 (3) K1iv—O1—S1—N1 130.04 (12)
S1ii—K1—O2—S1 −80.6 (3) K1iii—O1—S1—C1 166.2 (6)
O1i—K1—O2—K1iv −141.38 (9) K1iv—O1—S1—C1 −107.68 (12)
O3—K1—O2—K1iv 15.65 (9) K1iii—O1—S1—K1iv −86.2 (6)
O4—K1—O2—K1iv −53.99 (9) Br1—N1—S1—O2 −177.66 (15)
O3ii—K1—O2—K1iv 146.08 (11) Br1—N1—S1—O1 54.1 (2)
O2ii—K1—O2—K1iv 86.54 (16) Br1—N1—S1—C1 −63.8 (2)
O1ii—K1—O2—K1iv 24.1 (3) Br1—N1—S1—K1iv 129.71 (11)
S1ii—K1—O2—K1iv 66.47 (16) C2—C1—S1—O2 60.1 (3)
O2—K1—O3—K1iv −15.68 (9) C6—C1—S1—O2 −117.8 (3)
O1i—K1—O3—K1iv 124.69 (15) C2—C1—S1—O1 −178.6 (3)
O4—K1—O3—K1iv 89.55 (10) C6—C1—S1—O1 3.6 (3)
O3ii—K1—O3—K1iv −80.34 (16) C2—C1—S1—N1 −53.3 (3)
O2ii—K1—O3—K1iv −142.87 (10) C6—C1—S1—N1 128.9 (3)
O1ii—K1—O3—K1iv 167.49 (10) C2—C1—S1—K1iv 116.6 (3)
S1ii—K1—O3—K1iv −167.32 (9) C6—C1—S1—K1iv −61.2 (3)
O2—K1—O4—K1v −165.44 (7)

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O3—H31···N1iv 0.80 (2) 2.16 (2) 2.937 (4) 164 (5)
O3—H32···Br1vi 0.80 (2) 2.83 (3) 3.574 (3) 156 (4)
O4—H41···N1vii 0.82 (2) 2.13 (3) 2.905 (4) 157 (5)

Symmetry codes: (iv) −x+1/2, −y, z+1/2; (vi) −x, −y, z; (vii) x+1/2, y, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NC2232).

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/S1600536811022136/nc2232sup1.cif

e-67-0m926-sup1.cif (19.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022136/nc2232Isup2.hkl

e-67-0m926-Isup2.hkl (94.2KB, 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

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