Literature DB >> 23468813

N-(2-Amino-5-chloro-phen-yl)-2-bromo-benzene-sulfonamide.

Maria Altamura1, Valentina Fedi, Rossano Nannicini, Paola Paoli, Patrizia Rossi.   

Abstract

In the title compound, C12H10BrClN2O2S, the sulfonamide group adopts a staggered conformation about the N-S bond [the C-S-N-H torsion angle is 97 (3)°] with the N-atom lone pair bis-ecting the O=S=O angle. For the C(Ar)-S bond, the ortho-substituted C atom bis-ects one of O=S-N angles [the C-C-S-N torsion angle is -57.7 (3)°]. The mean planes of the aromatic rings form a dihedral angle of 75.1 (1)°. In the crystal, mol-ecules form inversion dimers through pairs of N-H⋯NH2 hydrogen bonds. The mol-ecules are further consolidated into layers along the bc plane by weaker N-H⋯O inter-actions.

Entities:  

Year:  2012        PMID: 23468813      PMCID: PMC3588848          DOI: 10.1107/S160053681204562X

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the synthesis of the title compound, see: Altamura et al. (2009 ▶). For the biological activity of sulfa drugs, see: Chegwidden et al. (2000 ▶); Lu & Tucker (2007 ▶); Tappe et al. (2008 ▶); Purushottamachar et al. (2008 ▶). For structural studies of mol­ecules having the sulfonamideSO2—NH group, see: Parkin et al. (2008 ▶); Perlovich et al. (2009 ▶, 2011 ▶); Vega-Hissi et al. (2011 ▶); Altamura et al. (2009 ▶, 2012 ▶).

Experimental

Crystal data

C12H10BrClN2O2S M = 361.64 Monoclinic, a = 13.657 (1) Å b = 14.361 (2) Å c = 7.0829 (9) Å β = 100.75 (1)° V = 1364.8 (3) Å3 Z = 4 Mo Kα radiation μ = 3.36 mm−1 T = 298 K 0.32 × 0.26 × 0.22 mm

Data collection

Oxford Diffraction Xcalibur3 CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.365, T max = 0.447 6647 measured reflections 2533 independent reflections 1629 reflections with I > 2σ(I) R int = 0.028

Refinement

R[F 2 > 2σ(F 2)] = 0.038 wR(F 2) = 0.082 S = 0.94 2533 reflections 181 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.32 e Å−3 Δρmin = −0.38 e Å−3 Data collection: CrysAlis CCD (Oxford Diffraction, 2006 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2006 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: PARST (Nardelli, 1995 ▶). Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S160053681204562X/ld2080sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681204562X/ld2080Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S160053681204562X/ld2080Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C12H10BrClN2O2SZ = 4
Mr = 361.64F(000) = 720
Monoclinic, P21/cDx = 1.760 Mg m3
a = 13.657 (1) ÅMo Kα radiation, λ = 0.71069 Å
b = 14.361 (2) ŵ = 3.36 mm1
c = 7.0829 (9) ÅT = 298 K
β = 100.75 (1)°Prismatic, colourless
V = 1364.8 (3) Å30.32 × 0.26 × 0.22 mm
Oxford Diffraction Xcalibur3 CCD diffractometer2533 independent reflections
Radiation source: Enhance (Mo) X-ray Source1629 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
Detector resolution: 16.4547 pixels mm-1θmax = 27.3°, θmin = 4.5°
ω scansh = −16→16
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)k = −17→18
Tmin = 0.365, Tmax = 0.447l = −8→8
6647 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.082H atoms treated by a mixture of independent and constrained refinement
S = 0.94w = 1/[σ2(Fo2) + (0.0371P)2] where P = (Fo2 + 2Fc2)/3
2533 reflections(Δ/σ)max < 0.001
181 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = −0.38 e Å3
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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.
xyzUiso*/Ueq
O10.09409 (17)0.35073 (16)0.8889 (4)0.0597 (7)
O20.11627 (17)0.51070 (16)1.0184 (3)0.0530 (6)
S10.13873 (6)0.44073 (6)0.88946 (13)0.0402 (2)
Cl10.37936 (7)0.67877 (7)0.45078 (14)0.0597 (3)
Br10.26467 (3)0.30924 (3)0.61701 (6)0.0772 (2)
C10.2700 (2)0.4257 (2)0.9480 (5)0.0353 (8)
C20.3192 (3)0.4646 (2)1.1197 (5)0.0501 (9)
H20.28420.50221.19120.060*
C30.4190 (3)0.4482 (3)1.1847 (6)0.0648 (11)
H30.45090.47431.30000.078*
C40.4715 (3)0.3937 (3)1.0807 (6)0.0626 (11)
H40.53890.38291.12580.075*
C50.4252 (3)0.3548 (2)0.9097 (6)0.0527 (10)
H50.46110.31830.83800.063*
C60.3248 (2)0.3706 (2)0.8458 (5)0.0419 (8)
C70.1417 (2)0.5706 (2)0.6229 (4)0.0313 (7)
C80.2332 (2)0.5803 (2)0.5710 (4)0.0362 (8)
H80.27420.52860.56970.043*
C90.2643 (2)0.6666 (2)0.5209 (5)0.0373 (8)
C100.2038 (3)0.7433 (2)0.5235 (4)0.0398 (8)
H100.22520.80160.49110.048*
C110.1118 (2)0.7335 (2)0.5742 (4)0.0391 (8)
H110.07120.78540.57450.047*
C120.0789 (2)0.6470 (2)0.6248 (4)0.0292 (7)
N10.1089 (2)0.48048 (18)0.6746 (4)0.0380 (7)
HN10.091 (2)0.443 (2)0.595 (5)0.046*
N2−0.0166 (2)0.6362 (2)0.6676 (4)0.0428 (8)
HN2A−0.045 (3)0.689 (2)0.687 (5)0.051*
HN2B−0.021 (3)0.597 (2)0.750 (5)0.051*
U11U22U33U12U13U23
O10.0480 (14)0.0428 (15)0.088 (2)−0.0138 (13)0.0117 (13)0.0216 (13)
O20.0536 (15)0.0621 (16)0.0470 (15)0.0154 (13)0.0193 (12)−0.0013 (12)
S10.0373 (5)0.0376 (5)0.0473 (5)−0.0003 (4)0.0122 (4)0.0064 (4)
Cl10.0463 (6)0.0695 (7)0.0655 (7)−0.0078 (5)0.0160 (5)0.0115 (5)
Br10.0876 (4)0.0665 (3)0.0700 (3)0.0282 (2)−0.0049 (2)−0.0302 (2)
C10.0377 (19)0.0259 (18)0.043 (2)−0.0002 (15)0.0094 (16)0.0059 (14)
C20.053 (2)0.052 (2)0.044 (2)0.008 (2)0.0050 (18)−0.0004 (17)
C30.062 (3)0.071 (3)0.054 (3)0.001 (2)−0.009 (2)−0.006 (2)
C40.042 (2)0.065 (3)0.077 (3)0.006 (2)0.003 (2)0.012 (2)
C50.048 (2)0.051 (2)0.062 (3)0.009 (2)0.016 (2)0.0096 (19)
C60.044 (2)0.033 (2)0.049 (2)0.0027 (17)0.0091 (17)0.0018 (15)
C70.0335 (19)0.0278 (18)0.0318 (18)−0.0037 (16)0.0040 (14)0.0002 (13)
C80.040 (2)0.0309 (19)0.038 (2)0.0035 (16)0.0072 (15)0.0028 (14)
C90.0369 (19)0.043 (2)0.0308 (19)−0.0014 (17)0.0046 (14)0.0013 (14)
C100.052 (2)0.032 (2)0.034 (2)−0.0057 (18)0.0023 (17)0.0065 (14)
C110.048 (2)0.034 (2)0.0329 (19)0.0083 (18)0.0013 (16)−0.0009 (14)
C120.0305 (18)0.0313 (18)0.0250 (17)0.0009 (16)0.0029 (13)−0.0030 (13)
N10.0424 (17)0.0304 (16)0.0391 (17)−0.0034 (14)0.0021 (13)−0.0018 (12)
N20.0429 (19)0.040 (2)0.046 (2)0.0065 (16)0.0081 (15)−0.0001 (14)
O1—S11.429 (2)C5—H50.9300
O2—S11.429 (2)C7—C81.375 (4)
S1—N11.605 (3)C7—C121.395 (4)
S1—C11.776 (3)C7—N11.438 (4)
Cl1—C91.743 (3)C8—C91.377 (4)
Br1—C61.892 (3)C8—H80.9300
C1—C61.383 (4)C9—C101.379 (4)
C1—C21.392 (4)C10—C111.376 (4)
C2—C31.375 (5)C10—H100.9300
C2—H20.9300C11—C121.390 (4)
C3—C41.366 (5)C11—H110.9300
C3—H30.9300C12—N21.402 (4)
C4—C51.377 (5)N1—HN10.78 (3)
C4—H40.9300N2—HN2A0.87 (3)
C5—C61.380 (4)N2—HN2B0.82 (3)
O1—S1—O2119.70 (16)C8—C7—C12121.0 (3)
O1—S1—N1106.66 (16)C8—C7—N1120.0 (3)
O2—S1—N1108.00 (14)C12—C7—N1119.0 (3)
O1—S1—C1107.58 (14)C7—C8—C9119.9 (3)
O2—S1—C1105.30 (15)C7—C8—H8120.0
N1—S1—C1109.34 (15)C9—C8—H8120.0
C6—C1—C2117.8 (3)C8—C9—C10120.1 (3)
C6—C1—S1124.6 (3)C8—C9—Cl1120.1 (3)
C2—C1—S1117.2 (3)C10—C9—Cl1119.8 (3)
C3—C2—C1120.7 (3)C11—C10—C9120.0 (3)
C3—C2—H2119.7C11—C10—H10120.0
C1—C2—H2119.7C9—C10—H10120.0
C4—C3—C2120.4 (4)C10—C11—C12120.9 (3)
C4—C3—H3119.8C10—C11—H11119.6
C2—C3—H3119.8C12—C11—H11119.6
C3—C4—C5120.4 (4)C11—C12—C7118.1 (3)
C3—C4—H4119.8C11—C12—N2120.9 (3)
C5—C4—H4119.8C7—C12—N2120.9 (3)
C4—C5—C6119.1 (3)C7—N1—S1121.7 (2)
C4—C5—H5120.4C7—N1—HN1120 (3)
C6—C5—H5120.4S1—N1—HN1115 (3)
C5—C6—C1121.6 (3)C12—N2—HN2A114 (2)
C5—C6—Br1116.7 (3)C12—N2—HN2B116 (3)
C1—C6—Br1121.6 (2)HN2A—N2—HN2B112 (3)
HN1—N1—S1—C197 (3)C6—C1—S1—N1−57.7 (3)
HN1—N1—S1—O1−19 (3)C6—C1—S1—O157.8 (3)
C7—N1—S1—O250.2 (3)
D—H···AD—HH···AD···AD—H···A
N1—HN1···N2i0.78 (3)2.26 (3)3.022 (4)166 (3)
N2—HN2A···O1ii0.87 (3)2.45 (3)3.258 (4)154 (3)
Table 1

Selected torsion angles (°)

HN1—N1—S1—C197 (3)
HN1—N1—S1—O1−19 (3)
C7—N1—S1—O250.2 (3)
C6—C1—S1—N1−57.7 (3)
C6—C1—S1—O157.8 (3)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
N1—HN1⋯N2i 0.78 (3)2.26 (3)3.022 (4)166 (3)
N2—HN2A⋯O1ii 0.87 (3)2.45 (3)3.258 (4)154 (3)

Symmetry codes: (i) ; (ii) .

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