Literature DB >> 21577654

o-Toluene-sulfonamide: a redetermination.

B Thimme Gowda, Sabine Foro, K Shakuntala, Hartmut Fuess.   

Abstract

The structure of the title compound, C(7)H(9)NO(2)S, was previously determined from powder diffraction data [n class="Chemical">Tremayne, Seaton & Glidewell (2002). Acta Cryst. B58, 823-834]. It has now been refined to a significantly higher precision. The amino N-atom is bent with a C-C-S-N torsion angle of -65.8 (2)deg;. In the crystal, mol-ecules are packed into a three-dimensional framework/supramolecular structure through hydrogen bonds between the two H atoms of the sulfonamide group and sulfonyl O atoms of neighbouring mol-ecules.

Entities:  

Year:  2009        PMID: 21577654      PMCID: PMC2970068          DOI: 10.1107/S1600536809033686

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


Related literature

For our studies of the effect of substituents on the solid state structures of sulfonamides, see: Gowda et al. (2003 ▶, 2009 ▶); Gowda, Srilatha et al. (2007 ▶). For the parent benzene­sulfonamide, see: Gowda, Nayak et al. (2007 ▶). For other aryl sulfonamides, see: Gowda et al. (2003 ▶, 2009 ▶); Gowda, Srilatha et al. (2007 ▶); Jones & Weinkauf (1993 ▶); Kumar et al. (1992 ▶); O’Connor & Maslen (1965 ▶). For the powder structure of the title compound, see: Tremayne et al. (2002 ▶).

Experimental

Crystal data

C7H9NO2S M = 171.21 Tetragonal, a = 18.670 (3) Å c = 9.057 (1) Å V = 3157.0 (8) Å3 Z = 16 Cu Kα radiation μ = 3.24 mm−1 T = 299 K 0.40 × 0.35 × 0.02 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.324, T max = 0.938 5320 measured reflections 1403 independent reflections 1290 reflections with I > 2σ(I) R int = 0.059 3 standard reflections frequency: 120 min intensity decay: 1.5%

Refinement

R[F 2 > 2σ(F 2)] = 0.039 wR(F 2) = 0.101 S = 1.07 1403 reflections 108 parameters 2 restraints H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.28 e Å−3 Δρmin = −0.41 e Å−3 Data collection: CAD-4-PC (Enraf–Nonius, 1996 ▶); cell refinement: CAD-4-PC; data reduction: REDU4 (Stoe & Cie, 1987 ▶); 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. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809033686/fl2262sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809033686/fl2262Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C7H9NO2SDx = 1.441 Mg m3
Mr = 171.21Cu Kα radiation, λ = 1.54180 Å
Tetragonal, I41/aCell parameters from 25 reflections
Hall symbol: -I 4adθ = 4.7–17.9°
a = 18.670 (3) ŵ = 3.24 mm1
c = 9.057 (1) ÅT = 299 K
V = 3157.0 (8) Å3Prism, colourless
Z = 160.40 × 0.35 × 0.02 mm
F(000) = 1440
Enraf–Nonius CAD-4 diffractometer1290 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.059
graphiteθmax = 66.8°, θmin = 4.7°
ω/2θ scansh = −22→22
Absorption correction: ψ scan (North et al., 1968)k = −22→22
Tmin = 0.324, Tmax = 0.938l = −10→0
5320 measured reflections3 standard reflections every 120 min
1403 independent reflections intensity decay: 1.5%
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.101w = 1/[σ2(Fo2) + (0.0529P)2 + 2.2812P] where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
1403 reflectionsΔρmax = 0.28 e Å3
108 parametersΔρmin = −0.41 e Å3
2 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00227 (18)
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.
xyzUiso*/Ueq
S10.13337 (2)0.12556 (2)0.26312 (5)0.0365 (2)
O10.20600 (8)0.10124 (10)0.24990 (15)0.0543 (5)
O20.11947 (10)0.20074 (8)0.25836 (16)0.0612 (5)
N10.09068 (10)0.08933 (10)0.13117 (18)0.0454 (4)
H110.0510 (10)0.1073 (12)0.108 (3)0.054*
H120.1053 (12)0.0484 (10)0.107 (3)0.054*
C10.10065 (9)0.09226 (9)0.43325 (19)0.0329 (4)
C20.03095 (11)0.10630 (10)0.4810 (2)0.0395 (5)
C30.01179 (12)0.07885 (12)0.6185 (2)0.0522 (5)
H3−0.03410.08730.65420.063*
C40.05868 (14)0.03960 (13)0.7032 (2)0.0575 (6)
H40.04410.02220.79460.069*
C50.12671 (13)0.02595 (13)0.6539 (2)0.0545 (6)
H50.1583−0.00070.71130.065*
C60.14805 (11)0.05211 (11)0.5179 (2)0.0430 (5)
H60.19400.04290.48320.052*
C7−0.02347 (13)0.14733 (13)0.3939 (3)0.0609 (6)
H7A−0.03440.12180.30470.073*
H7B−0.00460.19370.36950.073*
H7C−0.06630.15290.45150.073*
U11U22U33U12U13U23
S10.0422 (3)0.0384 (3)0.0289 (3)−0.00894 (17)−0.00042 (16)0.00272 (16)
O10.0375 (8)0.0865 (12)0.0388 (8)−0.0106 (7)0.0015 (6)0.0054 (7)
O20.1032 (14)0.0364 (8)0.0441 (9)−0.0154 (8)0.0039 (8)0.0066 (6)
N10.0483 (10)0.0500 (10)0.0378 (9)0.0088 (8)−0.0116 (7)−0.0078 (7)
C10.0401 (10)0.0305 (8)0.0281 (8)−0.0057 (7)−0.0005 (7)−0.0006 (7)
C20.0427 (11)0.0357 (10)0.0401 (10)−0.0035 (8)0.0019 (8)−0.0061 (7)
C30.0541 (13)0.0591 (13)0.0435 (11)−0.0101 (10)0.0151 (9)−0.0081 (9)
C40.0769 (16)0.0612 (14)0.0345 (10)−0.0178 (12)0.0063 (10)0.0060 (10)
C50.0673 (15)0.0549 (13)0.0413 (12)−0.0066 (10)−0.0086 (10)0.0160 (9)
C60.0445 (11)0.0439 (11)0.0405 (10)−0.0014 (8)−0.0025 (8)0.0056 (8)
C70.0474 (12)0.0632 (14)0.0721 (16)0.0123 (11)0.0017 (11)0.0027 (12)
S1—O21.4281 (16)C3—C41.375 (4)
S1—O11.4349 (16)C3—H30.9300
S1—N11.5877 (17)C4—C51.370 (3)
S1—C11.7703 (17)C4—H40.9300
N1—H110.839 (16)C5—C61.384 (3)
N1—H120.841 (16)C5—H50.9300
C1—C61.390 (3)C6—H60.9300
C1—C21.396 (3)C7—H7A0.9600
C2—C31.394 (3)C7—H7B0.9600
C2—C71.497 (3)C7—H7C0.9600
O2—S1—O1118.70 (11)C2—C3—H3119.0
O2—S1—N1107.74 (10)C5—C4—C3120.5 (2)
O1—S1—N1106.07 (9)C5—C4—H4119.8
O2—S1—C1107.98 (9)C3—C4—H4119.8
O1—S1—C1106.72 (8)C4—C5—C6119.4 (2)
N1—S1—C1109.41 (9)C4—C5—H5120.3
S1—N1—H11117.3 (17)C6—C5—H5120.3
S1—N1—H12114.9 (17)C5—C6—C1119.9 (2)
H11—N1—H12126 (2)C5—C6—H6120.1
C6—C1—C2121.59 (17)C1—C6—H6120.1
C6—C1—S1116.72 (15)C2—C7—H7A109.5
C2—C1—S1121.69 (14)C2—C7—H7B109.5
C3—C2—C1116.55 (19)H7A—C7—H7B109.5
C3—C2—C7119.0 (2)C2—C7—H7C109.5
C1—C2—C7124.44 (19)H7A—C7—H7C109.5
C4—C3—C2122.1 (2)H7B—C7—H7C109.5
C4—C3—H3119.0
O2—S1—C1—C6−128.04 (16)S1—C1—C2—C72.5 (3)
O1—S1—C1—C60.61 (17)C1—C2—C3—C4−0.3 (3)
N1—S1—C1—C6114.96 (15)C7—C2—C3—C4178.8 (2)
O2—S1—C1—C251.23 (17)C2—C3—C4—C5−0.2 (3)
O1—S1—C1—C2179.89 (15)C3—C4—C5—C60.1 (4)
N1—S1—C1—C2−65.77 (17)C4—C5—C6—C10.4 (3)
C6—C1—C2—C30.9 (3)C2—C1—C6—C5−0.9 (3)
S1—C1—C2—C3−178.38 (14)S1—C1—C6—C5178.33 (17)
C6—C1—C2—C7−178.2 (2)
D—H···AD—HH···AD···AD—H···A
N1—H11···O2i0.84 (2)2.19 (2)3.003 (2)162 (2)
N1—H12···O1ii0.84 (2)2.14 (2)2.964 (2)167 (2)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H11⋯O2i0.839 (16)2.193 (18)3.003 (2)162 (2)
N1—H12⋯O1ii0.841 (16)2.138 (17)2.964 (2)167 (2)

Symmetry codes: (i) ; (ii) .

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