Abstract
The asymmetric unit of the title compound, C20H24N2O6S2, comprises one half-molecule, the remaining portion being generated via an inversion centre. The dihedral angle between the plane of the benzene ring and the SO2—NH—C(O)—C—C segment is 89.9 (1)°. In the crystal, intermolecular N—H⋯O(S) hydrogen bonds link the molecules into infinite chains in [101].
Related literature
For related structures, see: Gowda et al. (2007 ▶, 2010a ▶,b
▶).
Experimental
Crystal data
C20H24N2O6S2
M r = 452.53
Monoclinic,
a = 11.928 (2) Å
b = 5.523 (1) Å
c = 16.447 (4) Å
β = 96.05 (2)°
V = 1077.5 (4) Å3
Z = 2
Mo Kα radiation
μ = 0.29 mm−1
T = 293 K
0.48 × 0.12 × 0.04 mm
Data collection
Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.875, T max = 0.989
3521 measured reflections
2135 independent reflections
1571 reflections with I > 2σ(I)
R int = 0.037
Refinement
R[F 2 > 2σ(F 2)] = 0.076
wR(F 2) = 0.147
S = 1.31
2135 reflections
140 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.52 e Å−3
Δρmin = −0.29 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/S1600536811007203/vm2082sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811007203/vm2082Isup2.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⋯O1i | 0.84 (2) | 2.09 (2) | 2.917 (4) | 166 (4) |
Symmetry code: (i)
.
Acknowledgments
VZR thanks the University Grants Commission, Government of India, New Delhi, for the award of a research fellowship.
supplementary crystallographic information
Comment
The sulfonamide moiety is an important constituent of many biologically important compounds. As a part of studying the substituent effects on the structures of this class of compounds (Gowda et al., 2007, 2010a,b), in the present work, the structure of N,N-bis(2-methylphenylsulfonyl)-adipamide has been determined (Fig.1). The asymmetric unit comprises half of a molecule, the remaining portion being generated via an inversion centre. The conformation of the N—H and C=O bonds in the C—SO2—NH—C(O)—C—C segment is anti to each other and the amide O atom is also anti to the H atoms attached to the adjacent C atom. Further, the conformation of the N—H bond in the amide fragment is syn to the ortho-methyl group in the adjacent benzene ring. The molecule is bent at the S atom with the C—SO2—NH—C(O) torsion angle of -63.7 (4)°. Further, the S1—N1—C7—C8 and C7—N1—S1—O1 segments are nearly linear. The torsion angles C2—C1—S1—N1 and C6—C1—S1—N1 are -71.3 (4)° and 106.9 (4)°, respectively.
The dihedral angle between the planes of the benzene ring and the SO2—NH—C(O)—C—C segment is 89.9 (1)°.
N—H···O1(S) H-bond formation results in an S=O1 bond longer than the S=O2 bond. A series of N—H···O(S) intermolecular hydrogen bonds (Table 1) link the molecules into infinite chains running in the [101] direction (Fig. 2).
Experimental
N,N-Bis(2-methylphenylsulfonyl)-adipamide was prepared by refluxing a mixture of adipic acid (0.01 mol) with o-toluenesulfonamide (0.02 mol) and POCl3 for 1 hr on a water bath. The reaction mixture was allowed to cool and added ether to it. The solid product obtained was filtered, washed thoroughly with ether and hot ethanol. The compound was recrystallized to the constant melting point and was characterized by its infrared and NMR spectra.
Needle like colorless single crystals used in the X-ray diffraction studies were grown by a slow evaporation of a solution of the compound in ethanol 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 (2) Å. The other H atoms were positioned with idealized geometry using a riding model with ring C—H distance = 0.93 Å, methylene C—H = 0.97 Å and methyl C—H = 0.96 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.
Molecular structure of (I), showing the atom labelling scheme and displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.
Molecular packing of (I) with hydrogen bonding shown as dashed lines.
Crystal data
| C20H24N2O6S2 | F(000) = 476 |
| Mr = 452.53 | Dx = 1.395 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 1186 reflections |
| a = 11.928 (2) Å | θ = 2.9–27.9° |
| b = 5.523 (1) Å | µ = 0.29 mm−1 |
| c = 16.447 (4) Å | T = 293 K |
| β = 96.05 (2)° | Needle, colourless |
| V = 1077.5 (4) Å3 | 0.48 × 0.12 × 0.04 mm |
| Z = 2 |
Data collection
| Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector | 2135 independent reflections |
| Radiation source: fine-focus sealed tube | 1571 reflections with I > 2σ(I) |
| graphite | Rint = 0.037 |
| Rotation method data acquisition using ω scans | θmax = 26.4°, θmin = 3.4° |
| Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) | h = −14→13 |
| Tmin = 0.875, Tmax = 0.989 | k = −5→6 |
| 3521 measured reflections | l = −14→20 |
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)] = 0.076 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.147 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.31 | w = 1/[σ2(Fo2) + (0.0079P)2 + 2.6127P] where P = (Fo2 + 2Fc2)/3 |
| 2135 reflections | (Δ/σ)max = 0.001 |
| 140 parameters | Δρmax = 0.52 e Å−3 |
| 1 restraint | Δρmin = −0.28 e Å−3 |
Special details
| 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 | ||
| S1 | −0.08049 (9) | −0.2084 (2) | 0.23912 (6) | 0.0351 (3) | |
| O1 | −0.1885 (2) | −0.2313 (6) | 0.19216 (18) | 0.0455 (8) | |
| O2 | −0.0301 (3) | −0.4181 (6) | 0.27714 (19) | 0.0516 (9) | |
| O3 | 0.0740 (2) | 0.0040 (6) | 0.37419 (19) | 0.0477 (9) | |
| N1 | −0.1032 (3) | −0.0087 (7) | 0.3094 (2) | 0.0369 (9) | |
| H1N | −0.165 (2) | 0.064 (7) | 0.300 (3) | 0.044* | |
| C1 | 0.0160 (3) | −0.0737 (8) | 0.1790 (3) | 0.0369 (10) | |
| C2 | −0.0143 (4) | 0.1150 (9) | 0.1259 (3) | 0.0482 (12) | |
| C3 | 0.0713 (5) | 0.2137 (13) | 0.0847 (4) | 0.0775 (19) | |
| H3 | 0.0547 | 0.3411 | 0.0485 | 0.093* | |
| C4 | 0.1795 (6) | 0.1268 (15) | 0.0966 (4) | 0.092 (2) | |
| H4 | 0.2356 | 0.1986 | 0.0696 | 0.110* | |
| C5 | 0.2054 (5) | −0.0632 (15) | 0.1476 (4) | 0.082 (2) | |
| H5 | 0.2783 | −0.1248 | 0.1535 | 0.098* | |
| C6 | 0.1249 (4) | −0.1647 (11) | 0.1902 (3) | 0.0589 (15) | |
| H6 | 0.1428 | −0.2924 | 0.2261 | 0.071* | |
| C7 | −0.0216 (3) | 0.0753 (8) | 0.3696 (2) | 0.0324 (9) | |
| C8 | −0.0659 (3) | 0.2492 (8) | 0.4283 (2) | 0.0345 (10) | |
| H8A | −0.1013 | 0.1582 | 0.4691 | 0.041* | |
| H8B | −0.1233 | 0.3495 | 0.3989 | 0.041* | |
| C9 | 0.0242 (3) | 0.4117 (8) | 0.4713 (2) | 0.0361 (10) | |
| H91 | 0.0808 | 0.3124 | 0.5021 | 0.043* | |
| H92 | 0.0608 | 0.5012 | 0.4308 | 0.043* | |
| C10 | −0.1313 (4) | 0.2174 (11) | 0.1094 (3) | 0.0661 (16) | |
| H10A | −0.1779 | 0.1063 | 0.0761 | 0.079* | |
| H10B | −0.1282 | 0.3693 | 0.0814 | 0.079* | |
| H10C | −0.1625 | 0.2418 | 0.1603 | 0.079* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0338 (5) | 0.0381 (6) | 0.0326 (5) | −0.0040 (5) | −0.0005 (4) | −0.0031 (5) |
| O1 | 0.0365 (16) | 0.055 (2) | 0.0431 (17) | −0.0145 (16) | −0.0039 (13) | −0.0087 (16) |
| O2 | 0.064 (2) | 0.041 (2) | 0.049 (2) | 0.0036 (17) | 0.0004 (16) | 0.0035 (17) |
| O3 | 0.0293 (16) | 0.059 (2) | 0.053 (2) | 0.0087 (15) | −0.0038 (13) | −0.0119 (17) |
| N1 | 0.0268 (18) | 0.049 (2) | 0.0343 (19) | 0.0053 (17) | −0.0021 (15) | −0.0065 (18) |
| C1 | 0.031 (2) | 0.045 (3) | 0.035 (2) | −0.005 (2) | 0.0055 (18) | −0.008 (2) |
| C2 | 0.055 (3) | 0.047 (3) | 0.042 (3) | −0.002 (2) | 0.006 (2) | −0.002 (2) |
| C3 | 0.087 (4) | 0.081 (5) | 0.068 (4) | −0.008 (4) | 0.030 (3) | 0.020 (4) |
| C4 | 0.069 (4) | 0.114 (6) | 0.099 (5) | −0.029 (4) | 0.044 (4) | 0.007 (5) |
| C5 | 0.043 (3) | 0.125 (6) | 0.082 (5) | −0.003 (4) | 0.023 (3) | −0.013 (5) |
| C6 | 0.041 (3) | 0.083 (4) | 0.054 (3) | 0.007 (3) | 0.007 (2) | −0.001 (3) |
| C7 | 0.030 (2) | 0.037 (2) | 0.029 (2) | −0.0020 (19) | −0.0008 (17) | 0.0015 (19) |
| C8 | 0.029 (2) | 0.044 (3) | 0.030 (2) | 0.0057 (19) | −0.0005 (16) | −0.002 (2) |
| C9 | 0.034 (2) | 0.041 (3) | 0.033 (2) | −0.001 (2) | −0.0007 (17) | −0.004 (2) |
| C10 | 0.072 (4) | 0.061 (4) | 0.065 (4) | 0.015 (3) | 0.006 (3) | 0.016 (3) |
Geometric parameters (Å, °)
| S1—O2 | 1.419 (3) | C4—H4 | 0.9300 |
| S1—O1 | 1.436 (3) | C5—C6 | 1.368 (8) |
| S1—N1 | 1.641 (4) | C5—H5 | 0.9300 |
| S1—C1 | 1.760 (4) | C6—H6 | 0.9300 |
| O3—C7 | 1.201 (5) | C7—C8 | 1.497 (6) |
| N1—C7 | 1.393 (5) | C8—C9 | 1.516 (6) |
| N1—H1N | 0.843 (19) | C8—H8A | 0.9700 |
| C1—C2 | 1.383 (7) | C8—H8B | 0.9700 |
| C1—C6 | 1.387 (6) | C9—C9i | 1.514 (8) |
| C2—C3 | 1.394 (7) | C9—H91 | 0.9700 |
| C2—C10 | 1.504 (7) | C9—H92 | 0.9700 |
| C3—C4 | 1.372 (9) | C10—H10A | 0.9600 |
| C3—H3 | 0.9300 | C10—H10B | 0.9600 |
| C4—C5 | 1.358 (10) | C10—H10C | 0.9600 |
| O2—S1—O1 | 118.7 (2) | C5—C6—C1 | 118.7 (6) |
| O2—S1—N1 | 109.39 (19) | C5—C6—H6 | 120.6 |
| O1—S1—N1 | 103.45 (18) | C1—C6—H6 | 120.6 |
| O2—S1—C1 | 108.7 (2) | O3—C7—N1 | 121.6 (4) |
| O1—S1—C1 | 109.7 (2) | O3—C7—C8 | 124.5 (4) |
| N1—S1—C1 | 106.1 (2) | N1—C7—C8 | 113.9 (3) |
| C7—N1—S1 | 124.7 (3) | C7—C8—C9 | 113.6 (3) |
| C7—N1—H1N | 120 (3) | C7—C8—H8A | 108.8 |
| S1—N1—H1N | 114 (3) | C9—C8—H8A | 108.8 |
| C2—C1—C6 | 122.4 (4) | C7—C8—H8B | 108.8 |
| C2—C1—S1 | 122.1 (3) | C9—C8—H8B | 108.8 |
| C6—C1—S1 | 115.5 (4) | H8A—C8—H8B | 107.7 |
| C1—C2—C3 | 116.5 (5) | C9i—C9—C8 | 112.0 (4) |
| C1—C2—C10 | 124.9 (4) | C9i—C9—H91 | 109.2 |
| C3—C2—C10 | 118.6 (5) | C8—C9—H91 | 109.2 |
| C4—C3—C2 | 121.4 (6) | C9i—C9—H92 | 109.2 |
| C4—C3—H3 | 119.3 | C8—C9—H92 | 109.2 |
| C2—C3—H3 | 119.3 | H91—C9—H92 | 107.9 |
| C5—C4—C3 | 120.5 (6) | C2—C10—H10A | 109.5 |
| C5—C4—H4 | 119.8 | C2—C10—H10B | 109.5 |
| C3—C4—H4 | 119.8 | H10A—C10—H10B | 109.5 |
| C4—C5—C6 | 120.5 (6) | C2—C10—H10C | 109.5 |
| C4—C5—H5 | 119.7 | H10A—C10—H10C | 109.5 |
| C6—C5—H5 | 119.7 | H10B—C10—H10C | 109.5 |
| O2—S1—N1—C7 | 53.4 (4) | C1—C2—C3—C4 | 0.1 (9) |
| O1—S1—N1—C7 | −179.3 (4) | C10—C2—C3—C4 | −179.4 (6) |
| C1—S1—N1—C7 | −63.7 (4) | C2—C3—C4—C5 | 1.7 (11) |
| O2—S1—C1—C2 | 171.1 (4) | C3—C4—C5—C6 | −2.5 (11) |
| O1—S1—C1—C2 | 39.9 (4) | C4—C5—C6—C1 | 1.5 (10) |
| N1—S1—C1—C2 | −71.3 (4) | C2—C1—C6—C5 | 0.3 (8) |
| O2—S1—C1—C6 | −10.7 (4) | S1—C1—C6—C5 | −177.8 (5) |
| O1—S1—C1—C6 | −141.9 (4) | S1—N1—C7—O3 | −0.2 (6) |
| N1—S1—C1—C6 | 106.9 (4) | S1—N1—C7—C8 | −177.5 (3) |
| C6—C1—C2—C3 | −1.1 (7) | O3—C7—C8—C9 | 25.3 (6) |
| S1—C1—C2—C3 | 176.9 (4) | N1—C7—C8—C9 | −157.5 (4) |
| C6—C1—C2—C10 | 178.4 (5) | C7—C8—C9—C9i | 178.8 (4) |
| S1—C1—C2—C10 | −3.6 (7) |
Symmetry codes: (i) −x, −y+1, −z+1.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O1ii | 0.84 (2) | 2.09 (2) | 2.917 (4) | 166 (4) |
Symmetry codes: (ii) −x−1/2, y+1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: VM2082).
References
- Gowda, B. T., Foro, S. & Fuess, H. (2007). Acta Cryst. E63, o2570.
- Gowda, B. T., Foro, S., Suchetan, P. A. & Fuess, H. (2010a). Acta Cryst. E66, o181. [DOI] [PMC free article] [PubMed]
- Gowda, B. T., Tokarčík, M., Rodrigues, V. Z., Kožíšek, J. & Fuess, H. (2010b). Acta Cryst. E66, o1363. [DOI] [PMC free article] [PubMed]
- Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Abingdon, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- 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/S1600536811007203/vm2082sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811007203/vm2082Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


