Abstract
In the crystal structure of the title compound, C11H13NO5S, the amide C=O and the carboxyl C=O groups of the acid segment orient themselves away from each other. The dihedral angle between the benzene ring and the amide group is 69.0 (2)°. In the crystal, N—H⋯O and O—H⋯O hydrogen bonds link the molecules into layers parallel to the bc plane.
Related literature
For our studies on the effects of substituents on the structures and other aspects of N-(aryl)-amides, see: Gowda et al. (2000 ▶); Saraswathi et al. (2011 ▶), of N-chloroarylamides, see: Gowda & Rao (1989 ▶); Jyothi & Gowda (2004 ▶) and of N-bromoarylsulfonamides, see: Gowda & Mahadevappa (1983 ▶); Usha & Gowda (2006 ▶).
Experimental
Crystal data
C11H13NO5S
M r = 271.28
Monoclinic,
a = 10.2496 (9) Å
b = 17.041 (2) Å
c = 7.4721 (6) Å
β = 101.909 (9)°
V = 1277.0 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.27 mm−1
T = 293 K
0.48 × 0.32 × 0.16 mm
Data collection
Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.883, T max = 0.959
4739 measured reflections
2597 independent reflections
2107 reflections with I > 2σ(I)
R int = 0.014
Refinement
R[F 2 > 2σ(F 2)] = 0.046
wR(F 2) = 0.110
S = 1.12
2597 reflections
170 parameters
2 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.23 e Å−3
Δρmin = −0.32 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 datablock(s) I, global. DOI: 10.1107/S1600536812023276/rz2761sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812023276/rz2761Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812023276/rz2761Isup3.cml
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 | 0.83 (2) | 2.14 (2) | 2.948 (2) | 164 (2) |
| O5—H5O⋯O4ii | 0.83 (2) | 1.83 (2) | 2.663 (3) | 178 (3) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
HP thanks the Department of Science and Technology, Government of India, New Delhi, for a research fellowship under its INSPIRE Program. BTG thanks the University Grants Commission, Government of India, New Delhi, for a special grant under the UGC–BSR one-time grant to faculty.
supplementary crystallographic information
Comment
As part of our studies on the substituent effects on the structures and other aspects of N-(aryl)-amides (Gowda et al., 2000; Saraswathi et al., 2011); N-chloroarylsulfonamides (Gowda & Rao, 1989; Jyothi & Gowda, 2004) and N-bromoaryl- sulfonamides (Gowda & Mahadevappa, 1983; Usha & Gowda, 2006), in the present work, the crystal structure of N-(4-methylphenylsulfonyl)succinamic acid has been determined (Fig. 1). The conformations of the N—H and C=O bonds in the amide segment are anti to each other. Further, the amide C═O and the carboxyl C═O of the acid segment orient themselves away from each other, in contrast to the anti conformation observed between the the amide oxygen and the carboxyl oxygen in N-(4-methylphenyl)-succinamic acid (I) (Saraswathi et al., 2011). But both the amide oxygen and the carboxyl oxygen are anti to the H atoms on the adjacent –CH2 groups, in both the compounds.
In the title compound, the C═O and O—H bonds of the acid group are in syn position to each other, similar to that observed in (I). The molecule is bent at the S-atom with the C1–S1–N1–C7 torsion angle of 79.2 (1)°. Further, the dihedral angle between the phenyl ring and the amide group is 69.0 (2)°. In the crystal, the pairs of O—H···O and N—H···O intermolecular hydrogen bonds link the molecules into layers parallel to the bc plane (Table 1, Fig. 2).
Experimental
Succinic anhydride (0.015 mole) and 4-dimethylaminopyridine (0.01 mole) were added to a solution of p-toluenesulfonamide (0.01 mole) in dichloromethane. The reaction mixture was strirred for 18 h at room temperature and set aside for completion of the reaction. The reaction mixture was concentrated to dryness. The resultant title compound was washed with dilute HCl and then with water thoroughly, to remove the unreacted base and the succinic anhydride. It was recrystallized to constant melting point from ethyl acetate (173–175 °C). The purity of the compound was checked and characterized by its infrared spectrum. Prism-like colourless single crystals used in X-ray diffraction studies were grown by slow evaporation of an ethyl acetate solution at room temperature.
Refinement
The H atoms of the NH group and the OH group were located in a difference Fourier map and later restrained to the distances of N—H = 0.86 (2) Å and O—H = 0.82 (2) Å, respectively. The other H atoms were positioned with idealized geometry using a riding model with the aromatic C—H = 0.93 Å, methyl C—H = 0.96 Å and methylene C—H = 0.97 Å. All H atoms were refined with isotropic displacement parameters set at 1.2 Ueq(C-aromatic, N) and 1.5 Ueq(C-methyl).
Figures
Fig. 1.
The molecular structure of the title compound, showing displacement ellipsoids drawn at the 50% probability level.
Fig. 2.
The molecular packing of the title compound with hydrogen bonding shown as dashed lines.
Crystal data
| C11H13NO5S | F(000) = 568 |
| Mr = 271.28 | Dx = 1.411 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 2495 reflections |
| a = 10.2496 (9) Å | θ = 3.0–27.6° |
| b = 17.041 (2) Å | µ = 0.27 mm−1 |
| c = 7.4721 (6) Å | T = 293 K |
| β = 101.909 (9)° | Prism, colourless |
| V = 1277.0 (2) Å3 | 0.48 × 0.32 × 0.16 mm |
| Z = 4 |
Data collection
| Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector | 2597 independent reflections |
| Radiation source: fine-focus sealed tube | 2107 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.014 |
| Rotation method data acquisition using ω and phi scans | θmax = 26.4°, θmin = 3.0° |
| Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) | h = −12→11 |
| Tmin = 0.883, Tmax = 0.959 | k = −21→8 |
| 4739 measured reflections | l = −9→9 |
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)] = 0.046 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.110 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.12 | w = 1/[σ2(Fo2) + (0.034P)2 + 0.9166P] where P = (Fo2 + 2Fc2)/3 |
| 2597 reflections | (Δ/σ)max = 0.001 |
| 170 parameters | Δρmax = 0.23 e Å−3 |
| 2 restraints | Δρmin = −0.32 e Å−3 |
Special details
| Experimental. Absorption correction: 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 | 0.1649 (2) | 0.82620 (14) | 0.0924 (3) | 0.0398 (5) | |
| C2 | 0.1077 (3) | 0.75638 (15) | 0.0207 (4) | 0.0507 (6) | |
| H2 | 0.1604 | 0.7126 | 0.0132 | 0.061* | |
| C3 | −0.0291 (3) | 0.75296 (17) | −0.0394 (4) | 0.0625 (7) | |
| H3 | −0.0682 | 0.7063 | −0.0881 | 0.075* | |
| C4 | −0.1092 (3) | 0.81770 (18) | −0.0286 (4) | 0.0607 (7) | |
| C5 | −0.0496 (3) | 0.88660 (16) | 0.0469 (4) | 0.0582 (7) | |
| H5 | −0.1025 | 0.9301 | 0.0572 | 0.070* | |
| C6 | 0.0864 (3) | 0.89152 (14) | 0.1068 (4) | 0.0482 (6) | |
| H6 | 0.1255 | 0.9381 | 0.1563 | 0.058* | |
| C7 | 0.3668 (2) | 0.93791 (13) | −0.0993 (3) | 0.0349 (5) | |
| C8 | 0.4086 (2) | 0.94773 (14) | −0.2799 (3) | 0.0394 (5) | |
| H8A | 0.3879 | 0.9001 | −0.3514 | 0.047* | |
| H8B | 0.5042 | 0.9557 | −0.2582 | 0.047* | |
| C9 | 0.3388 (2) | 1.01660 (14) | −0.3874 (3) | 0.0439 (6) | |
| H9A | 0.3582 | 1.0638 | −0.3143 | 0.053* | |
| H9B | 0.3743 | 1.0236 | −0.4971 | 0.053* | |
| C10 | 0.1912 (2) | 1.00645 (14) | −0.4408 (3) | 0.0419 (5) | |
| C11 | −0.2586 (3) | 0.8130 (2) | −0.0975 (6) | 0.0995 (13) | |
| H11A | −0.2856 | 0.7590 | −0.1091 | 0.119* | |
| H11B | −0.2822 | 0.8382 | −0.2147 | 0.119* | |
| H11C | −0.3029 | 0.8389 | −0.0126 | 0.119* | |
| N1 | 0.3902 (2) | 0.86326 (11) | −0.0248 (2) | 0.0387 (4) | |
| H1N | 0.404 (3) | 0.8261 (12) | −0.090 (3) | 0.046* | |
| O1 | 0.39301 (18) | 0.75502 (11) | 0.1880 (2) | 0.0565 (5) | |
| O2 | 0.37311 (18) | 0.89014 (11) | 0.2992 (2) | 0.0558 (5) | |
| O3 | 0.32175 (17) | 0.99012 (10) | −0.0214 (2) | 0.0479 (4) | |
| O4 | 0.13237 (16) | 0.94917 (10) | −0.4003 (3) | 0.0552 (5) | |
| O5 | 0.13192 (19) | 1.06525 (12) | −0.5367 (3) | 0.0672 (6) | |
| H5O | 0.0496 (18) | 1.0596 (19) | −0.557 (4) | 0.081* | |
| S1 | 0.33860 (6) | 0.83267 (4) | 0.15920 (7) | 0.04120 (18) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0465 (13) | 0.0405 (13) | 0.0342 (11) | −0.0018 (10) | 0.0130 (9) | 0.0004 (10) |
| C2 | 0.0567 (15) | 0.0388 (13) | 0.0565 (15) | 0.0028 (12) | 0.0116 (12) | −0.0042 (12) |
| C3 | 0.0639 (18) | 0.0487 (16) | 0.0723 (19) | −0.0113 (14) | 0.0080 (14) | −0.0089 (14) |
| C4 | 0.0482 (15) | 0.0634 (18) | 0.0701 (18) | −0.0024 (13) | 0.0112 (13) | 0.0047 (15) |
| C5 | 0.0537 (16) | 0.0479 (15) | 0.0771 (19) | 0.0076 (13) | 0.0230 (14) | 0.0025 (14) |
| C6 | 0.0562 (15) | 0.0359 (13) | 0.0564 (15) | −0.0021 (11) | 0.0209 (12) | −0.0030 (11) |
| C7 | 0.0315 (11) | 0.0392 (12) | 0.0328 (11) | −0.0044 (9) | 0.0038 (9) | −0.0022 (9) |
| C8 | 0.0365 (12) | 0.0479 (13) | 0.0336 (11) | −0.0005 (10) | 0.0072 (9) | 0.0029 (10) |
| C9 | 0.0405 (12) | 0.0479 (14) | 0.0430 (12) | −0.0051 (11) | 0.0082 (10) | 0.0080 (11) |
| C10 | 0.0464 (13) | 0.0400 (13) | 0.0376 (12) | 0.0007 (11) | 0.0047 (10) | 0.0042 (10) |
| C11 | 0.054 (2) | 0.098 (3) | 0.140 (4) | −0.0050 (19) | 0.003 (2) | −0.001 (3) |
| N1 | 0.0485 (11) | 0.0360 (10) | 0.0341 (10) | 0.0027 (9) | 0.0142 (8) | −0.0011 (8) |
| O1 | 0.0609 (11) | 0.0531 (11) | 0.0559 (11) | 0.0110 (9) | 0.0129 (9) | 0.0202 (9) |
| O2 | 0.0649 (11) | 0.0689 (12) | 0.0326 (8) | −0.0113 (10) | 0.0075 (8) | −0.0062 (8) |
| O3 | 0.0580 (10) | 0.0423 (10) | 0.0467 (9) | 0.0046 (8) | 0.0181 (8) | −0.0041 (8) |
| O4 | 0.0420 (9) | 0.0466 (10) | 0.0718 (12) | −0.0054 (8) | −0.0001 (8) | 0.0162 (9) |
| O5 | 0.0451 (10) | 0.0579 (12) | 0.0924 (15) | 0.0011 (9) | 0.0001 (10) | 0.0301 (11) |
| S1 | 0.0478 (3) | 0.0445 (3) | 0.0315 (3) | −0.0001 (3) | 0.0087 (2) | 0.0046 (2) |
Geometric parameters (Å, º)
| C1—C2 | 1.385 (3) | C8—H8A | 0.9700 |
| C1—C6 | 1.390 (3) | C8—H8B | 0.9700 |
| C1—S1 | 1.750 (2) | C9—C10 | 1.493 (3) |
| C2—C3 | 1.382 (4) | C9—H9A | 0.9700 |
| C2—H2 | 0.9300 | C9—H9B | 0.9700 |
| C3—C4 | 1.387 (4) | C10—O4 | 1.218 (3) |
| C3—H3 | 0.9300 | C10—O5 | 1.307 (3) |
| C4—C5 | 1.388 (4) | C11—H11A | 0.9600 |
| C4—C11 | 1.514 (4) | C11—H11B | 0.9600 |
| C5—C6 | 1.377 (4) | C11—H11C | 0.9600 |
| C5—H5 | 0.9300 | N1—S1 | 1.6559 (19) |
| C6—H6 | 0.9300 | N1—H1N | 0.828 (16) |
| C7—O3 | 1.206 (3) | O1—S1 | 1.4349 (19) |
| C7—N1 | 1.390 (3) | O2—S1 | 1.4234 (18) |
| C7—C8 | 1.507 (3) | O5—H5O | 0.832 (18) |
| C8—C9 | 1.516 (3) | ||
| C2—C1—C6 | 120.8 (2) | H8A—C8—H8B | 107.9 |
| C2—C1—S1 | 119.28 (19) | C10—C9—C8 | 113.14 (19) |
| C6—C1—S1 | 119.88 (19) | C10—C9—H9A | 109.0 |
| C3—C2—C1 | 118.8 (2) | C8—C9—H9A | 109.0 |
| C3—C2—H2 | 120.6 | C10—C9—H9B | 109.0 |
| C1—C2—H2 | 120.6 | C8—C9—H9B | 109.0 |
| C2—C3—C4 | 121.3 (3) | H9A—C9—H9B | 107.8 |
| C2—C3—H3 | 119.3 | O4—C10—O5 | 123.6 (2) |
| C4—C3—H3 | 119.3 | O4—C10—C9 | 123.6 (2) |
| C3—C4—C5 | 118.7 (3) | O5—C10—C9 | 112.9 (2) |
| C3—C4—C11 | 120.5 (3) | C4—C11—H11A | 109.5 |
| C5—C4—C11 | 120.8 (3) | C4—C11—H11B | 109.5 |
| C6—C5—C4 | 121.0 (2) | H11A—C11—H11B | 109.5 |
| C6—C5—H5 | 119.5 | C4—C11—H11C | 109.5 |
| C4—C5—H5 | 119.5 | H11A—C11—H11C | 109.5 |
| C5—C6—C1 | 119.3 (2) | H11B—C11—H11C | 109.5 |
| C5—C6—H6 | 120.3 | C7—N1—S1 | 124.26 (16) |
| C1—C6—H6 | 120.3 | C7—N1—H1N | 120.1 (18) |
| O3—C7—N1 | 122.2 (2) | S1—N1—H1N | 111.6 (18) |
| O3—C7—C8 | 123.9 (2) | C10—O5—H5O | 111 (2) |
| N1—C7—C8 | 113.78 (19) | O2—S1—O1 | 119.62 (11) |
| C7—C8—C9 | 111.76 (19) | O2—S1—N1 | 108.68 (10) |
| C7—C8—H8A | 109.3 | O1—S1—N1 | 103.54 (10) |
| C9—C8—H8A | 109.3 | O2—S1—C1 | 109.68 (11) |
| C7—C8—H8B | 109.3 | O1—S1—C1 | 109.01 (11) |
| C9—C8—H8B | 109.3 | N1—S1—C1 | 105.27 (10) |
| C6—C1—C2—C3 | 1.0 (4) | C8—C9—C10—O4 | 0.8 (3) |
| S1—C1—C2—C3 | −177.0 (2) | C8—C9—C10—O5 | −178.6 (2) |
| C1—C2—C3—C4 | −0.2 (4) | O3—C7—N1—S1 | 10.0 (3) |
| C2—C3—C4—C5 | −0.9 (5) | C8—C7—N1—S1 | −172.55 (15) |
| C2—C3—C4—C11 | 179.2 (3) | C7—N1—S1—O2 | −48.4 (2) |
| C3—C4—C5—C6 | 1.3 (4) | C7—N1—S1—O1 | −176.60 (18) |
| C11—C4—C5—C6 | −178.8 (3) | C7—N1—S1—C1 | 69.0 (2) |
| C4—C5—C6—C1 | −0.5 (4) | C2—C1—S1—O2 | −153.06 (19) |
| C2—C1—C6—C5 | −0.7 (4) | C6—C1—S1—O2 | 28.8 (2) |
| S1—C1—C6—C5 | 177.4 (2) | C2—C1—S1—O1 | −20.3 (2) |
| O3—C7—C8—C9 | −23.2 (3) | C6—C1—S1—O1 | 161.55 (18) |
| N1—C7—C8—C9 | 159.36 (19) | C2—C1—S1—N1 | 90.2 (2) |
| C7—C8—C9—C10 | −63.7 (3) | C6—C1—S1—N1 | −87.9 (2) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O1i | 0.83 (2) | 2.14 (2) | 2.948 (2) | 164 (2) |
| O5—H5O···O4ii | 0.83 (2) | 1.83 (2) | 2.663 (3) | 178 (3) |
Symmetry codes: (i) x, −y+3/2, z−1/2; (ii) −x, −y+2, −z−1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2761).
References
- Gowda, B. T. & Mahadevappa, D. S. (1983). Talanta, 30, 359–362. [DOI] [PubMed]
- Gowda, B. T., Paulus, H. & Fuess, H. (2000). Z. Naturforsch. Teil A, 55, 711–720.
- Gowda, B. T. & Rao, P. J. M. (1989). Bull. Chem. Soc. Jpn, 62, 3303–3310.
- Jyothi, K. & Gowda, B. T. (2004). Z. Naturforsch. Teil A, 59, 64–68.
- Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
- Saraswathi, B. S., Foro, S., Gowda, B. T. & Fuess, H. (2011). Acta Cryst. E67, o227. [DOI] [PMC free article] [PubMed]
- 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]
- Usha, K. M. & Gowda, B. T. (2006). J. Chem. Sci. 118, 351–359.
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/S1600536812023276/rz2761sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812023276/rz2761Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812023276/rz2761Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


