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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jan 29;67(Pt 2):o536. doi: 10.1107/S1600536811003400

2,2-Dimethyl-N-(2-methyl­phenyl­sulfon­yl)propanamide

K Shakuntala a, Sabine Foro b, B Thimme Gowda a,*
PMCID: PMC3051617  PMID: 21523184

Abstract

In the title compound, C12H17NO3S, the amide H atom is syn to the ortho-methyl group of the benzene ring and the C—S—N—C torsion angle is −65.39 (17)°. The crystal structure features inversion-related dimers linked by pairs of N—H⋯O hydrogen bonds in which the acceptor O atom is bound to the S atom.

Related literature

Sulfonamide drugs contain the sulfanilamide moiety (Maren, 1976). Their tendency and preferences for hydrogen bonding in the solid state can give rise to polymorphism, see: Yang & Guillory (1972); Adsmond & Grant (2001). For our studies on the effect of substituents on the crystal structures of this class of compounds, see: Gowda et al. (2008a,b , 2010). graphic file with name e-67-0o536-scheme1.jpg

Experimental

Crystal data

  • C12H17NO3S

  • M r = 255.33

  • Monoclinic, Inline graphic

  • a = 7.3827 (6) Å

  • b = 21.986 (2) Å

  • c = 8.6060 (8) Å

  • β = 97.158 (9)°

  • V = 1386.0 (2) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 2.06 mm−1

  • T = 299 K

  • 0.30 × 0.25 × 0.25 mm

Data collection

  • Enraf–Nonius CAD-4 diffractometer

  • 3884 measured reflections

  • 2472 independent reflections

  • 2202 reflections with I > 2σ(I)

  • R int = 0.050

  • 3 standard reflections every 120 min intensity decay: 0.5%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.098

  • S = 1.05

  • 2472 reflections

  • 162 parameters

  • 1 restraint

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

  • Δρmax = 0.38 e Å−3

  • Δρmin = −0.35 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.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811003400/tk2712sup1.cif

e-67-0o536-sup1.cif (17.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811003400/tk2712Isup2.hkl

e-67-0o536-Isup2.hkl (121.5KB, 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
N1—H1N⋯O1i 0.82 (2) 2.10 (2) 2.906 (2) 170 (2)

Symmetry code: (i) Inline graphic.

Acknowledgments

KS thanks the University Grants Commission, Government of India, New Delhi, for the award of a research fellowship under its faculty improvement program.

supplementary crystallographic information

Comment

The molecular structures of sulfonamide drugs contain the sulfanilamide moiety (Maren, 1976), and their propensity for hydrogen bonding in the solid state, due to the presence of various hydrogen bond donors and acceptors, can give rise to polymorphism (Yang & Guillory, 1972; Adsmond & Grant, 2001). Hence, the nature and position of substituents play a significant role on the crystal structures of N-(aryl)sulfonoamides. As a part of a study of the substituent effects on the crystal structures of this class of compounds (Gowda et al., 2008a,b, 2010), the structure of N-(2-methylphenylsulfonyl)-2,2,2- trimethylacetamide (I) has been determined.

The N—H and C=O bonds are anti to each other (Fig. 1), as observed in each of N-(phenylsulfonyl)acetamide (II) (Gowda et al., 2010), N-(phenylsulfonyl)-2,2,2-trimethylacetamide (III) (Gowda et al., 2008b) and N-(4-methylphenylsulfonyl)-2,2,2-trimethylacetamide (IV) (Gowda et al., 2008a). Further, the amide hydrogen is syn to the ortho-methyl group in the benzene ring. The molecule in (I) is bent at the S-atom with the C1—S1—N1—C7 torsion angle being -65.39 (17)°, compared to the values of -58.8 (4)° in (II), -64.5 (3)° in (III) and -68.2 (2)° in (IV).

In the crystal structure, the pairs of intermolecular N–H···O hydrogen bonds (Table 1) link inversion-related molecules into dimeric aggregates where the acceptor O atom is bound to the S atom; Fig. 2.

Experimental

Compound (I) was prepared by refluxing 2-methylbenzenesulfonamide (0.10 mole) with an excess of pivalyl chloride (0.20 mole) for about an hour on a water bath. The reaction mixture was cooled and poured into ice cold water. The resulting solid was separated, washed thoroughly with water and dissolved in warm dilute sodium hydrogen carbonate solution.Compound (I) was reprecipitated by acidifying the filtered solution with glacial acetic acid. It was filtered, dried and recrystallized from ethanol. Prism like red crystals were obtained from a slow evaporation of an ethanolic solution of (I).

Refinement

The amide-H atom was located in a difference map and refined with the distance restraint N—H = 0.86 (2) Å. The other H atoms were positioned with idealized geometry using a riding model with C—H = 0.93–0.96 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.

Fig. 1.

Molecular structure of (I), showing the atom- labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Molecular packing for (I) viewed in projection down the a axis. Hydrogen bonds are shown as dashed lines.

Crystal data

C12H17NO3S F(000) = 544
Mr = 255.33 Dx = 1.224 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54180 Å
Hall symbol: -P 2ybc Cell parameters from 25 reflections
a = 7.3827 (6) Å θ = 6.0–21.6°
b = 21.986 (2) Å µ = 2.06 mm1
c = 8.6060 (8) Å T = 299 K
β = 97.158 (9)° Prism, red
V = 1386.0 (2) Å3 0.30 × 0.25 × 0.25 mm
Z = 4

Data collection

Enraf–Nonius CAD-4 diffractometer Rint = 0.050
Radiation source: fine-focus sealed tube θmax = 67.0°, θmin = 4.0°
graphite h = −8→4
ω/2θ scans k = −26→0
3884 measured reflections l = −10→10
2472 independent reflections 3 standard reflections every 120 min
2202 reflections with I > 2σ(I) intensity decay: 0.5%

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)] = 0.037 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.098 w = 1/[σ2(Fo2) + (0.0444P)2 + 0.5143P] where P = (Fo2 + 2Fc2)/3
S = 1.05 (Δ/σ)max = 0.001
2472 reflections Δρmax = 0.38 e Å3
162 parameters Δρmin = −0.35 e Å3
1 restraint Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0174 (8)

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
C1 0.5655 (2) 0.64776 (8) 0.66047 (17) 0.0386 (4)
C2 0.7426 (2) 0.64421 (9) 0.6175 (2) 0.0460 (4)
C3 0.8623 (3) 0.69061 (10) 0.6714 (2) 0.0574 (5)
H3 0.9803 0.6902 0.6443 0.069*
C4 0.8114 (3) 0.73713 (10) 0.7636 (3) 0.0643 (6)
H4 0.8957 0.7669 0.7998 0.077*
C5 0.6366 (3) 0.73991 (10) 0.8024 (3) 0.0637 (6)
H5 0.6026 0.7715 0.8644 0.076*
C6 0.5122 (3) 0.69569 (9) 0.7493 (2) 0.0495 (4)
H6 0.3928 0.6979 0.7728 0.059*
C7 0.2796 (2) 0.62930 (9) 0.32969 (19) 0.0452 (4)
C8 0.2533 (3) 0.61352 (10) 0.1557 (2) 0.0574 (5)
C9 0.4402 (4) 0.60025 (15) 0.1019 (3) 0.0859 (9)
H9A 0.4938 0.5654 0.1569 0.103*
H9B 0.5187 0.6348 0.1237 0.103*
H9C 0.4248 0.5922 −0.0087 0.103*
C10 0.1352 (5) 0.55743 (18) 0.1291 (3) 0.1121 (12)
H10A 0.0191 0.5649 0.1648 0.135*
H10B 0.1942 0.5239 0.1861 0.135*
H10C 0.1173 0.5479 0.0193 0.135*
C11 0.1705 (5) 0.66816 (14) 0.0647 (3) 0.0888 (9)
H11A 0.2493 0.7027 0.0855 0.107*
H11B 0.0532 0.6770 0.0965 0.107*
H11C 0.1566 0.6592 −0.0453 0.107*
C12 0.8070 (3) 0.59462 (12) 0.5168 (3) 0.0670 (6)
H12A 0.7316 0.5940 0.4175 0.080*
H12B 0.7990 0.5561 0.5679 0.080*
H12C 0.9314 0.6022 0.5008 0.080*
N1 0.3642 (2) 0.58401 (7) 0.42600 (16) 0.0439 (4)
H1N 0.403 (3) 0.5529 (8) 0.390 (2) 0.053*
O1 0.49106 (18) 0.53203 (6) 0.66336 (13) 0.0508 (3)
O2 0.24290 (17) 0.60428 (7) 0.68099 (15) 0.0536 (4)
O3 0.2347 (2) 0.67637 (7) 0.38512 (15) 0.0604 (4)
S1 0.40583 (5) 0.588952 (19) 0.61796 (4) 0.03927 (17)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0424 (9) 0.0401 (9) 0.0319 (7) 0.0023 (7) −0.0013 (6) 0.0018 (6)
C2 0.0418 (9) 0.0505 (10) 0.0441 (9) 0.0040 (8) −0.0020 (7) 0.0020 (8)
C3 0.0455 (10) 0.0631 (13) 0.0613 (12) −0.0043 (9) −0.0029 (9) 0.0057 (9)
C4 0.0690 (14) 0.0542 (12) 0.0650 (13) −0.0143 (10) −0.0107 (10) −0.0032 (10)
C5 0.0817 (15) 0.0485 (12) 0.0588 (12) −0.0006 (10) 0.0006 (11) −0.0143 (9)
C6 0.0556 (10) 0.0488 (10) 0.0438 (9) 0.0043 (8) 0.0049 (8) −0.0049 (8)
C7 0.0458 (9) 0.0525 (11) 0.0360 (8) 0.0026 (8) −0.0005 (7) 0.0001 (7)
C8 0.0759 (13) 0.0610 (13) 0.0325 (9) 0.0066 (11) −0.0040 (8) −0.0011 (8)
C9 0.113 (2) 0.102 (2) 0.0456 (12) 0.0371 (17) 0.0222 (13) 0.0108 (12)
C10 0.145 (3) 0.113 (3) 0.0665 (16) −0.038 (2) −0.0314 (17) −0.0137 (16)
C11 0.122 (2) 0.098 (2) 0.0431 (11) 0.0481 (18) −0.0054 (12) 0.0072 (11)
C12 0.0462 (11) 0.0754 (16) 0.0807 (15) 0.0058 (10) 0.0127 (10) −0.0192 (12)
N1 0.0523 (9) 0.0455 (9) 0.0321 (7) 0.0068 (7) −0.0017 (6) −0.0044 (6)
O1 0.0696 (8) 0.0416 (7) 0.0393 (6) 0.0031 (6) −0.0009 (6) 0.0037 (5)
O2 0.0457 (7) 0.0712 (9) 0.0455 (7) −0.0024 (6) 0.0112 (5) −0.0053 (6)
O3 0.0777 (10) 0.0550 (8) 0.0466 (7) 0.0184 (7) 0.0007 (6) −0.0044 (6)
S1 0.0434 (3) 0.0433 (3) 0.0304 (2) 0.00067 (17) 0.00183 (16) −0.00052 (15)

Geometric parameters (Å, °)

C1—C6 1.387 (3) C8—C9 1.537 (3)
C1—C2 1.405 (2) C9—H9A 0.9600
C1—S1 1.7570 (17) C9—H9B 0.9600
C2—C3 1.391 (3) C9—H9C 0.9600
C2—C12 1.506 (3) C10—H10A 0.9600
C3—C4 1.375 (3) C10—H10B 0.9600
C3—H3 0.9300 C10—H10C 0.9600
C4—C5 1.374 (3) C11—H11A 0.9600
C4—H4 0.9300 C11—H11B 0.9600
C5—C6 1.376 (3) C11—H11C 0.9600
C5—H5 0.9300 C12—H12A 0.9600
C6—H6 0.9300 C12—H12B 0.9600
C7—O3 1.203 (2) C12—H12C 0.9600
C7—N1 1.393 (2) N1—S1 1.6459 (14)
C7—C8 1.526 (2) N1—H1N 0.817 (16)
C8—C10 1.511 (4) O1—S1 1.4330 (13)
C8—C11 1.520 (3) O2—S1 1.4204 (13)
C6—C1—C2 121.63 (17) C8—C9—H9C 109.5
C6—C1—S1 116.41 (14) H9A—C9—H9C 109.5
C2—C1—S1 121.78 (14) H9B—C9—H9C 109.5
C3—C2—C1 116.41 (18) C8—C10—H10A 109.5
C3—C2—C12 119.35 (18) C8—C10—H10B 109.5
C1—C2—C12 124.24 (18) H10A—C10—H10B 109.5
C4—C3—C2 122.0 (2) C8—C10—H10C 109.5
C4—C3—H3 119.0 H10A—C10—H10C 109.5
C2—C3—H3 119.0 H10B—C10—H10C 109.5
C5—C4—C3 120.4 (2) C8—C11—H11A 109.5
C5—C4—H4 119.8 C8—C11—H11B 109.5
C3—C4—H4 119.8 H11A—C11—H11B 109.5
C4—C5—C6 119.7 (2) C8—C11—H11C 109.5
C4—C5—H5 120.1 H11A—C11—H11C 109.5
C6—C5—H5 120.1 H11B—C11—H11C 109.5
C5—C6—C1 119.75 (19) C2—C12—H12A 109.5
C5—C6—H6 120.1 C2—C12—H12B 109.5
C1—C6—H6 120.1 H12A—C12—H12B 109.5
O3—C7—N1 120.29 (16) C2—C12—H12C 109.5
O3—C7—C8 125.23 (17) H12A—C12—H12C 109.5
N1—C7—C8 114.48 (16) H12B—C12—H12C 109.5
C10—C8—C11 112.3 (2) C7—N1—S1 124.33 (13)
C10—C8—C7 109.58 (19) C7—N1—H1N 121.7 (15)
C11—C8—C7 108.65 (18) S1—N1—H1N 113.9 (15)
C10—C8—C9 108.8 (3) O2—S1—O1 117.84 (8)
C11—C8—C9 108.3 (2) O2—S1—N1 109.75 (8)
C7—C8—C9 109.25 (17) O1—S1—N1 103.69 (7)
C8—C9—H9A 109.5 O2—S1—C1 108.90 (8)
C8—C9—H9B 109.5 O1—S1—C1 108.99 (8)
H9A—C9—H9B 109.5 N1—S1—C1 107.11 (8)
C6—C1—C2—C3 1.3 (3) N1—C7—C8—C11 −176.7 (2)
S1—C1—C2—C3 −173.65 (13) O3—C7—C8—C9 120.8 (2)
C6—C1—C2—C12 −177.79 (19) N1—C7—C8—C9 −58.8 (2)
S1—C1—C2—C12 7.3 (3) O3—C7—N1—S1 1.5 (3)
C1—C2—C3—C4 0.8 (3) C8—C7—N1—S1 −178.99 (14)
C12—C2—C3—C4 179.9 (2) C7—N1—S1—O2 52.69 (18)
C2—C3—C4—C5 −1.6 (3) C7—N1—S1—O1 179.43 (15)
C3—C4—C5—C6 0.3 (3) C7—N1—S1—C1 −65.39 (17)
C4—C5—C6—C1 1.8 (3) C6—C1—S1—O2 2.45 (16)
C2—C1—C6—C5 −2.6 (3) C2—C1—S1—O2 177.61 (13)
S1—C1—C6—C5 172.59 (15) C6—C1—S1—O1 −127.33 (13)
O3—C7—C8—C10 −120.1 (3) C2—C1—S1—O1 47.82 (15)
N1—C7—C8—C10 60.3 (3) C6—C1—S1—N1 121.08 (14)
O3—C7—C8—C11 2.9 (3) C2—C1—S1—N1 −63.76 (15)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O1i 0.82 (2) 2.10 (2) 2.906 (2) 170 (2)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: TK2712).

References

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  2. Enraf–Nonius (1996). CAD-4-PC Enraf–Nonius, Delft, The Netherlands.
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  4. Gowda, B. T., Foro, S., Sowmya, B. P., Nirmala, P. G. & Fuess, H. (2008a). Acta Cryst. E64, o1274. [DOI] [PMC free article] [PubMed]
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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 datablocks I, global. DOI: 10.1107/S1600536811003400/tk2712sup1.cif

e-67-0o536-sup1.cif (17.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811003400/tk2712Isup2.hkl

e-67-0o536-Isup2.hkl (121.5KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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