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Acta Cryst. (2009). E65, o1204    [ doi:10.1107/S160053680901616X ]

Methyl 2-(benzenesulfonamido)acetate

M. N. Arshad, I. U. Khan, M. Zia-ur-Rehman and M. Shafiq

Abstract top

The title compound, C9H11NO4S, is of interest as a precursor to biologically active benzothiazines. The crystal structure is stabilized by intermolecular N-H...O and C-H...O interactions.

Comment top

Sulfonamide is an important functionality found in many naturally occurring as well as synthetic compounds which possess numerous types of biological activities (Soledade et al., 2006; Esteve & Bidal, 2002; Xiao & Timberlake, 2000; Martinez et al., 2000; Berredjem et al., 2000; Lee & Lee, 2002). In the present paper, the structure of the title compound has been determined as a part of our ongoing research on the synthesis and biological evaluation of sulfur containing heterocyclic compounds (Zia-ur-Rehman et al., 2005, 2006, 2009). In the molecule of (I) (Fig. 1), bond lengths and bond angles are almost similar to those in related sulfonamide molecules (Gowda et al., 2007a, 2007b, 2007c) and the bond lengths are within normal ranges. In the crystal structure, each molecule is linked to an adjacent one through C7—H7B···O3 contacts giving rise to chains along b-axis. Each molecule of the chain is further linked to the one of its neighbouring chain along a through intermolecular N—H···O interactions.

Related literature top

For the synthesis and biological evaluation of sulfur-containing heterocyclic compounds, see: Zia-ur-Rehman et al. (2005, 2006, 2009); Xiao & Timberlake (2000); Martinez et al. (2000); Berredjem et al. (2000); Lee & Lee (2002). For related literature on sulfonamides, see: Esteve & Bidal (2002); Soledade et al. (2006). For rlated structures, see: Gowda et al. (2007a,b,c).

Experimental top

A mixture of benzene sulfonic acid (4.14 g, 23.44 mmoles), glycine methyl ester hydrochloride (2.94 g, 23.44 mmol.) and distilled water (50.0 ml) was stirred for half an hour. pH of the reaction mixture was adjusted to 8.0 with an aqueous sodium carbonate solution. After completion of the reaction, a white solid product was isolated, washed, dried and recrystallized in methanol to get the crystals suitable for for X-ray studies; m.p. 332 K.

Refinement top

H atoms were placed in geometric positions (C—H = 0.93-0.97 Å; N—H = 0.86 Å) using a riding model with Uiso(H) = 1.2 Ueq(C,N) or Uiso(H) = 1.5 Ueq(Cmethyl).

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and local programs.

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound showing the atom labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. Part of the crystal structure, showing hydrogen bond interactions (dashed lines). along the [0 0 1] direction. H atoms not involved in hydrogen bonding have been omitted for clarity.
Methyl 2-(benzenesulfonamido)acetate top
Crystal data top
C9H11NO4SF000 = 240
Mr = 229.26Dx = 1.433 Mg m3
Monoclinic, P21Melting point: 332 K
Hall symbol: P 2ybMo Kα radiation
λ = 0.71073 Å
a = 9.7268 (8) ÅCell parameters from 2710 reflections
b = 5.0781 (4) Åθ = 2.6–26.6º
c = 10.9286 (9) ŵ = 0.30 mm1
β = 100.087 (3)ºT = 296 K
V = 531.46 (7) Å3Plates, colourless
Z = 20.23 × 0.11 × 0.08 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2216 independent reflections
Radiation source: fine-focus sealed tube1944 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.028
T = 296 Kθmax = 29.3º
φ and ω scansθmin = 2.6º
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
h = 12→13
Tmin = 0.935, Tmax = 0.977k = 4→6
6159 measured reflectionsl = 11→15
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.036  w = 1/[σ2(Fo2) + (0.0526P)2 + 0.0105P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.092(Δ/σ)max < 0.001
S = 1.07Δρmax = 0.25 e Å3
2216 reflectionsΔρmin = 0.26 e Å3
137 parametersExtinction correction: none
1 restraintAbsolute structure: Flack (1983), 394 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.089 (8)
Secondary atom site location: difference Fourier map
Crystal data top
C9H11NO4SV = 531.46 (7) Å3
Mr = 229.26Z = 2
Monoclinic, P21Mo Kα
a = 9.7268 (8) ŵ = 0.30 mm1
b = 5.0781 (4) ÅT = 296 K
c = 10.9286 (9) Å0.23 × 0.11 × 0.08 mm
β = 100.087 (3)º
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2216 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
1944 reflections with I > 2σ(I)
Tmin = 0.935, Tmax = 0.977Rint = 0.028
6159 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.092Δρmax = 0.25 e Å3
S = 1.07Δρmin = 0.26 e Å3
2216 reflectionsAbsolute structure: Flack (1983), 394 Friedel pairs
137 parametersFlack parameter: 0.089 (8)
1 restraint
Special details top

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) top
xyzUiso*/Ueq
S10.61607 (5)0.09862 (10)0.21011 (5)0.03580 (15)
O10.52527 (16)0.0799 (4)0.25831 (16)0.0482 (4)
O20.72360 (15)0.0024 (4)0.14799 (15)0.0468 (4)
O30.27134 (16)0.0012 (4)0.03143 (16)0.0469 (4)
O40.16275 (17)0.2366 (4)0.15812 (18)0.0589 (5)
N10.51744 (17)0.2853 (4)0.11147 (16)0.0389 (5)
H10.54230.32940.04260.047*
C10.6962 (2)0.2993 (5)0.3344 (2)0.0366 (5)
C20.6546 (3)0.2854 (7)0.4486 (2)0.0537 (7)
H20.58470.16870.46140.064*
C30.7181 (3)0.4473 (8)0.5441 (2)0.0669 (9)
H30.69130.43820.62160.080*
C40.8199 (3)0.6206 (8)0.5249 (3)0.0646 (8)
H40.86120.73030.58910.078*
C50.8614 (3)0.6333 (7)0.4113 (3)0.0602 (7)
H50.93170.74940.39920.072*
C60.7990 (2)0.4739 (5)0.3148 (2)0.0481 (6)
H60.82590.48430.23740.058*
C70.3858 (2)0.3768 (5)0.1419 (2)0.0365 (5)
H7B0.36100.54370.10080.044*
H7A0.39660.40500.23090.044*
C80.2709 (2)0.1813 (5)0.10223 (19)0.0346 (5)
C90.0435 (3)0.0566 (10)0.1303 (3)0.0886 (12)
H9A0.01320.04690.04190.133*
H9B0.03150.12040.16870.133*
H9C0.07090.11550.16190.133*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0316 (2)0.0341 (3)0.0417 (3)0.0008 (3)0.00653 (19)0.0014 (3)
O10.0446 (9)0.0426 (10)0.0565 (10)0.0084 (8)0.0069 (8)0.0094 (9)
O20.0390 (8)0.0496 (11)0.0525 (10)0.0075 (8)0.0099 (7)0.0064 (8)
O30.0415 (9)0.0443 (10)0.0559 (10)0.0052 (8)0.0114 (7)0.0095 (9)
O40.0329 (8)0.0774 (14)0.0701 (11)0.0025 (9)0.0194 (8)0.0181 (11)
N10.0333 (9)0.0445 (12)0.0393 (10)0.0014 (9)0.0074 (8)0.0040 (9)
C10.0292 (10)0.0377 (13)0.0412 (11)0.0037 (9)0.0014 (8)0.0020 (10)
C20.0461 (14)0.0662 (19)0.0502 (14)0.0020 (14)0.0123 (11)0.0009 (14)
C30.0632 (17)0.091 (3)0.0467 (15)0.0050 (18)0.0092 (13)0.0126 (16)
C40.0643 (16)0.064 (2)0.0587 (15)0.0052 (18)0.0098 (12)0.0190 (18)
C50.0537 (14)0.051 (2)0.0701 (16)0.0110 (15)0.0044 (12)0.0030 (16)
C60.0469 (13)0.0451 (16)0.0518 (14)0.0052 (12)0.0071 (11)0.0017 (12)
C70.0352 (11)0.0327 (13)0.0423 (11)0.0031 (10)0.0082 (9)0.0019 (10)
C80.0295 (10)0.0394 (14)0.0342 (10)0.0059 (9)0.0038 (8)0.0031 (10)
C90.0397 (14)0.116 (3)0.114 (3)0.0180 (19)0.0257 (16)0.015 (3)
Geometric parameters (Å, °) top
S1—O11.4290 (16)C3—C41.369 (4)
S1—O21.4291 (15)C3—H30.9300
S1—N11.618 (2)C4—C51.372 (4)
S1—C11.767 (2)C4—H40.9300
O3—C81.198 (3)C5—C61.383 (4)
O4—C81.336 (2)C5—H50.9300
O4—C91.466 (4)C6—H60.9300
N1—C71.454 (3)C7—C81.501 (3)
N1—H10.8600C7—H7B0.9700
C1—C21.380 (3)C7—H7A0.9700
C1—C61.381 (3)C9—H9A0.9600
C2—C31.386 (4)C9—H9B0.9600
C2—H20.9300C9—H9C0.9600
O1—S1—O2120.61 (11)C4—C5—C6120.2 (3)
O1—S1—N1106.53 (9)C4—C5—H5119.9
O2—S1—N1106.36 (9)C6—C5—H5119.9
O1—S1—C1107.48 (10)C1—C6—C5119.4 (2)
O2—S1—C1107.55 (10)C1—C6—H6120.3
N1—S1—C1107.73 (10)C5—C6—H6120.3
C8—O4—C9115.6 (2)N1—C7—C8111.31 (18)
C7—N1—S1118.54 (14)N1—C7—H7B109.4
C7—N1—H1120.7C8—C7—H7B109.4
S1—N1—H1120.7N1—C7—H7A109.4
C2—C1—C6120.6 (2)C8—C7—H7A109.4
C2—C1—S1120.4 (2)H7B—C7—H7A108.0
C6—C1—S1119.01 (17)O3—C8—O4123.2 (2)
C1—C2—C3119.2 (3)O3—C8—C7127.20 (19)
C1—C2—H2120.4O4—C8—C7109.60 (19)
C3—C2—H2120.4O4—C9—H9A109.5
C4—C3—C2120.3 (3)O4—C9—H9B109.5
C4—C3—H3119.8H9A—C9—H9B109.5
C2—C3—H3119.8O4—C9—H9C109.5
C3—C4—C5120.3 (3)H9A—C9—H9C109.5
C3—C4—H4119.9H9B—C9—H9C109.5
C5—C4—H4119.9
O1—S1—N1—C740.2 (2)C1—C2—C3—C40.6 (5)
O2—S1—N1—C7170.05 (17)C2—C3—C4—C50.8 (5)
C1—S1—N1—C774.87 (19)C3—C4—C5—C61.0 (5)
O1—S1—C1—C27.1 (2)C2—C1—C6—C50.8 (4)
O2—S1—C1—C2138.4 (2)S1—C1—C6—C5179.5 (2)
N1—S1—C1—C2107.3 (2)C4—C5—C6—C11.0 (4)
O1—S1—C1—C6174.20 (18)S1—N1—C7—C886.9 (2)
O2—S1—C1—C642.9 (2)C9—O4—C8—O31.7 (3)
N1—S1—C1—C671.3 (2)C9—O4—C8—C7178.5 (2)
C6—C1—C2—C30.6 (4)N1—C7—C8—O315.8 (3)
S1—C1—C2—C3179.2 (2)N1—C7—C8—O4164.42 (18)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O3i0.862.282.998 (2)141
C7—H7B···O3ii0.972.553.503 (4)168
Symmetry codes: (i) −x+1, y+1/2, −z; (ii) x, y+1, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1···O3i0.862.282.998 (2)141
C7—H7B···O3ii0.972.553.503 (4)168
Symmetry codes: (i) −x+1, y+1/2, −z; (ii) x, y+1, z.
Acknowledgements top

The authors are grateful to the Higher Education Commission of Pakistan for financial support to purchase the diffractometer. MNA acknowledges the Higher Education Commission, Pakistan, for providing a PhD Scholarship under PIN 042- 120607-PS2–183.

references
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