supplementary materials


Acta Cryst. (2008). E64, o2109    [ doi:10.1107/S1600536808032273 ]

4-Nitro-N-(4-pyridinio)benzenesulfonamidate monohydrate

Y.-Z. Chen, H. Gao, G. Li, X.-J. Chen and S.-Y. Niu

Abstract top

The title compound, C11H9N3O4S·H2O, contains both an acid and a base centre, and displays a zwitterionic structure in the solid state. The benzene ring makes an angle of 109.1 (2)° with the pyridinium ring. The crystal structure is stabilized by O-H...N, O-H...O and N-H...O hydrogen bonds.

Comment top

Organic pyridinium salts have been widely used in the construction of supramolecular architectures (Teresa et al., 2007). As part of our ongoing studies of supramolecular chemistry involving the pyridinium rings (Li et al., 2007), the structure of the title compound (I) was determined by X-ray diffraction.

In the cations of (I) (Fig. 1), the short C—N distance [N2—C1 = 1.370 (3) Å] has a value between those of a typical CN double and C—N single bond [1.47–1.50 Å and 1.34–1.38 Å, respectively; Allen et al., 1987]. This might be indicative of a slight π electron conjugation of the sulphonamide N with the pyridinium ring. The benzene ring exhibits an angle of 109.1 (2) ° with the pyridinium ring. The dihedral angle between the nitro group and the benzene ring is 2.2 (1) °.

The crystal structure is stabilized by O—H···N, O—H···O and N—H···O hydrogen bonds (Table 1).

Related literature top

For related literature, see: Allen et al. (1987); Li et al. (2007); Teresa et al. (2007); Yu & Li (2007).

Experimental top

A solution of 4-nitrobenzenesulfonyl chloride (2.2 g, 10 mmol) in CH2Cl2 (10 ml) was added dropwise to a suspension of 4-aminopyridine (0.9 g, 10 mmol) in CH2Cl2 (10 ml) at room temperature with stirring. The reaction mixture was stirred overnight. The yellow solid obtained was washed with warm water to obtain the title compound in a yield of 55.3%. A colourless single-crystal suitable for X-ray analysis was obtained by slow evaporation of an acetic acid solution at room temperature over a period of a week.

Refinement top

The H atoms of the water molecule were found on a difference Fourier map and refined freely. The N-bound H atoms were located in a difference map and their coordinates were refined with Uiso(H) = 1.2Ueq(N). The C-bound H atoms were positioned geometrically (C—H = 0.95 Å) and refined as riding with Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Molecular view of the title compound (I) showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 35% probability level (arbitrary spheres for the H atoms).
4-Nitro-N-(4-pyridinio)benzenesulfonamidate monohydrate top
Crystal data top
C11H9N3O4S·H2OF(000) = 616
Mr = 297.29Dx = 1.600 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 3340 reflections
a = 6.7766 (14) Åθ = 1.9–27.9°
b = 8.3932 (17) ŵ = 0.29 mm1
c = 21.717 (4) ÅT = 113 K
β = 92.35 (3)°Block, colourless
V = 1234.2 (4) Å30.20 × 0.18 × 0.12 mm
Z = 4
Data collection top
Rigaku Saturn CCD area-detector
diffractometer
2908 independent reflections
Radiation source: rotating anode2022 reflections with I > 2σ(I)
confocalRint = 0.061
Detector resolution: 7.31 pixels mm-1θmax = 27.9°, θmin = 1.9°
ω and φ scansh = 87
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
k = 1110
Tmin = 0.932, Tmax = 0.963l = 1928
9708 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.055Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.136H atoms treated by a mixture of independent and constrained refinement
S = 1.17 w = 1/[σ2(Fo2) + (0.031P)2 + 1.5168P]
where P = (Fo2 + 2Fc2)/3
2908 reflections(Δ/σ)max = 0.002
193 parametersΔρmax = 0.35 e Å3
0 restraintsΔρmin = 0.45 e Å3
Crystal data top
C11H9N3O4S·H2OV = 1234.2 (4) Å3
Mr = 297.29Z = 4
Monoclinic, P21/nMo Kα radiation
a = 6.7766 (14) ŵ = 0.29 mm1
b = 8.3932 (17) ÅT = 113 K
c = 21.717 (4) Å0.20 × 0.18 × 0.12 mm
β = 92.35 (3)°
Data collection top
Rigaku Saturn CCD area-detector
diffractometer
2908 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
2022 reflections with I > 2σ(I)
Tmin = 0.932, Tmax = 0.963Rint = 0.061
9708 measured reflectionsθmax = 27.9°
Refinement top
R[F2 > 2σ(F2)] = 0.055H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.136Δρmax = 0.35 e Å3
S = 1.17Δρmin = 0.45 e Å3
2908 reflectionsAbsolute structure: ?
193 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
S10.89206 (11)0.18818 (8)0.12547 (3)0.01574 (18)
N10.7145 (4)0.7176 (3)0.00969 (13)0.0228 (6)
H1A0.707 (6)0.823 (5)0.0019 (19)0.048 (12)*
N20.8061 (4)0.2477 (3)0.06005 (11)0.0166 (5)
N30.2350 (4)0.1341 (3)0.29976 (12)0.0236 (6)
O11.0378 (3)0.2937 (2)0.15368 (9)0.0197 (5)
O20.9523 (3)0.0240 (2)0.11577 (10)0.0208 (5)
O30.2477 (4)0.2106 (3)0.34777 (10)0.0332 (6)
O40.0934 (4)0.0497 (3)0.28506 (13)0.0401 (7)
C10.7738 (4)0.4058 (3)0.04742 (13)0.0151 (6)
C20.7618 (5)0.5312 (3)0.09068 (14)0.0203 (6)
H20.77360.50990.13360.024*
C30.7329 (5)0.6835 (4)0.06978 (16)0.0259 (7)
H30.72570.76770.09890.031*
C40.7199 (5)0.6006 (4)0.03300 (14)0.0204 (6)
H40.70530.62650.07550.024*
C50.7463 (4)0.4454 (3)0.01543 (14)0.0176 (6)
H50.74620.36380.04580.021*
C60.6953 (4)0.1762 (3)0.17671 (13)0.0150 (6)
C70.5306 (5)0.0811 (3)0.16067 (13)0.0182 (6)
H70.52300.02750.12210.022*
C80.3798 (5)0.0659 (3)0.20114 (14)0.0180 (6)
H80.26780.00130.19120.022*
C90.3961 (4)0.1475 (3)0.25685 (13)0.0171 (6)
C100.5550 (5)0.2447 (3)0.27298 (14)0.0199 (6)
H100.55980.30110.31090.024*
C110.7072 (5)0.2580 (3)0.23239 (13)0.0189 (6)
H110.81890.32260.24260.023*
O50.7268 (4)0.0224 (2)0.03361 (11)0.0216 (5)
H5A0.763 (6)0.079 (5)0.003 (2)0.046 (13)*
H5B0.815 (7)0.027 (5)0.060 (2)0.049 (14)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0176 (4)0.0143 (3)0.0154 (3)0.0017 (3)0.0016 (3)0.0006 (3)
N10.0216 (15)0.0139 (11)0.0326 (15)0.0023 (10)0.0021 (12)0.0047 (11)
N20.0213 (14)0.0133 (11)0.0152 (11)0.0014 (10)0.0005 (10)0.0005 (9)
N30.0253 (15)0.0227 (13)0.0231 (14)0.0026 (11)0.0061 (12)0.0037 (11)
O10.0175 (11)0.0213 (10)0.0203 (11)0.0013 (9)0.0007 (8)0.0004 (9)
O20.0254 (12)0.0151 (10)0.0222 (11)0.0054 (8)0.0056 (9)0.0025 (8)
O30.0445 (16)0.0358 (13)0.0202 (11)0.0024 (11)0.0134 (11)0.0026 (10)
O40.0294 (15)0.0468 (15)0.0452 (16)0.0171 (12)0.0146 (13)0.0081 (13)
C10.0116 (15)0.0138 (12)0.0201 (14)0.0010 (10)0.0029 (12)0.0012 (11)
C20.0251 (17)0.0172 (13)0.0184 (14)0.0024 (12)0.0027 (13)0.0017 (12)
C30.0309 (19)0.0169 (14)0.0292 (17)0.0010 (13)0.0068 (14)0.0050 (13)
C40.0158 (16)0.0244 (14)0.0211 (15)0.0013 (12)0.0026 (12)0.0048 (12)
C50.0135 (15)0.0199 (13)0.0196 (14)0.0005 (11)0.0037 (12)0.0003 (12)
C60.0155 (15)0.0147 (12)0.0148 (13)0.0028 (11)0.0008 (11)0.0019 (11)
C70.0204 (16)0.0189 (13)0.0150 (13)0.0013 (12)0.0024 (12)0.0021 (11)
C80.0164 (16)0.0166 (13)0.0207 (14)0.0005 (11)0.0012 (12)0.0003 (12)
C90.0180 (15)0.0170 (13)0.0165 (14)0.0022 (11)0.0033 (12)0.0033 (11)
C100.0241 (17)0.0205 (13)0.0151 (13)0.0021 (12)0.0000 (12)0.0035 (12)
C110.0221 (16)0.0190 (13)0.0156 (13)0.0026 (12)0.0008 (12)0.0012 (11)
O50.0292 (14)0.0158 (10)0.0199 (11)0.0026 (9)0.0037 (10)0.0011 (9)
Geometric parameters (Å, °) top
S1—O11.444 (2)C4—C51.367 (4)
S1—O21.455 (2)C4—H40.9500
S1—N21.594 (2)C5—H50.9500
S1—C61.774 (3)C6—C111.390 (4)
N1—C31.337 (4)C6—C71.404 (4)
N1—C41.352 (4)C7—C81.381 (4)
N1—H1A0.92 (4)C7—H70.9500
N2—C11.370 (3)C8—C91.391 (4)
N3—O41.224 (4)C8—H80.9500
N3—O31.225 (3)C9—C101.385 (4)
N3—C91.468 (4)C10—C111.388 (4)
C1—C51.410 (4)C10—H100.9500
C1—C21.416 (4)C11—H110.9500
C2—C31.368 (4)O5—H5A0.85 (4)
C2—H20.9500O5—H5B0.85 (5)
C3—H30.9500
O1—S1—O2116.81 (13)C5—C4—H4119.8
O1—S1—N2113.86 (13)C4—C5—C1120.4 (3)
O2—S1—N2105.21 (12)C4—C5—H5119.8
O1—S1—C6106.69 (13)C1—C5—H5119.8
O2—S1—C6105.05 (13)C11—C6—C7120.9 (3)
N2—S1—C6108.69 (13)C11—C6—S1120.0 (2)
C3—N1—C4120.7 (3)C7—C6—S1119.1 (2)
C3—N1—H1A118 (3)C8—C7—C6119.8 (3)
C4—N1—H1A121 (3)C8—C7—H7120.1
C1—N2—S1122.1 (2)C6—C7—H7120.1
O4—N3—O3123.5 (3)C7—C8—C9118.2 (3)
O4—N3—C9118.3 (3)C7—C8—H8120.9
O3—N3—C9118.2 (3)C9—C8—H8120.9
N2—C1—C5115.9 (2)C10—C9—C8122.9 (3)
N2—C1—C2126.9 (3)C10—C9—N3118.4 (3)
C5—C1—C2117.2 (3)C8—C9—N3118.7 (3)
C3—C2—C1119.1 (3)C9—C10—C11118.5 (3)
C3—C2—H2120.5C9—C10—H10120.8
C1—C2—H2120.5C11—C10—H10120.8
N1—C3—C2122.0 (3)C10—C11—C6119.6 (3)
N1—C3—H3119.0C10—C11—H11120.2
C2—C3—H3119.0C6—C11—H11120.2
N1—C4—C5120.5 (3)H5A—O5—H5B109 (4)
N1—C4—H4119.8
O1—S1—N2—C136.5 (3)O2—S1—C6—C755.7 (3)
O2—S1—N2—C1165.6 (2)N2—S1—C6—C756.5 (3)
C6—S1—N2—C182.3 (3)C11—C6—C7—C81.3 (4)
S1—N2—C1—C5164.4 (2)S1—C6—C7—C8177.6 (2)
S1—N2—C1—C216.8 (4)C6—C7—C8—C90.5 (4)
N2—C1—C2—C3178.6 (3)C7—C8—C9—C101.0 (4)
C5—C1—C2—C32.7 (5)C7—C8—C9—N3179.0 (3)
C4—N1—C3—C21.4 (5)O4—N3—C9—C10179.1 (3)
C1—C2—C3—N10.4 (5)O3—N3—C9—C100.6 (4)
C3—N1—C4—C50.6 (5)O4—N3—C9—C80.9 (4)
N1—C4—C5—C11.8 (5)O3—N3—C9—C8177.6 (3)
N2—C1—C5—C4177.7 (3)C8—C9—C10—C111.7 (4)
C2—C1—C5—C43.4 (4)N3—C9—C10—C11179.8 (3)
O1—S1—C6—C111.5 (3)C9—C10—C11—C61.0 (4)
O2—S1—C6—C11123.1 (2)C7—C6—C11—C100.5 (4)
N2—S1—C6—C11124.7 (2)S1—C6—C11—C10178.3 (2)
O1—S1—C6—C7179.7 (2)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O5—H5A···N20.85 (4)1.97 (4)2.813 (3)167 (4)
O5—H5B···O2i0.85 (5)2.07 (5)2.895 (3)164 (4)
N1—H1A···O5ii0.92 (4)1.82 (4)2.728 (3)170 (4)
Symmetry codes: (i) −x+2, −y, −z; (ii) x, y+1, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O5—H5A···N20.85 (4)1.97 (4)2.813 (3)167 (4)
O5—H5B···O2i0.85 (5)2.07 (5)2.895 (3)164 (4)
N1—H1A···O5ii0.92 (4)1.82 (4)2.728 (3)170 (4)
Symmetry codes: (i) −x+2, −y, −z; (ii) x, y+1, z.
Acknowledgements top

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references
References top

Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. 1–19.

Li, J. S., Chen, L. G., Zhang, Y. Y., Xu, Y. J., Deng, Y. & Huang, P. M. (2007). J. Chem. Res. 6, 350–352.

Rigaku/MSC (2005). CrystalClear. Rigaku/MSC, The Woodlands, Texas, USA.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Teresa, D., Daniel, M. & Adam, N. (2007). Org. Biomol. Chem. 5, 2735–2752.

Yu, H.-J. & Li, J.-S. (2007). Acta Cryst. E63, o3399.