supplementary materials


at2777 scheme

Acta Cryst. (2009). E65, o1257    [ doi:10.1107/S1600536809016651 ]

N'-(Phenylsulfonyl)isonicotinohydrazide monohydrate

C.-R. Li, K.-Z. Zhou, Y.-Q. Zhang, S.-F. Xue and H. Cong

Abstract top

In the title compound, C12H11N3O3S·H2O, the pyridine ring makes a dihedral angle of 24.78 (14)° with the phenyl ring. Intramolecular N-H...O and intermolecular O-H...O hydrogen bonds are observed and stabilize the packing in the crystal structure.

Comment top

Hydrazide derivatives investigated in the present work are non-toxic in nature, which play an important role in latex, plastic industry (Lemin et al., 1961; Zhen et al., 2008) and corrosion inhibition of mild steel in acidic medium (Shanbhag et al., 2008). In this paper, a substituted hydrazide, benzenesulfisoniazide, was synthesized in the solution of ethanol with benzenesulfonyl chloride and isoniazide in the ice-bath is reported.

The crystal of the title compound, (I), consists of N'-(phenylsulfinyl)isonicotinohydrazide and one water molecule, (Fig. 1). Pyridine ring makes a dihedral angle of 24.78 (14)° with the phenyl ring. The N—H···O hydrogen bonds are observed between N3 and the water molecule O1W, which the distance of the N3(H3N)···O1W hydrogen bonds is 2.779 (3) Å. In addition, there are O—H···O hydrogen bonds between O1W and O2 with distance of 2.857 (3) Å (Table 1). These hydrogen bonding interactions may help to establish the packing in the crystal structure.

Related literature top

For general background to hydrazide derivatives, see: Lemin et al. (1961); Shanbhag et al. (2008); Zhen et al. (2008).

Experimental top

Solution of benzenesulfonyl chloride (0.04 mol) in ethanol was added to a stirred ethanol solution of isoniazid (0.02 mol) in the ice-bath, then the reaction was kept on for 2 h at room temperature. The solvent was removed by reduced pressure filter, the solid product was dissolved in 50 ml ethanol,. and then set aside for five days to obtain colourless crystals.

Refinement top

Water H atoms were located in a difference Fourier map and refined as riding in their as-found positions relative to O atoms with Uiso(H) = 1.5Ueq(O). All other H atoms were placed in calculated positions and refined as riding, with C—H = 0.93–0.97 Å, N—H = 0.86 Å, and Uiso(H) = 1.2–1.5 Ueq(C,N).

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level.
N'-(Phenylsulfonyl)isonicotinohydrazide monohydrate top
Crystal data top
C12H11N3O3S·H2OF000 = 616
Mr = 295.32Dx = 1.446 Mg m3
Monoclinic, P21/nMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 2343 reflections
a = 7.3525 (5) Åθ = 2.0–25.0º
b = 20.9324 (15) ŵ = 0.26 mm1
c = 9.2443 (6) ÅT = 273 K
β = 107.565 (2)ºBlock, colourless
V = 1356.41 (16) Å30.24 × 0.22 × 0.19 mm
Z = 4
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2343 independent reflections
Radiation source: fine-focus sealed tube1981 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.033
T = 273 Kθmax = 25.0º
φ and ω scanθmin = 2.0º
Absorption correction: multi-scan
(SADABS; Bruker, 2005)
h = 8→8
Tmin = 0.833, Tmax = 0.864k = 24→24
10653 measured reflectionsl = 10→10
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.120  w = 1/[σ2(Fo2) + (0.0631P)2 + 0.5954P]
where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max < 0.001
2343 reflectionsΔρmax = 0.43 e Å3
189 parametersΔρmin = 0.53 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C12H11N3O3S·H2OV = 1356.41 (16) Å3
Mr = 295.32Z = 4
Monoclinic, P21/nMo Kα
a = 7.3525 (5) ŵ = 0.26 mm1
b = 20.9324 (15) ÅT = 273 K
c = 9.2443 (6) Å0.24 × 0.22 × 0.19 mm
β = 107.565 (2)º
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2343 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2005)
1981 reflections with I > 2σ(I)
Tmin = 0.833, Tmax = 0.864Rint = 0.033
10653 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.037189 parameters
wR(F2) = 0.120H atoms treated by a mixture of
independent and constrained refinement
S = 1.12Δρmax = 0.43 e Å3
2343 reflectionsΔρmin = 0.53 e Å3
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
C10.5180 (5)0.38868 (12)0.1480 (3)0.0457 (7)
H10.47800.37690.04630.055*
C20.5608 (5)0.45147 (13)0.1899 (3)0.0598 (9)
H20.55230.48100.11310.072*
C30.6284 (4)0.42875 (11)0.4392 (3)0.0339 (6)
H30.66530.44200.53990.041*
C40.5927 (3)0.36459 (11)0.4100 (2)0.0297 (5)
H40.60650.33590.48940.036*
C50.5361 (3)0.34348 (10)0.2611 (2)0.0257 (5)
C60.4884 (3)0.27532 (10)0.2125 (2)0.0253 (5)
C70.4594 (3)0.13874 (10)0.5560 (3)0.0289 (5)
C80.4371 (3)0.19677 (11)0.6218 (3)0.0322 (5)
H80.38440.23170.56160.039*
C90.4947 (4)0.20161 (12)0.7788 (3)0.0370 (6)
H90.48260.24030.82460.044*
C100.5702 (4)0.14896 (14)0.8673 (3)0.0424 (6)
H100.60660.15230.97250.051*
C110.5917 (4)0.09153 (13)0.8006 (3)0.0439 (7)
H110.64260.05650.86110.053*
C120.5379 (4)0.08587 (12)0.6439 (3)0.0359 (6)
H120.55400.04750.59860.043*
N10.6133 (3)0.47292 (9)0.3323 (2)0.0400 (5)
N20.5685 (3)0.23082 (8)0.31946 (19)0.0258 (4)
H2N0.63980.24250.40750.031*
N30.5352 (3)0.16619 (9)0.2867 (2)0.0293 (5)
H3N0.59250.14580.23240.035*
O10.3873 (2)0.26165 (8)0.08506 (16)0.0340 (4)
O20.2057 (2)0.16569 (8)0.30300 (19)0.0366 (4)
O30.3881 (3)0.06518 (8)0.31658 (19)0.0421 (5)
S10.38198 (8)0.13081 (3)0.35666 (6)0.0294 (2)
H1E0.942 (6)0.1209 (16)0.248 (4)0.063 (12)*
H1F0.849 (5)0.0671 (18)0.196 (4)0.063 (10)*
O1W0.8432 (3)0.10382 (10)0.2345 (2)0.0421 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.074 (2)0.0366 (14)0.0207 (12)0.0022 (13)0.0047 (12)0.0032 (10)
C20.109 (3)0.0334 (15)0.0298 (14)0.0045 (16)0.0109 (16)0.0109 (11)
C30.0439 (15)0.0309 (13)0.0245 (11)0.0031 (10)0.0068 (11)0.0011 (10)
C40.0356 (14)0.0298 (13)0.0210 (11)0.0041 (10)0.0047 (10)0.0035 (9)
C50.0239 (12)0.0290 (12)0.0223 (11)0.0043 (9)0.0042 (9)0.0018 (9)
C60.0226 (12)0.0323 (12)0.0192 (11)0.0027 (9)0.0037 (9)0.0000 (9)
C70.0306 (13)0.0260 (12)0.0285 (12)0.0040 (9)0.0064 (10)0.0012 (9)
C80.0360 (14)0.0282 (12)0.0348 (12)0.0019 (10)0.0144 (11)0.0008 (10)
C90.0384 (15)0.0392 (14)0.0378 (13)0.0110 (11)0.0181 (12)0.0107 (11)
C100.0422 (16)0.0572 (17)0.0273 (12)0.0089 (13)0.0096 (11)0.0029 (12)
C110.0493 (18)0.0434 (16)0.0350 (14)0.0029 (12)0.0068 (12)0.0098 (12)
C120.0393 (15)0.0298 (13)0.0341 (13)0.0012 (11)0.0044 (11)0.0001 (10)
N10.0537 (14)0.0300 (11)0.0331 (11)0.0006 (9)0.0084 (10)0.0014 (9)
N20.0283 (11)0.0243 (10)0.0191 (9)0.0005 (7)0.0015 (8)0.0017 (7)
N30.0354 (12)0.0252 (10)0.0259 (9)0.0027 (8)0.0073 (8)0.0044 (8)
O10.0341 (10)0.0392 (10)0.0205 (8)0.0009 (7)0.0041 (7)0.0024 (7)
O20.0273 (10)0.0362 (10)0.0401 (10)0.0004 (7)0.0008 (7)0.0024 (7)
O30.0606 (13)0.0233 (9)0.0349 (9)0.0036 (8)0.0031 (9)0.0048 (7)
S10.0332 (4)0.0227 (3)0.0273 (3)0.0019 (2)0.0014 (2)0.0017 (2)
O1W0.0352 (12)0.0344 (11)0.0582 (12)0.0005 (9)0.0161 (10)0.0123 (9)
Geometric parameters (Å, °) top
C1—C21.379 (4)C8—H80.9300
C1—C51.386 (3)C9—C101.385 (4)
C1—H10.9300C9—H90.9300
C2—N11.333 (3)C10—C111.382 (4)
C2—H20.9300C10—H100.9300
C3—N11.333 (3)C11—C121.386 (3)
C3—C41.379 (3)C11—H110.9300
C3—H30.9300C12—H120.9300
C4—C51.385 (3)N2—N31.392 (2)
C4—H40.9300N2—H2N0.8600
C5—C61.505 (3)N3—S11.635 (2)
C6—O11.223 (3)N3—H3N0.8600
C6—N21.356 (3)O2—S11.4393 (17)
C7—C81.390 (3)O3—S11.4272 (17)
C7—C121.392 (3)O1W—H1E0.78 (4)
C7—S11.764 (2)O1W—H1F0.86 (4)
C8—C91.387 (3)
C2—C1—C5118.5 (2)C10—C9—H9120.0
C2—C1—H1120.8C8—C9—H9120.0
C5—C1—H1120.8C11—C10—C9120.5 (2)
N1—C2—C1124.9 (2)C11—C10—H10119.7
N1—C2—H2117.6C9—C10—H10119.7
C1—C2—H2117.6C10—C11—C12120.4 (2)
N1—C3—C4124.2 (2)C10—C11—H11119.8
N1—C3—H3117.9C12—C11—H11119.8
C4—C3—H3117.9C11—C12—C7118.7 (2)
C3—C4—C5119.2 (2)C11—C12—H12120.7
C3—C4—H4120.4C7—C12—H12120.7
C5—C4—H4120.4C2—N1—C3115.6 (2)
C4—C5—C1117.6 (2)C6—N2—N3120.00 (17)
C4—C5—C6124.90 (19)C6—N2—H2N120.0
C1—C5—C6117.5 (2)N3—N2—H2N120.0
O1—C6—N2123.1 (2)N2—N3—S1116.82 (14)
O1—C6—C5121.90 (19)N2—N3—H3N121.6
N2—C6—C5115.02 (18)S1—N3—H3N121.6
C8—C7—C12121.5 (2)O3—S1—O2119.65 (11)
C8—C7—S1119.73 (18)O3—S1—N3104.70 (10)
C12—C7—S1118.79 (17)O2—S1—N3106.88 (10)
C9—C8—C7118.9 (2)O3—S1—C7109.64 (10)
C9—C8—H8120.6O2—S1—C7106.57 (11)
C7—C8—H8120.6N3—S1—C7109.05 (10)
C10—C9—C8120.1 (2)H1E—O1W—H1F108 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N3—H3N···O1W0.862.042.779 (3)144
O1W—H1E···O2i0.78 (4)2.07 (4)2.857 (3)175 (4)
Symmetry codes: (i) x+1, y, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N3—H3N···O1W0.862.042.779 (3)144
O1W—H1E···O2i0.78 (4)2.07 (4)2.857 (3)175 (4)
Symmetry codes: (i) x+1, y, z.
Acknowledgements top

The authors gratefully acknowledge the Natural Science Foundation of China (No. 20767001), the International Collaborative Project of Guizhou Province and the Governor Foundation of Guizhou Province for financial support.

references
References top

Bruker (2002). SMART and SAINT. Bruker AXS, Inc., Madison, Wisconsin, USA.

Bruker (2005). SADABS. Bruker AXS, Inc., Madison, Wisconsin, USA.

Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.

Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.

Lemin, A. J. (1961). US Patent 2993829.

Shanbhag, A. V., Venkatesha, T. V., Prabhu, R. A., Kalkhambkar, R. G. & Kulkarni, G. M. (2008). J. Appl. Electrochem. 38, 279–287.

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

Zhen, X.-L. & Li, X.-L. (2008). Acta Cryst. E64, o2170.