supplementary materials


Acta Cryst. (2007). E63, o3696    [ doi:10.1107/S1600536807037518 ]

p-Tosylhydrazine: a redetermination from single-crystal data at 100 K

S. Roy and A. Nangia

Abstract top

Redetermination of the structure of the title compound, alternatively called 4-methylbenzenesulfonohydrazide, C7H10N2O2S, at 100 K reveals that both H atoms of the NH2 group form intermolecular N-H...O hydrogen bonds, which together with an N-H...O hydrogen bond from the NH group form a sheet-like structure in the ab plane.

Comment top

The structure of the title compound, C7H10N2O2S (Figure 1), has been determined previously by Lightfoot et al. (1993) from powder X-ray diffraction data. However, H atoms could not be located using that technique and the authors assumed the presence of an intramolecular N—H···O hydrogen bond (graph-set motif S(5)). Re-determination of the structure using single-crystal X-ray diffraction reveals that the H atoms of the NH2 group actually make intermolecular N—H···O hydrogen bonds, with O1 and O2 acting as acceptors (Table 1). The N1—H1···O1 and N2—H2A···O2 hydrogen bonds link the molecules into double chains along the b axis, and these chains are linked via N2—H2B···O2 hydrogen bonds to form a sheet-like structure in the ab planes.

Related literature top

For a previous determination of the structure from powder X-ray diffraction data, see: Lightfoot et al. (1993). For synthesis details, see: Friedman et al. (1973).

Experimental top

Single crystals of 4-tosylhydrazine (Friedman et al., 1973) were obtained by recrystallization from ethanol.

Refinement top

Atoms H2A and H2B of the NH2 group were located in difference Fourier maps and refined isotropically without restraint. Atom H1 was also located in a difference Fourier map and refined with the N—H distance restrained to be 1.01 (2) Å. All other H atoms were visible in difference Fourier maps but were placed at calculated positions and allowed to ride with C—H = 0.95 Å and Uiso(H) = 1.2Ueq(C) for aromatic H atoms, and with C—H = 0.98 Å and Uiso(H) = 1.5Ueq(C) for methyl H atoms.

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2000); software used to prepare material for publication: SHELXTL and X-SEED (Barbour, 2001).

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound with displacement ellipsoids drawn at the 50% probability level for non-H atoms.
[Figure 2] Fig. 2. N—H···O hydrogen bonds connect the molecules into double chains along the b axis.
4-Methylbenzenesulfonohydrazide top
Crystal data top
C7H10N2O2SF000 = 392
Mr = 186.23Dx = 1.484 Mg m3
Monoclinic, P21/cMelting point: 382 K
Hall symbol: -P 2ybcMo Kα radiation
λ = 0.71073 Å
a = 8.4166 (8) ÅCell parameters from 5282 reflections
b = 5.6056 (5) Åθ = 2.3–26.0º
c = 17.9484 (17) ŵ = 0.35 mm1
β = 100.260 (1)ºT = 100 (2) K
V = 833.27 (13) Å3Block, colourless
Z = 40.30 × 0.18 × 0.10 mm
Data collection top
Bruker APEX CCD
diffractometer
1641 independent reflections
Radiation source: fine-focus sealed tube1584 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.034
T = 100(2) Kθmax = 26.0º
φ and ω scansθmin = 2.3º
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 10→10
Tmin = 0.903, Tmax = 0.966k = 6→6
8195 measured reflectionsl = 22→22
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)] = 0.060H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.117  w = 1/[σ2(Fo2) + (0.0212P)2 + 1.9226P]
where P = (Fo2 + 2Fc2)/3
S = 1.30(Δ/σ)max = 0.001
1641 reflectionsΔρmax = 0.65 e Å3
122 parametersΔρmin = 0.31 e Å3
1 restraintExtinction correction: none
Primary atom site location: structure-invariant direct methods
Crystal data top
C7H10N2O2SV = 833.27 (13) Å3
Mr = 186.23Z = 4
Monoclinic, P21/cMo Kα
a = 8.4166 (8) ŵ = 0.35 mm1
b = 5.6056 (5) ÅT = 100 (2) K
c = 17.9484 (17) Å0.30 × 0.18 × 0.10 mm
β = 100.260 (1)º
Data collection top
Bruker APEX CCD
diffractometer
1641 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
1584 reflections with I > 2σ(I)
Tmin = 0.903, Tmax = 0.966Rint = 0.034
8195 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0601 restraint
wR(F2) = 0.117H atoms treated by a mixture of
independent and constrained refinement
S = 1.30Δρmax = 0.65 e Å3
1641 reflectionsΔρmin = 0.31 e Å3
122 parameters
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 > 2sigma(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
S10.27606 (8)0.14178 (13)0.17916 (4)0.0144 (2)
O10.4359 (2)0.0492 (4)0.20362 (12)0.0207 (5)
O20.1440 (2)0.0239 (4)0.16470 (12)0.0184 (5)
N10.2469 (3)0.3220 (5)0.24704 (14)0.0173 (6)
H10.346 (3)0.402 (5)0.2665 (17)0.015 (8)*
N20.1052 (3)0.4620 (5)0.22597 (16)0.0191 (6)
H2A0.130 (4)0.605 (7)0.215 (2)0.026 (10)*
H2B0.056 (4)0.467 (7)0.266 (2)0.027 (10)*
C10.2708 (3)0.3161 (5)0.09705 (16)0.0149 (6)
C20.3625 (4)0.5216 (6)0.10103 (17)0.0179 (6)
H20.42790.56810.14750.021*
C30.3581 (4)0.6590 (6)0.03662 (17)0.0204 (7)
H30.42150.80010.03920.024*
C40.2624 (4)0.5941 (6)0.03207 (17)0.0182 (6)
C50.1721 (4)0.3860 (6)0.03418 (18)0.0252 (7)
H50.10700.33830.08060.030*
C60.1747 (4)0.2466 (6)0.02964 (17)0.0207 (7)
H60.11160.10530.02730.025*
C70.2553 (4)0.7451 (7)0.10152 (18)0.0256 (7)
H7A0.27190.64440.14410.038*
H7B0.34000.86710.09230.038*
H7C0.14950.82250.11360.038*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0148 (4)0.0132 (4)0.0152 (4)0.0006 (3)0.0022 (3)0.0006 (3)
O10.0182 (11)0.0210 (11)0.0221 (12)0.0033 (9)0.0017 (9)0.0038 (9)
O20.0199 (11)0.0146 (11)0.0210 (11)0.0003 (9)0.0045 (9)0.0008 (9)
C50.0239 (16)0.0307 (19)0.0185 (16)0.0005 (14)0.0029 (13)0.0018 (14)
C10.0130 (13)0.0165 (15)0.0148 (14)0.0025 (11)0.0017 (11)0.0025 (12)
N10.0162 (12)0.0191 (14)0.0159 (12)0.0016 (11)0.0008 (10)0.0001 (10)
N20.0186 (13)0.0181 (14)0.0216 (14)0.0017 (11)0.0058 (11)0.0009 (12)
C20.0168 (14)0.0209 (16)0.0155 (14)0.0011 (12)0.0015 (12)0.0037 (12)
C60.0198 (15)0.0197 (16)0.0213 (16)0.0022 (13)0.0002 (12)0.0004 (13)
C30.0197 (15)0.0192 (16)0.0229 (16)0.0009 (13)0.0053 (12)0.0015 (13)
C70.0247 (17)0.0330 (19)0.0193 (16)0.0039 (15)0.0042 (13)0.0066 (14)
C40.0171 (14)0.0201 (16)0.0182 (15)0.0070 (12)0.0054 (12)0.0022 (12)
Geometric parameters (Å, °) top
S1—O11.436 (2)N2—H2A0.86 (4)
S1—O21.436 (2)N2—H2B0.89 (4)
S1—N11.635 (3)C2—C31.384 (4)
S1—C11.762 (3)C2—H20.950
C5—C61.384 (4)C6—H60.950
C5—C41.389 (5)C3—C41.395 (4)
C5—H50.950C3—H30.950
C1—C21.381 (4)C7—C41.499 (4)
C1—C61.386 (4)C7—H7A0.980
N1—N21.422 (4)C7—H7B0.980
N1—H10.96 (2)C7—H7C0.980
O1—S1—O2118.33 (13)C1—C2—C3119.3 (3)
O1—S1—N1104.61 (13)C1—C2—H2120.3
O2—S1—N1108.68 (13)C3—C2—H2120.3
O1—S1—C1109.81 (13)C5—C6—C1119.0 (3)
O2—S1—C1107.70 (13)C5—C6—H6120.5
N1—S1—C1107.22 (14)C1—C6—H6120.5
C6—C5—C4121.6 (3)C2—C3—C4121.2 (3)
C6—C5—H5119.2C2—C3—H3119.4
C4—C5—H5119.2C4—C3—H3119.4
C2—C1—C6120.9 (3)C4—C7—H7A109.5
C2—C1—S1119.2 (2)C4—C7—H7B109.5
C6—C1—S1119.9 (2)H7A—C7—H7B109.5
N2—N1—S1111.91 (19)C4—C7—H7C109.5
N2—N1—H1118 (2)H7A—C7—H7C109.5
S1—N1—H1108.8 (19)H7B—C7—H7C109.5
N1—N2—H2A110 (2)C5—C4—C3118.0 (3)
N1—N2—H2B107 (2)C5—C4—C7120.7 (3)
H2A—N2—H2B109 (3)C3—C4—C7121.3 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.96 (2)2.00 (2)2.948 (3)173 (3)
N2—H2A···O2ii0.86 (4)2.28 (4)3.122 (4)167 (3)
N2—H2B···O2iii0.89 (4)2.27 (4)3.118 (3)160 (3)
Symmetry codes: (i) −x+1, y+1/2, −z+1/2; (ii) x, y+1, z; (iii) −x, y+1/2, −z+1/2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.96 (2)2.00 (2)2.948 (3)173 (3)
N2—H2A···O2ii0.86 (4)2.28 (4)3.122 (4)167 (3)
N2—H2B···O2iii0.89 (4)2.27 (4)3.118 (3)160 (3)
Symmetry codes: (i) −x+1, y+1/2, −z+1/2; (ii) x, y+1, z; (iii) −x, y+1/2, −z+1/2.
Acknowledgements top

AN thanks DST (SR/S5/OC-02/2002) for financial assistance. SR thanks the UGC for a fellowship.

references
References top

Barbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.

Bruker (1997). SMART (Version 5.054) and SAINT (Version ?). Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2000). SHELXTL. Versions 6.10 and 6.12. Bruker AXS Inc., Madison, Wisconsin, USA.

Friedman, L., Litle, R. L. & Reichle, W. R. (1973). Org. Synth. Coll. Vol. V, pp. 1055–1057.

Lightfoot, P., Tremayne, M., Glidewell, C., Harris, K. D. M. & Bruce, P. G. (1993). J. Chem. Soc. Perkin Trans. 2, pp. 1625–1630.

Sheldrick, G. M. (1997). SHELXL97 and SHELXS97. University of Göttingen, Germany.

Sheldrick, G. M. (2003). SADABS. Version 2.10. University of Göttingen, Germany.