Abstract
The title compound, C9H11N3OS, was prepared by the reaction of 3-methoxybenzaldehyde and thiosemicarbazide. The benzylidene ring and the thiosemicarbazone fragment are slightly twisted, making a dihedral angle of 14.1 (1)°. A weak intramolecular N—H⋯N hydrogen bond may influence the conformation of the molecule. Intermolecular N—H⋯S hydrogen bonds build up a three-dimensional network.
Related literature
For a general background to thiosemicarbazone compounds, see: Casas et al. (2000 ▶); Tarafder et al. (2000 ▶); Ferrari et al. (2000 ▶); Deschamps et al. (2003 ▶); Maccioni et al. (2003 ▶); Chimenti et al.(2007 ▶). For bond-length data, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C9H11N3OS
M r = 209.27
Monoclinic,
a = 11.814 (2) Å
b = 5.6760 (11) Å
c = 15.248 (3) Å
β = 90.29 (3)°
V = 1022.5 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.29 mm−1
T = 293 K
0.30 × 0.20 × 0.10 mm
Data collection
Enraf–Nonius CAD-4 diffractometer
Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.908, T max = 0.969
1946 measured reflections
1852 independent reflections
1494 reflections with I > 2σ(I)
R int = 0.017
3 standard reflections every 200 reflections intensity decay: 9%
Refinement
R[F 2 > 2σ(F 2)] = 0.041
wR(F 2) = 0.110
S = 1.06
1852 reflections
128 parameters
H-atom parameters constrained
Δρmax = 0.20 e Å−3
Δρmin = −0.26 e Å−3
Data collection: CAD-4 Software (Enraf–Nonius, 1989 ▶); cell refinement: CAD-4 Software; data reduction: XCAD4 (Harms & Wocadlo, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053680901040X/dn2432sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053680901040X/dn2432Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N2—H2⋯S1i | 0.86 | 2.57 | 3.370 (2) | 156 |
| N3—H3B⋯S1ii | 0.86 | 2.57 | 3.411 (2) | 166 |
| N3—H3A⋯N1 | 0.86 | 2.25 | 2.611 (3) | 105 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors thank the Center of Testing and Analysis, Nanjing University, for support.
supplementary crystallographic information
Comment
Thiosemicarbazones constitute an important class of N,S donor ligands due to their propensity to react with a wide range of metals (Casas et al., 2000). Thiosemicarbazones exhibit various biological activities and have therefore attracted considerable pharmaceutical interest (Maccioni et al., 2003; Ferrari et al., 2000). They have been evaluated as antiviral, antibacterial and anticancer therapeutics. Thiosemicarbazones belong to a large group of thiourea derivatives, whose biological activities are a function of parent aldehyde or ketone moiety (Chimenti et al., 2007). Schiff bases show potential as antimicrobial and anticancer agents (Tarafder et al., 2000; Deschamps et al., 2003) and so have biochemical and pharmacological applications. We here report the crystal structure of the title compound (I).
The sulfur atom and the hydrazine nitrogen N1 are in trans position with respect to the C9–N2 bond. This conformation may be induced by the weak intramolecular N-H···N hydrogen bond (Fig. 1, Table 1). All bond lengths are within normal ranges (Allen et al., 1987).
At first glance the molecule is roughly planar with the largest deviation from the mean plane being -0.272 (3) Å at N3, however the benzaldehyde ring and the thiosemicarbazone fragment are twisted with respect to each other making a dihedral angle of 14.1 (1)°.
The molecules are connected by intermolecular N—H···S hydrogen bonds which build up a three dimensional network (Table 1, Fig.2).
Experimental
A mixture of 3-methoxybenzaldehyde (1.36 g, 0.01 mol) and hydrazinecarbothioamide (0.91 g, 0.01 mol) in 20 ml of absolute methanol was refluxed for about 3 h. On cooling, the solid separated was filtered and recrystallized from ethyl acetate. Crystals of (I) suitable for X-ray diffraction were obtained by slow evaporation of ethyl acetate. 1H NMR (DMSO, δ, p.p.m.) 11.39 (s, 1 H), 8.17 (s, 1 H), 8.02 (s,2 H), 7.42 (m, 1 H), 7.30 (t, 2 H), 6.99 (t,1 H), 3.79 (t, 3 H).
Refinement
All H atoms were positioned geometrically, with C—H = 0.93 Å (aromatic) or 0.96 Å (methyl) and N—H = 0.86 Å, and constrained to ride on their parent atoms, with Uiso(H) = xUeq(C), where x= 1.5 for methyl H and x = 1.2 for C(aromatic) and N atoms.
Figures
Fig. 1.
A view of the molecular structure of (I) showing the atom-numbering scheme and 30% displacement ellipsoids. H atoms are represented as smal sphere of arbitrary radii. Intramolecular hydrogen bond is shown as dashed line.
Fig. 2.
Partial packing view showing the N-H···S hydrogen bonds network. H atoms not involved in hydrogen bonding have been omitted for clarity. H bonds are shown as dashed lines. [Symmetry codes: (i) -x+1, -y+3, -z+1; (ii) -x+1, y-1/2, -z+1/2]
Crystal data
| C9H11N3OS | F(000) = 440 |
| Mr = 209.27 | Dx = 1.359 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 27 reflections |
| a = 11.814 (2) Å | θ = 1–25° |
| b = 5.6760 (11) Å | µ = 0.29 mm−1 |
| c = 15.248 (3) Å | T = 293 K |
| β = 90.29 (3)° | Block, colorless |
| V = 1022.5 (3) Å3 | 0.30 × 0.20 × 0.10 mm |
| Z = 4 |
Data collection
| Enraf–Nonius CAD-4 diffractometer | 1494 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.017 |
| graphite | θmax = 25.3°, θmin = 1.7° |
| ω/2θ scans | h = −14→0 |
| Absorption correction: ψ scan (North et al., 1968) | k = 0→6 |
| Tmin = 0.908, Tmax = 0.969 | l = −18→18 |
| 1946 measured reflections | 3 standard reflections every 200 reflections |
| 1852 independent reflections | intensity decay: 9% |
Refinement
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.110 | H-atom parameters constrained |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.0521P)2 + 0.3815P] where P = (Fo2 + 2Fc2)/3 |
| 1852 reflections | (Δ/σ)max < 0.001 |
| 128 parameters | Δρmax = 0.20 e Å−3 |
| 0 restraints | Δρmin = −0.26 e Å−3 |
Special details
| Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 | ||
| S1 | 0.51511 (6) | 1.47619 (10) | 0.35880 (3) | 0.0442 (2) | |
| O1 | 0.85492 (14) | 0.6407 (3) | 0.83956 (9) | 0.0496 (5) | |
| N1 | 0.66878 (15) | 1.0213 (3) | 0.50804 (11) | 0.0369 (4) | |
| N2 | 0.60984 (16) | 1.2149 (3) | 0.47967 (11) | 0.0407 (5) | |
| H2 | 0.5936 | 1.3268 | 0.5155 | 0.049* | |
| N3 | 0.59915 (18) | 1.0451 (4) | 0.34546 (12) | 0.0497 (5) | |
| H3A | 0.6324 | 0.9237 | 0.3674 | 0.060* | |
| H3B | 0.5800 | 1.0463 | 0.2910 | 0.060* | |
| C1 | 0.9085 (2) | 0.4449 (6) | 0.88050 (16) | 0.0614 (8) | |
| H1A | 0.9862 | 0.4377 | 0.8627 | 0.092* | |
| H1B | 0.8706 | 0.3024 | 0.8634 | 0.092* | |
| H1C | 0.9049 | 0.4624 | 0.9430 | 0.092* | |
| C2 | 0.84356 (18) | 0.6327 (4) | 0.75008 (14) | 0.0383 (5) | |
| C3 | 0.77906 (17) | 0.8120 (4) | 0.71427 (13) | 0.0366 (5) | |
| H3 | 0.7479 | 0.9264 | 0.7505 | 0.044* | |
| C4 | 0.76070 (17) | 0.8221 (4) | 0.62447 (13) | 0.0350 (5) | |
| C5 | 0.8097 (2) | 0.6510 (4) | 0.57024 (14) | 0.0428 (6) | |
| H5 | 0.7982 | 0.6566 | 0.5099 | 0.051* | |
| C6 | 0.8741 (2) | 0.4764 (4) | 0.60621 (16) | 0.0503 (6) | |
| H6 | 0.9071 | 0.3642 | 0.5700 | 0.060* | |
| C7 | 0.8914 (2) | 0.4638 (4) | 0.69715 (16) | 0.0472 (6) | |
| H7 | 0.9346 | 0.3430 | 0.7214 | 0.057* | |
| C8 | 0.69256 (18) | 1.0136 (4) | 0.58932 (13) | 0.0379 (5) | |
| H8 | 0.6663 | 1.1311 | 0.6265 | 0.045* | |
| C9 | 0.57769 (17) | 1.2279 (4) | 0.39499 (13) | 0.0332 (5) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0643 (4) | 0.0374 (3) | 0.0309 (3) | 0.0090 (3) | −0.0081 (3) | 0.0035 (2) |
| O1 | 0.0534 (10) | 0.0621 (12) | 0.0333 (8) | 0.0106 (9) | −0.0062 (7) | 0.0109 (8) |
| N1 | 0.0429 (10) | 0.0363 (10) | 0.0315 (9) | 0.0058 (9) | −0.0045 (8) | 0.0024 (8) |
| N2 | 0.0555 (12) | 0.0378 (11) | 0.0286 (9) | 0.0118 (9) | −0.0091 (8) | −0.0020 (8) |
| N3 | 0.0732 (14) | 0.0442 (12) | 0.0315 (9) | 0.0164 (11) | −0.0128 (9) | −0.0056 (9) |
| C1 | 0.0631 (16) | 0.077 (2) | 0.0444 (14) | 0.0194 (15) | −0.0057 (12) | 0.0225 (14) |
| C2 | 0.0335 (11) | 0.0471 (14) | 0.0343 (11) | −0.0031 (10) | −0.0041 (9) | 0.0072 (10) |
| C3 | 0.0338 (11) | 0.0429 (13) | 0.0331 (11) | 0.0020 (10) | 0.0002 (9) | 0.0024 (10) |
| C4 | 0.0331 (11) | 0.0380 (12) | 0.0340 (11) | −0.0035 (10) | −0.0043 (9) | 0.0045 (10) |
| C5 | 0.0526 (14) | 0.0413 (14) | 0.0346 (11) | 0.0013 (11) | −0.0061 (10) | −0.0020 (10) |
| C6 | 0.0622 (16) | 0.0432 (14) | 0.0454 (13) | 0.0109 (12) | −0.0051 (12) | −0.0084 (11) |
| C7 | 0.0517 (14) | 0.0401 (13) | 0.0497 (14) | 0.0076 (11) | −0.0091 (11) | 0.0061 (11) |
| C8 | 0.0389 (11) | 0.0439 (13) | 0.0309 (11) | 0.0039 (10) | −0.0012 (9) | 0.0002 (10) |
| C9 | 0.0372 (11) | 0.0357 (12) | 0.0266 (10) | −0.0032 (10) | −0.0024 (8) | 0.0015 (9) |
Geometric parameters (Å, °)
| S1—C9 | 1.683 (2) | C2—C7 | 1.377 (3) |
| O1—C2 | 1.371 (2) | C2—C3 | 1.382 (3) |
| O1—C1 | 1.422 (3) | C3—C4 | 1.386 (3) |
| N1—C8 | 1.270 (3) | C3—H3 | 0.9300 |
| N1—N2 | 1.370 (2) | C4—C5 | 1.402 (3) |
| N2—C9 | 1.346 (3) | C4—C8 | 1.454 (3) |
| N2—H2 | 0.8600 | C5—C6 | 1.363 (3) |
| N3—C9 | 1.309 (3) | C5—H5 | 0.9300 |
| N3—H3A | 0.8600 | C6—C7 | 1.402 (3) |
| N3—H3B | 0.8600 | C6—H6 | 0.9300 |
| C1—H1A | 0.9600 | C7—H7 | 0.9300 |
| C1—H1B | 0.9600 | C8—H8 | 0.9300 |
| C1—H1C | 0.9600 | ||
| C2—O1—C1 | 116.9 (2) | C4—C3—H3 | 119.9 |
| C8—N1—N2 | 116.44 (18) | C3—C4—C5 | 119.4 (2) |
| C9—N2—N1 | 119.16 (18) | C3—C4—C8 | 118.6 (2) |
| C9—N2—H2 | 120.4 | C5—C4—C8 | 122.00 (19) |
| N1—N2—H2 | 120.4 | C6—C5—C4 | 119.8 (2) |
| C9—N3—H3A | 120.0 | C6—C5—H5 | 120.1 |
| C9—N3—H3B | 120.0 | C4—C5—H5 | 120.1 |
| H3A—N3—H3B | 120.0 | C5—C6—C7 | 120.9 (2) |
| O1—C1—H1A | 109.5 | C5—C6—H6 | 119.6 |
| O1—C1—H1B | 109.5 | C7—C6—H6 | 119.6 |
| H1A—C1—H1B | 109.5 | C2—C7—C6 | 119.1 (2) |
| O1—C1—H1C | 109.5 | C2—C7—H7 | 120.5 |
| H1A—C1—H1C | 109.5 | C6—C7—H7 | 120.5 |
| H1B—C1—H1C | 109.5 | N1—C8—C4 | 120.3 (2) |
| O1—C2—C7 | 124.6 (2) | N1—C8—H8 | 119.8 |
| O1—C2—C3 | 114.8 (2) | C4—C8—H8 | 119.8 |
| C7—C2—C3 | 120.6 (2) | N3—C9—N2 | 117.1 (2) |
| C2—C3—C4 | 120.2 (2) | N3—C9—S1 | 124.11 (16) |
| C2—C3—H3 | 119.9 | N2—C9—S1 | 118.78 (16) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2···S1i | 0.86 | 2.57 | 3.370 (2) | 156 |
| N3—H3B···S1ii | 0.86 | 2.57 | 3.411 (2) | 166 |
| N3—H3A···N1 | 0.86 | 2.25 | 2.611 (3) | 105 |
Symmetry codes: (i) −x+1, −y+3, −z+1; (ii) −x+1, y−1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2432).
References
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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 global, I. DOI: 10.1107/S160053680901040X/dn2432sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053680901040X/dn2432Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


