Abstract
In the title thiourea derivative, C10H17N3O2S, the carboxyl group and the least-squares plane through the cyclohexyl ring are twisted out of the plane through the central CN3S residue; the respective dihedral angles are 7.18 (8) and 62.29 (4)°. The conformation about the azomethine bond [1.275 (2) Å] is E. The NH groups are anti, with one forming an intramolecular N—H⋯N hydrogen bond. The main feature of the crystal structure is the formation of linear supramolecular chains along [110] mediated by alternating pairs of O—H⋯O and pairs of N—H⋯S hydrogen bonds.
Related literature
For related thiourea structures, see: Normaya et al. (2011 ▶); Salam et al. (2011 ▶).
Experimental
Crystal data
C10H17N3O2S
M r = 243.33
Monoclinic,
a = 8.9204 (2) Å
b = 6.0350 (2) Å
c = 22.4750 (6) Å
β = 90.051 (3)°
V = 1209.93 (6) Å3
Z = 4
Mo Kα radiation
μ = 0.26 mm−1
T = 100 K
0.30 × 0.20 × 0.10 mm
Data collection
Agilent Supernova Dual diffractometer with an Atlas detector
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010 ▶) T min = 0.687, T max = 1.000
7394 measured reflections
2723 independent reflections
2251 reflections with I > 2σ(I)
R int = 0.036
Refinement
R[F 2 > 2σ(F 2)] = 0.041
wR(F 2) = 0.143
S = 0.98
2723 reflections
158 parameters
3 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.36 e Å−3
Δρmin = −0.32 e Å−3
Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811014449/hb5851sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014449/hb5851Isup2.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 |
|---|---|---|---|---|
| N3—H3⋯N1 | 0.87 (1) | 2.20 (2) | 2.574 (2) | 106 (2) |
| O1—H1⋯O2i | 0.85 (1) | 1.80 (1) | 2.6416 (17) | 172 (3) |
| N2—H2⋯S1ii | 0.89 (1) | 2.65 (1) | 3.5384 (15) | 176 (2) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported financially by the Ministry of Science, Technology and Innovation (MOSTI) under a research grant (No. 06-01-09-SF0046). The authors thank Universiti Malaysia Sarawak (UNIMAS) for the facilities to carry out the research work. The authors also thank the University of Malaya for support of the crystallographic facility.
supplementary crystallographic information
Comment
In continuation of structural investigations into conformation and hydrogen bonding in thiourea derivatives (Normaya et al. 2011; Salam et al., 2011), the title compound, (I), was investigated.
The central CN3S chromophore in (I), Fig. 1, is planar (r.m.s. = 0.0039 Å). The carboxylate residue is slightly twisted out this plane (dihedral angle = 7.18 (8) °), and, by contrast, the least-squares plane through the cyclohexyl group (which has the conformation of a chair) is twisted significantly out of the central plane (dihedral angle = 62.29 (4) °). The H atoms of the NH groups are anti, and the conformation about the azomethine bond [1.275 (2) Å] is E. The N3—H forms an intramolecular hydrogen bond with the imino-N3 atom, Table 1. Finally, the thione and carboxylic acid groups lie to opposite sides of the molecule. This arrangements enables the formation of linear supramolecular chains via hydrogen bonds along [110] in the crystal packing, Fig. 2 and Table 1. The carboxylic acid residues self-associate via a centrosymmetric eight-membered {···HOC═O}2 synthon. Similarly, the thiourea entity with the NH atom not involved in the intramolecular N—H···N interaction, self-associates via a centrosymmetric eight-membered {···HNC═ S}2 synthon. Chains lie in the ab plane with the cyclohexyl rings inter-digitating along the c axis, Fig. 3.
Experimental
Cyclohexylisothiocyanate (0.706 g, 5 mmol) and hydrazine hydrate (0.250 g, 5 mmol), each dissolved in 10 ml e thanol were mixed with constant stirring. The stirring was continued for 30 min and the white product that formed, N(4)-cyclohexylthiosemicarbazide, was washed with ethanol and dried in vacuo. A solution of this (0.51 g, 3 mmol) in 10 ml me thanol was refluxed with a methanolic solution of pyruvic acid (0.261 g, 3 mmol) for 5 h after the addition of 1–2 drops of glacial acetic acid. On cooling the solution to room temperature, white precipitate separated, which were filtered and washed with methanol. The white precipitate was recrystallized from methanol to yield colourless prisms and dried in vacuo over silica gel. (M.pt. 465–467 K. Yield 0.621 g (80%). Anal. Found: C, 49.31; H, 7.01; N, 17.18%. C10H17N3O2S requires: C, 49.36; H, 7.04; N, 17.26%. FT—IR (KBr, cm-1) νmax: 3322 (m, OH), 3197 (s, NH), 2922, 2851 (s, cyclohexyl), 1692 (m, C═O), 1619 (w, C═N), 980 (m, N—N), 1249, 873 (w, C═S).
Refinement
Carbon-bound H-atoms were placed in calculated positions (C–H = 0.98 to 1.00 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2–1.5Ueq(C). The O– and N-bound H-atoms were located in a difference Fourier map and were refined with distance restraints of O—H = 0.84±0.01 Å and N—H 0.88±0.01 Å, and with Uiso(H) = yUeq(N) for y = 1.5 (O) and 1.2 (N).
Figures
Fig. 1.
The molecular structure of (I) showing displacement ellipsoids at the 50% probability level.
Fig. 2.
A view of the supramolecular chain aligned along [110] in (I). The O—H···O and N—H···S hydrogen bonds are shown as orange and blue dashed lines, respectively.
Fig. 3.

A view in projection down the b axis of the crystal packing in (I) showing the inter-digitation of the cyclohexyl rings along the c direction. The O—H···O and N—H···S hydrogen bonds are shown as orange and blue dashed lines, respectively.
Crystal data
| C10H17N3O2S | F(000) = 520 |
| Mr = 243.33 | Dx = 1.336 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 3312 reflections |
| a = 8.9204 (2) Å | θ = 2.3–29.1° |
| b = 6.0350 (2) Å | µ = 0.26 mm−1 |
| c = 22.4750 (6) Å | T = 100 K |
| β = 90.051 (3)° | Prism, colourless |
| V = 1209.93 (6) Å3 | 0.30 × 0.20 × 0.10 mm |
| Z = 4 |
Data collection
| Agilent Supernova Dual diffractometer with an Atlas detector | 2723 independent reflections |
| Radiation source: SuperNova (Mo) X-ray Source | 2251 reflections with I > 2σ(I) |
| Mirror | Rint = 0.036 |
| Detector resolution: 10.4041 pixels mm-1 | θmax = 27.5°, θmin = 2.5° |
| ω scans | h = −11→11 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −6→7 |
| Tmin = 0.687, Tmax = 1.000 | l = −29→29 |
| 7394 measured reflections |
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) = 0.143 | H atoms treated by a mixture of independent and constrained refinement |
| S = 0.98 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
| 2723 reflections | (Δ/σ)max = 0.001 |
| 158 parameters | Δρmax = 0.36 e Å−3 |
| 3 restraints | Δρmin = −0.32 e Å−3 |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| S1 | 1.07001 (5) | 1.46426 (7) | 0.59008 (2) | 0.01940 (18) | |
| O1 | 0.65476 (14) | 0.6300 (2) | 0.54143 (6) | 0.0209 (3) | |
| O2 | 0.53180 (13) | 0.7099 (2) | 0.45694 (6) | 0.0196 (3) | |
| N1 | 0.80028 (16) | 1.0010 (2) | 0.53480 (7) | 0.0156 (3) | |
| N2 | 0.88614 (16) | 1.1878 (2) | 0.53543 (7) | 0.0170 (3) | |
| N3 | 0.94326 (16) | 1.0938 (3) | 0.63114 (7) | 0.0169 (3) | |
| C1 | 0.62814 (18) | 0.7522 (3) | 0.49413 (8) | 0.0164 (4) | |
| C2 | 0.72145 (19) | 0.9564 (3) | 0.48899 (8) | 0.0162 (4) | |
| C3 | 0.7098 (2) | 1.0904 (3) | 0.43363 (8) | 0.0211 (4) | |
| H3A | 0.6904 | 1.2455 | 0.4440 | 0.032* | |
| H3B | 0.6273 | 1.0339 | 0.4091 | 0.032* | |
| H3C | 0.8039 | 1.0800 | 0.4113 | 0.032* | |
| C4 | 0.96146 (18) | 1.2376 (3) | 0.58689 (8) | 0.0156 (4) | |
| C5 | 1.00682 (18) | 1.1176 (3) | 0.69060 (7) | 0.0157 (4) | |
| H5 | 1.1055 | 1.1951 | 0.6871 | 0.019* | |
| C6 | 1.0336 (2) | 0.8900 (3) | 0.71759 (9) | 0.0210 (4) | |
| H6A | 1.1037 | 0.8054 | 0.6921 | 0.025* | |
| H6B | 0.9377 | 0.8076 | 0.7194 | 0.025* | |
| C7 | 1.0991 (2) | 0.9113 (3) | 0.78024 (8) | 0.0221 (4) | |
| H7A | 1.1116 | 0.7618 | 0.7977 | 0.026* | |
| H7B | 1.1994 | 0.9811 | 0.7779 | 0.026* | |
| C8 | 0.9984 (2) | 1.0501 (3) | 0.82063 (9) | 0.0235 (4) | |
| H8A | 0.9019 | 0.9725 | 0.8267 | 0.028* | |
| H8B | 1.0471 | 1.0689 | 0.8599 | 0.028* | |
| C9 | 0.9696 (2) | 1.2771 (3) | 0.79289 (9) | 0.0250 (4) | |
| H9A | 0.8988 | 1.3610 | 0.8182 | 0.030* | |
| H9B | 1.0648 | 1.3611 | 0.7912 | 0.030* | |
| C10 | 0.9048 (2) | 1.2561 (3) | 0.73033 (8) | 0.0212 (4) | |
| H10A | 0.8046 | 1.1858 | 0.7325 | 0.025* | |
| H10B | 0.8924 | 1.4055 | 0.7128 | 0.025* | |
| H1 | 0.602 (2) | 0.514 (3) | 0.5431 (12) | 0.040 (7)* | |
| H2 | 0.892 (2) | 1.275 (3) | 0.5035 (6) | 0.026 (6)* | |
| H3 | 0.888 (2) | 0.976 (2) | 0.6260 (11) | 0.029 (6)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0251 (3) | 0.0177 (3) | 0.0154 (3) | −0.00825 (16) | −0.0030 (2) | 0.00088 (18) |
| O1 | 0.0233 (6) | 0.0208 (7) | 0.0185 (7) | −0.0089 (5) | −0.0048 (5) | 0.0055 (6) |
| O2 | 0.0200 (6) | 0.0205 (7) | 0.0182 (7) | −0.0064 (5) | −0.0030 (5) | 0.0018 (5) |
| N1 | 0.0148 (7) | 0.0144 (7) | 0.0178 (8) | −0.0030 (5) | 0.0009 (6) | −0.0010 (6) |
| N2 | 0.0214 (7) | 0.0140 (7) | 0.0157 (8) | −0.0039 (6) | −0.0007 (6) | 0.0036 (6) |
| N3 | 0.0196 (7) | 0.0172 (7) | 0.0140 (8) | −0.0068 (6) | −0.0047 (6) | 0.0006 (6) |
| C1 | 0.0159 (8) | 0.0178 (9) | 0.0155 (9) | 0.0010 (7) | 0.0000 (7) | −0.0017 (7) |
| C2 | 0.0153 (8) | 0.0168 (9) | 0.0166 (9) | −0.0015 (6) | 0.0005 (7) | 0.0006 (7) |
| C3 | 0.0247 (9) | 0.0215 (9) | 0.0169 (9) | −0.0069 (7) | −0.0040 (7) | 0.0022 (8) |
| C4 | 0.0154 (8) | 0.0160 (8) | 0.0155 (8) | −0.0002 (6) | 0.0004 (7) | −0.0008 (7) |
| C5 | 0.0173 (8) | 0.0184 (9) | 0.0112 (8) | −0.0030 (7) | −0.0038 (6) | −0.0006 (7) |
| C6 | 0.0255 (9) | 0.0168 (9) | 0.0208 (9) | 0.0006 (7) | 0.0006 (8) | −0.0003 (8) |
| C7 | 0.0266 (9) | 0.0186 (9) | 0.0210 (10) | 0.0007 (7) | −0.0032 (8) | 0.0036 (8) |
| C8 | 0.0301 (10) | 0.0263 (10) | 0.0141 (9) | −0.0050 (8) | −0.0001 (8) | −0.0016 (8) |
| C9 | 0.0318 (10) | 0.0241 (10) | 0.0191 (9) | 0.0032 (8) | −0.0004 (8) | −0.0057 (8) |
| C10 | 0.0255 (9) | 0.0197 (9) | 0.0185 (9) | 0.0037 (7) | −0.0007 (8) | −0.0011 (8) |
Geometric parameters (Å, °)
| S1—C4 | 1.6774 (18) | C5—C10 | 1.525 (2) |
| O1—C1 | 1.315 (2) | C5—H5 | 1.0000 |
| O1—H1 | 0.845 (10) | C6—C7 | 1.530 (3) |
| O2—C1 | 1.225 (2) | C6—H6A | 0.9900 |
| N1—C2 | 1.275 (2) | C6—H6B | 0.9900 |
| N1—N2 | 1.363 (2) | C7—C8 | 1.528 (3) |
| N2—C4 | 1.370 (2) | C7—H7A | 0.9900 |
| N2—H2 | 0.892 (9) | C7—H7B | 0.9900 |
| N3—C4 | 1.330 (2) | C8—C9 | 1.527 (3) |
| N3—C5 | 1.458 (2) | C8—H8A | 0.9900 |
| N3—H3 | 0.870 (9) | C8—H8B | 0.9900 |
| C1—C2 | 1.491 (2) | C9—C10 | 1.525 (3) |
| C2—C3 | 1.488 (3) | C9—H9A | 0.9900 |
| C3—H3A | 0.9800 | C9—H9B | 0.9900 |
| C3—H3B | 0.9800 | C10—H10A | 0.9900 |
| C3—H3C | 0.9800 | C10—H10B | 0.9900 |
| C5—C6 | 1.520 (3) | ||
| C1—O1—H1 | 113.7 (18) | C5—C6—H6A | 109.5 |
| C2—N1—N2 | 119.52 (15) | C7—C6—H6A | 109.5 |
| N1—N2—C4 | 117.71 (14) | C5—C6—H6B | 109.5 |
| N1—N2—H2 | 121.1 (14) | C7—C6—H6B | 109.5 |
| C4—N2—H2 | 121.2 (14) | H6A—C6—H6B | 108.1 |
| C4—N3—C5 | 124.97 (14) | C8—C7—C6 | 111.63 (15) |
| C4—N3—H3 | 120.2 (16) | C8—C7—H7A | 109.3 |
| C5—N3—H3 | 114.8 (16) | C6—C7—H7A | 109.3 |
| O2—C1—O1 | 124.08 (15) | C8—C7—H7B | 109.3 |
| O2—C1—C2 | 120.71 (15) | C6—C7—H7B | 109.3 |
| O1—C1—C2 | 115.18 (15) | H7A—C7—H7B | 108.0 |
| N1—C2—C3 | 126.77 (15) | C9—C8—C7 | 110.38 (16) |
| N1—C2—C1 | 114.80 (15) | C9—C8—H8A | 109.6 |
| C3—C2—C1 | 118.38 (15) | C7—C8—H8A | 109.6 |
| C2—C3—H3A | 109.5 | C9—C8—H8B | 109.6 |
| C2—C3—H3B | 109.5 | C7—C8—H8B | 109.6 |
| H3A—C3—H3B | 109.5 | H8A—C8—H8B | 108.1 |
| C2—C3—H3C | 109.5 | C10—C9—C8 | 111.43 (15) |
| H3A—C3—H3C | 109.5 | C10—C9—H9A | 109.3 |
| H3B—C3—H3C | 109.5 | C8—C9—H9A | 109.3 |
| N3—C4—N2 | 115.34 (15) | C10—C9—H9B | 109.3 |
| N3—C4—S1 | 124.83 (14) | C8—C9—H9B | 109.3 |
| N2—C4—S1 | 119.82 (13) | H9A—C9—H9B | 108.0 |
| N3—C5—C6 | 109.71 (14) | C5—C10—C9 | 111.06 (14) |
| N3—C5—C10 | 111.03 (14) | C5—C10—H10A | 109.4 |
| C6—C5—C10 | 110.79 (15) | C9—C10—H10A | 109.4 |
| N3—C5—H5 | 108.4 | C5—C10—H10B | 109.4 |
| C6—C5—H5 | 108.4 | C9—C10—H10B | 109.4 |
| C10—C5—H5 | 108.4 | H10A—C10—H10B | 108.0 |
| C5—C6—C7 | 110.56 (15) | ||
| C2—N1—N2—C4 | 175.80 (15) | C4—N3—C5—C6 | −151.10 (16) |
| N2—N1—C2—C3 | −0.7 (3) | C4—N3—C5—C10 | 86.1 (2) |
| N2—N1—C2—C1 | −178.00 (14) | N3—C5—C6—C7 | −179.54 (14) |
| O2—C1—C2—N1 | 169.21 (15) | C10—C5—C6—C7 | −56.59 (19) |
| O1—C1—C2—N1 | −8.9 (2) | C5—C6—C7—C8 | 56.5 (2) |
| O2—C1—C2—C3 | −8.4 (2) | C6—C7—C8—C9 | −55.6 (2) |
| O1—C1—C2—C3 | 173.52 (15) | C7—C8—C9—C10 | 55.2 (2) |
| C5—N3—C4—N2 | −177.12 (15) | N3—C5—C10—C9 | 178.84 (14) |
| C5—N3—C4—S1 | 4.2 (2) | C6—C5—C10—C9 | 56.7 (2) |
| N1—N2—C4—N3 | 0.7 (2) | C8—C9—C10—C5 | −56.1 (2) |
| N1—N2—C4—S1 | 179.49 (12) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N3—H3···N1 | 0.87 (1) | 2.20 (2) | 2.574 (2) | 106.(2) |
| O1—H1···O2i | 0.85 (1) | 1.80 (1) | 2.6416 (17) | 172 (3) |
| N2—H2···S1ii | 0.89 (1) | 2.65 (1) | 3.5384 (15) | 176.(2) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+2, −y+3, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB5851).
References
- Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
- Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Normaya, E., Farina, Y., Halim, S. N. A. & Tiekink, E. R. T. (2011). Acta Cryst. E67, o943–o944. [DOI] [PMC free article] [PubMed]
- Salam, M. A., Affan, M. A., Ahmad, F. B., Ng, S. W. & Tiekink, E. R. T. (2011). Acta Cryst. E67, o955. [DOI] [PMC free article] [PubMed]
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
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/S1600536811014449/hb5851sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014449/hb5851Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


