Abstract
The asymmetric unit of the title compound, C18H22N4S2, contains one half-molecule, the complete molecule being generated by crystallographic inversion symmetry. The crystal structure features two intermolecular N—H⋯S hydrogen-bonding interactions, the first generating an infinite chain along the b axis and the second an infinite chain along the a axis, together forming an interlocking structure.
Related literature
Thiourea derivatives are conspicuous for their biological activity as they form strong hydrogen-bonding interactions and coordinate to metal ions, see: Wittkopp & Schreiner (2003 ▶); Li et al. (2008 ▶). For appliactions of thiourea, see Abdallah et al. (2006 ▶); Karamé et al. (2003 ▶); Nan et al. (2000 ▶); Breuzard et al. (2000 ▶); Tommasino et al., (2000 ▶); Reinoso García et al. (2004 ▶); Leung et al. (2008 ▶). For synthesis of the title compound, see: Lee et al. (1985 ▶).
Experimental
Crystal data
C18H22N4S2
M r = 358.52
Monoclinic,
a = 9.6795 (3) Å
b = 7.8677 (3) Å
c = 12.3213 (4) Å
β = 105.816 (2)°
V = 902.81 (5) Å3
Z = 2
Mo Kα radiation
μ = 0.30 mm−1
T = 173 K
0.46 × 0.45 × 0.13 mm
Data collection
Bruker APEXII CCD diffractometer
9210 measured reflections
2192 independent reflections
1710 reflections with I > 2σ(I)
R int = 0.042
Refinement
R[F 2 > 2σ(F 2)] = 0.034
wR(F 2) = 0.093
S = 1.06
2192 reflections
117 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.45 e Å−3
Δρmin = −0.23 e Å−3
Data collection: APEX2 (Bruker, 2006 ▶); cell refinement: SAINT-Plus (Bruker, 2006 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: OLEX2 (Dolomanov et al., 2009 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811033071/om2458sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033071/om2458Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811033071/om2458Isup3.cml
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 |
|---|---|---|---|---|
| N1—H1N⋯S1i | 0.855 (18) | 2.508 (18) | 3.3465 (13) | 167.1 (15) |
| N2—H2N⋯S1ii | 0.806 (15) | 2.713 (16) | 3.3755 (14) | 140.7 (13) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors wish to thank Dr Manuel Fernandes from the Chemistry Department of the University of the Witwatersrand for his assistance with the data collection and c*change for financial support.
supplementary crystallographic information
Comment
Thiourea derivatives are conspicuous for their biological activity as they form strong hydrogen bonding interactions and coordinate metal ions (Wittkopp & Schreiner, 2003; Li et al., 2008). In recent years the use of thiourea groups as potential catalytic ligands has been extensively studied in reactions such as hydroformylation (Abdallah et al., 2006), hydrosilylation (Karamé et al., 2003), asymmetric reduction (Nan et al., 2000), cyclization (Breuzard et al., 2000) and hydrogenation (Tommasino et al., 2000). Other applications include their use as synthetic cation-anion ionophores (Reinoso García et al., 2004; Leung et al., 2008).
Here we report the crystal structure of the title compound (Lee et al., 1985) (Fig. 1). The structure shows two distinct intermolecular hydrogen bonding interactions. The first occurs between between N1–H1 and S1 2.508 (18) Å, that creates an infinite chain of molecules along the b axis. The second occurs between N2–H2 and S1 2.713 (16) Å, that generates an infinite chain along the a axis. Due to these interactions an interlocking molecular structure is formed (Fig. 2).
Experimental
A solution of phenyl isothiocyanate (6.75 g, 50 mmol) in diethyl ether (15 ml) was added dropwise at 15°C to a vigorously stirred solution of anhydrous butane-1,4-diamine (8.81 g, 100 mmol) in isopropyl alcohol (100 ml) over a period of 30 min.The reaction mixture was stirred for 2 hrs at room temperature and quenched with water (200 ml). The reaction mixture was maintained overnight at room temperature. Then the reaction mixture was acidified with conc. HCl up to pH 2.6. The solvents were evaporated under vacuum, the residue was suspended in hot water for 30 min and the resulting precipitate was filtered off. The product was washed with ice cold water and dried. The yield was 2.36 g (35%).
Crystals suitable for single-crystal X-ray diffraction were grown in methanol: methylene chloride (1:2) at room temperature. M.p. = 458 K.
1H NMR (CDCl3, 400 MHz) d (p.p.m.): 7.64 (br.s., 2H, NH—CS), 7.40- 7.46 (m, 4H, H-arom), 7.29–7.33 (t, 2H, H-arom), 7.19–7.21 (d, 4H, H-arom), 6.18 (br.s., 2H, –NH—CH2), 3.65 (m, 4H, –CH2–CH2), 1.61 (m, 4H, –CH2–CH2).
13C NMR (CDCl3, 400 MHz): 26.12, 44.75, 125.45, 127.55, 130.34, 180.92
IR. (ν, cm-1) 3155, 3005, 2933, 1591, 1518, 1492, 1294, 1254, 1178,1071.
Refinement
With the exception of those involved in hydrogen bonding, all hydrogen atoms were first located in the difference map then positioned geometrically and allowed to ride on their respective parent atoms with C—H = 0.95Å and Uiso(H) = 1.2Ueq(C) for aromatic and C—H = 0.99Å and Uiso(H) = 1.2Ueq(C) for CH2. Hydrogen atoms involved in hydrogen bonding were located in the difference map and refined freely.
Figures
Fig. 1.
The molecular structure of the title compound with atomic numbering scheme. The H atoms have been omitted for clarity. Displacement ellipsoids are drawn at 40% probability. The 1,1'-(butane-1,4-diyl)bis(3-phenylthiourea) has inversion symmetry [symmetry code: (i): 1 - x, -y, 1-z].
Fig. 2.
The hydrogen bonding interactions of the title compound as viewed down the a axis. All H atoms except those involved in hydrogen bonding interactions have been omitted for clarity.
Crystal data
| C18H22N4S2 | F(000) = 380 |
| Mr = 358.52 | Dx = 1.319 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 3394 reflections |
| a = 9.6795 (3) Å | θ = 3.1–28.2° |
| b = 7.8677 (3) Å | µ = 0.30 mm−1 |
| c = 12.3213 (4) Å | T = 173 K |
| β = 105.816 (2)° | Plate, colourless |
| V = 902.81 (5) Å3 | 0.46 × 0.45 × 0.13 mm |
| Z = 2 |
Data collection
| Bruker APEXII CCD diffractometer | 1710 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.042 |
| graphite | θmax = 28.0°, θmin = 2.2° |
| φ and ω scans | h = −12→12 |
| 9210 measured reflections | k = −10→10 |
| 2192 independent reflections | l = −16→16 |
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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.093 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.0513P)2 + 0.0075P] where P = (Fo2 + 2Fc2)/3 |
| 2192 reflections | (Δ/σ)max = 0.005 |
| 117 parameters | Δρmax = 0.45 e Å−3 |
| 0 restraints | Δρmin = −0.23 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 | ||
| C1 | 0.23226 (14) | −0.10682 (19) | 0.10971 (12) | 0.0250 (3) | |
| C2 | 0.17043 (15) | −0.0394 (2) | 0.19000 (13) | 0.0314 (4) | |
| H2 | 0.2223 | 0.0392 | 0.2445 | 0.038* | |
| C3 | 0.03242 (16) | −0.0880 (2) | 0.18976 (14) | 0.0383 (4) | |
| H3 | −0.0092 | −0.0449 | 0.2457 | 0.046* | |
| C4 | −0.04488 (16) | −0.1990 (2) | 0.10837 (15) | 0.0393 (4) | |
| H4 | −0.1387 | −0.2333 | 0.1092 | 0.047* | |
| C5 | 0.01453 (16) | −0.2598 (2) | 0.02594 (14) | 0.0366 (4) | |
| H5 | −0.0397 | −0.3326 | −0.0315 | 0.044* | |
| C6 | 0.15346 (15) | −0.2145 (2) | 0.02723 (12) | 0.0296 (3) | |
| H6 | 0.1947 | −0.2578 | −0.0289 | 0.036* | |
| C7 | 0.49385 (14) | −0.05136 (17) | 0.19228 (11) | 0.0223 (3) | |
| C8 | 0.60322 (15) | −0.0926 (2) | 0.39648 (12) | 0.0286 (3) | |
| H8A | 0.6645 | 0.0072 | 0.3938 | 0.034* | |
| H8B | 0.6631 | −0.1961 | 0.4027 | 0.034* | |
| C9 | 0.54395 (17) | −0.0793 (2) | 0.49881 (12) | 0.0316 (3) | |
| H9A | 0.4833 | −0.1801 | 0.5004 | 0.038* | |
| H9B | 0.6253 | −0.0821 | 0.5680 | 0.038* | |
| N1 | 0.37258 (12) | −0.05795 (17) | 0.10580 (10) | 0.0265 (3) | |
| N2 | 0.48550 (13) | −0.10013 (17) | 0.29351 (10) | 0.0261 (3) | |
| S1 | 0.65024 (4) | 0.01605 (5) | 0.16882 (3) | 0.02773 (13) | |
| H1N | 0.3820 (18) | −0.045 (2) | 0.0393 (15) | 0.036 (5)* | |
| H2N | 0.4173 (16) | −0.158 (2) | 0.2950 (13) | 0.028 (4)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0203 (7) | 0.0312 (8) | 0.0236 (7) | 0.0032 (6) | 0.0058 (5) | 0.0059 (6) |
| C2 | 0.0244 (7) | 0.0448 (9) | 0.0253 (8) | 0.0052 (6) | 0.0073 (6) | 0.0008 (6) |
| C3 | 0.0274 (8) | 0.0553 (11) | 0.0354 (9) | 0.0102 (7) | 0.0140 (7) | 0.0074 (8) |
| C4 | 0.0216 (7) | 0.0464 (10) | 0.0506 (10) | 0.0014 (7) | 0.0110 (7) | 0.0127 (8) |
| C5 | 0.0254 (8) | 0.0352 (9) | 0.0450 (10) | −0.0020 (6) | 0.0024 (7) | 0.0003 (7) |
| C6 | 0.0260 (7) | 0.0321 (8) | 0.0301 (8) | 0.0030 (6) | 0.0062 (6) | 0.0008 (6) |
| C7 | 0.0219 (7) | 0.0238 (7) | 0.0225 (7) | 0.0013 (5) | 0.0083 (5) | −0.0036 (5) |
| C8 | 0.0223 (7) | 0.0392 (8) | 0.0230 (7) | 0.0017 (6) | 0.0041 (6) | −0.0015 (6) |
| C9 | 0.0311 (8) | 0.0392 (9) | 0.0234 (7) | 0.0028 (7) | 0.0057 (6) | 0.0023 (6) |
| N1 | 0.0221 (6) | 0.0406 (7) | 0.0181 (6) | −0.0017 (5) | 0.0076 (5) | 0.0001 (5) |
| N2 | 0.0204 (6) | 0.0368 (7) | 0.0215 (6) | −0.0068 (5) | 0.0064 (5) | 0.0008 (5) |
| S1 | 0.0215 (2) | 0.0385 (2) | 0.0256 (2) | −0.00221 (15) | 0.01058 (15) | −0.00035 (15) |
Geometric parameters (Å, °)
| C1—C6 | 1.382 (2) | C7—N2 | 1.3283 (17) |
| C1—C2 | 1.393 (2) | C7—N1 | 1.3543 (18) |
| C1—N1 | 1.4250 (17) | C7—S1 | 1.7014 (14) |
| C2—C3 | 1.389 (2) | C8—N2 | 1.4572 (18) |
| C2—H2 | 0.9500 | C8—C9 | 1.5246 (19) |
| C3—C4 | 1.385 (2) | C8—H8A | 0.9900 |
| C3—H3 | 0.9500 | C8—H8B | 0.9900 |
| C4—C5 | 1.382 (2) | C9—C9i | 1.516 (3) |
| C4—H4 | 0.9500 | C9—H9A | 0.9900 |
| C5—C6 | 1.387 (2) | C9—H9B | 0.9900 |
| C5—H5 | 0.9500 | N1—H1N | 0.855 (18) |
| C6—H6 | 0.9500 | N2—H2N | 0.806 (15) |
| C6—C1—C2 | 119.85 (13) | N1—C7—S1 | 119.92 (10) |
| C6—C1—N1 | 118.73 (12) | N2—C8—C9 | 109.98 (11) |
| C2—C1—N1 | 121.28 (13) | N2—C8—H8A | 109.7 |
| C3—C2—C1 | 119.53 (15) | C9—C8—H8A | 109.7 |
| C3—C2—H2 | 120.2 | N2—C8—H8B | 109.7 |
| C1—C2—H2 | 120.2 | C9—C8—H8B | 109.7 |
| C4—C3—C2 | 120.30 (15) | H8A—C8—H8B | 108.2 |
| C4—C3—H3 | 119.9 | C9i—C9—C8 | 114.35 (16) |
| C2—C3—H3 | 119.9 | C9i—C9—H9A | 108.7 |
| C5—C4—C3 | 119.97 (14) | C8—C9—H9A | 108.7 |
| C5—C4—H4 | 120.0 | C9i—C9—H9B | 108.7 |
| C3—C4—H4 | 120.0 | C8—C9—H9B | 108.7 |
| C4—C5—C6 | 119.93 (15) | H9A—C9—H9B | 107.6 |
| C4—C5—H5 | 120.0 | C7—N1—C1 | 127.84 (12) |
| C6—C5—H5 | 120.0 | C7—N1—H1N | 117.0 (12) |
| C1—C6—C5 | 120.33 (14) | C1—N1—H1N | 114.6 (12) |
| C1—C6—H6 | 119.8 | C7—N2—C8 | 124.94 (12) |
| C5—C6—H6 | 119.8 | C7—N2—H2N | 116.4 (11) |
| N2—C7—N1 | 117.79 (12) | C8—N2—H2N | 117.0 (11) |
| N2—C7—S1 | 122.29 (11) | ||
| C6—C1—C2—C3 | 3.2 (2) | N2—C8—C9—C9i | −62.1 (2) |
| N1—C1—C2—C3 | 178.86 (14) | N2—C7—N1—C1 | 2.1 (2) |
| C1—C2—C3—C4 | −1.8 (2) | S1—C7—N1—C1 | −178.44 (12) |
| C2—C3—C4—C5 | −1.0 (3) | C6—C1—N1—C7 | −135.44 (15) |
| C3—C4—C5—C6 | 2.3 (3) | C2—C1—N1—C7 | 48.9 (2) |
| C2—C1—C6—C5 | −1.9 (2) | N1—C7—N2—C8 | −176.58 (13) |
| N1—C1—C6—C5 | −177.63 (14) | S1—C7—N2—C8 | 4.0 (2) |
| C4—C5—C6—C1 | −0.9 (2) | C9—C8—N2—C7 | 154.26 (15) |
Symmetry codes: (i) −x+1, −y, −z+1.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···S1ii | 0.855 (18) | 2.508 (18) | 3.3465 (13) | 167.1 (15) |
| N2—H2N···S1iii | 0.806 (15) | 2.713 (16) | 3.3755 (14) | 140.7 (13) |
Symmetry codes: (ii) −x+1, −y, −z; (iii) −x+1, y−1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: OM2458).
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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 datablock(s) I, global. DOI: 10.1107/S1600536811033071/om2458sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033071/om2458Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811033071/om2458Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


