Abstract
In the title compound, [Hg(CN)2(C9H20N2S)2], the Hg atom lies on a twofold rotation axis. There is only half a molecule in the asymmetric unit. The Hg atom has a distorted tetrahedral coordination involving the S atoms of two 1-butyl-3-propylthiourea groups and the C atoms of the two CN− anions. In the crystal packing, adjacent molecules are connected by intermolecular N—H⋯N and N—H⋯S hydrogen bonds, forming infinite chains in three dimensions.
Related literature
For the coordination chemistry of thiourea-type ligands, see: Nadeem et al. (2009 ▶, 2008 ▶); Zoufalá et al. (2007 ▶); Khan et al. (2007 ▶); Hanif et al. (2007 ▶); Fuks et al. (2005 ▶); Moro et al. (2009 ▶); Matesanz & Souza (2007 ▶). For crystallographic reports about mercury(II) complexes containing thioamides, see: Popovic et al. (2000 ▶, 2002 ▶); Pavlović et al. (2000 ▶); Jiang et al. (2001 ▶); Wu et al. (2004 ▶). For the spectroscopy and structural chemistry of cyanide complexes of silver(I) and gold(I) with thiones, see: Hanif et al. (2007 ▶); Wu et al. (2004 ▶); Ahmad, Isab & Ashraf (2002 ▶); Ahmad, Isab & Perzanowski (2002 ▶); Ashraf et al. (2002 ▶); Ahmad & Isab (2001 ▶); Ahmad (2004 ▶).
Experimental
Crystal data
[Hg(CN)2(C9H20N2S)2]
M r = 629.31
Monoclinic,
a = 17.4692 (3) Å
b = 9.5928 (2) Å
c = 17.4699 (4) Å
β = 111.540 (1)°
V = 2723.12 (10) Å3
Z = 4
Mo Kα radiation
μ = 5.82 mm−1
T = 296 K
0.14 × 0.15 × 0.17 mm
Data collection
Bruker Kappa APEXII CCD area-detector diffractometer
Absorption correction: none
15120 measured reflections
3372 independent reflections
2918 reflections with I > 2σ(I)
R int = 0.032
Refinement
R[F 2 > 2σ(F 2)] = 0.022
wR(F 2) = 0.044
S = 1.02
3372 reflections
134 parameters
H-atom parameters constrained
Δρmax = 0.40 e Å−3
Δρmin = −0.72 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; 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 ▶) and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809035594/bt5052sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809035594/bt5052Isup2.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 | 2.68 | 3.479 (2) | 155 |
| N3—H3⋯N1ii | 0.86 | 2.20 | 2.991 (3) | 153 |
| C7—H7B⋯S1 | 0.97 | 2.67 | 3.070 (3) | 105 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
The coordination chemistry of thiourea type ligands has been the subject of several recent studies because of the relevance of their binding sites to those in living systems (Nadeem et al., 2009; Nadeem et al., 2008; Zoufalá et al., 2007; Khan et al., 2007; Hanif et al., 2007; Fuks et al., 2005; Moro et al., 2009; Matesanz & Souza, 2007). Crystallographic reports about mercury (II) complexes containing thioamides establish that these ligands are coordinated via the sulfur atom(Popovic et al., 2000, 2002; Pavlović, Popović, Soldin et al., 2000; Jiang et al., 2001; Wu et al., 2004). We have been involved in investigating the spectral and structural chemistry of cyanido complexes of silver (I) and gold (I) with thiones with emphasis onligand scrambling reactions (Hanif et al., 2007; Wu et al., 2004; Ahmad, Isab & Ashraf, 2002; Ahmad, Isab & Perzanowski, 2002; Ashraf et al., 2002; Ahmad & Isab, 2001; Ahmad, 2004). As a part ofextension of our work towards complexation of Hg (CN)2 with thiones, we report here the crystal structures of [(N,N/-dibutylthiourea)2Hg(CN)2], (I).
In the title compound (I), (Fig. 1), the Hg anion lies on a twofold rotation axes paralel to the b axis in space group C2/c and one half of the molecule to the other half are connected by this symmetry operation. The Hg atom has a distorted tetrahedral coordination by the S atoms of two N,N/-dibutylthiourea groups and the C atoms of the two CN groups. The bond distances Hg—S and Hg—C are 2.7424 (7) Å and 2.072 (3) Å, and the bond angles C—Hg—C, S—Hg—S and C—Hg—C are 150.51 (11)°, 95.55 (2)° and 100.45 (8)°. All bond lengths and bond angles in (I) are in the range of expected values.
In the crystal packing, the adjacent molecules are connected by intermolecular N—H···N and N—H···S hydrogen bonds (Table 1). In Fig. 2, the packing and hydrogen bonding of (I) are shown viewed down b axis.
Experimental
For the preparation of the title complex, Hg (CN)2 was prepared first by the reaction of 1 mmol HgCl2 in methanol with 2 mmole of KCN in water. Then 0.253 g (1 mmole) Hg (CN)2 dissolved in15 ml methanol was mixed with 2 equivalents of N,N/-dibutylthiourea in 15 methanol. After stirring for 15 minutes, the resulting mixture was filtered and filtrate was kept at room temperature. After 24 h white crystals were obtained.
Refinement
H atoms were located geometrically and treated as riding with C—H = 0.97 Å (methylene), C—H = 0.96 Å (methyl) and N—H = 0.86 Å with Uiso(H) = 1.2 or 1.5Ueq(C, N).
Figures
Fig. 1.
The title molecule with the atom numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 30% probability level.
Fig. 2.
The packing and hydrogen bonding of (I) viewed down b axis. Hydrogen atoms not involved in the showed interactions have been omitted for clarity.
Crystal data
| [Hg(CN)2(C9H20N2S)2] | F(000) = 1256 |
| Mr = 629.31 | Dx = 1.535 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 6609 reflections |
| a = 17.4692 (3) Å | θ = 2.5–27.2° |
| b = 9.5928 (2) Å | µ = 5.82 mm−1 |
| c = 17.4699 (4) Å | T = 296 K |
| β = 111.540 (1)° | Irregular, white |
| V = 2723.12 (10) Å3 | 0.17 × 0.15 × 0.14 mm |
| Z = 4 |
Data collection
| Bruker Kappa APEXII CCD area-detector diffractometer | 2918 reflections with I > 2σ(I) |
| Radiation source: sealed tube | Rint = 0.032 |
| graphite | θmax = 28.3°, θmin = 2.5° |
| φ and ω scans | h = −23→23 |
| 15120 measured reflections | k = −12→12 |
| 3372 independent reflections | l = −20→23 |
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)] = 0.022 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.044 | H-atom parameters constrained |
| S = 1.02 | w = 1/[σ2(Fo2) + (0.0211P)2], where P = (Fo2 + 2Fc2)/3 |
| 3372 reflections | (Δ/σ)max = 0.001 |
| 134 parameters | Δρmax = 0.40 e Å−3 |
| 0 restraints | Δρmin = −0.72 e Å−3 |
Special details
| Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
| Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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 | ||
| Hg1 | 1.00000 | 0.20478 (1) | 0.75000 | 0.0405 (1) | |
| S1 | 1.08516 (3) | 0.39691 (7) | 0.86634 (4) | 0.0414 (2) | |
| N1 | 0.86048 (15) | 0.1224 (3) | 0.81955 (17) | 0.0718 (10) | |
| N2 | 1.11488 (12) | 0.5094 (2) | 0.74219 (12) | 0.0422 (7) | |
| N3 | 1.22801 (11) | 0.4758 (2) | 0.85840 (12) | 0.0411 (7) | |
| C1 | 0.91098 (16) | 0.1498 (3) | 0.79668 (17) | 0.0475 (9) | |
| C2 | 1.14750 (13) | 0.4655 (2) | 0.81878 (15) | 0.0341 (7) | |
| C3 | 1.16093 (17) | 0.5591 (3) | 0.69240 (17) | 0.0548 (10) | |
| C4 | 1.10347 (17) | 0.6051 (3) | 0.60900 (17) | 0.0534 (10) | |
| C5 | 1.0548 (2) | 0.7334 (4) | 0.6094 (2) | 0.0633 (12) | |
| C6 | 0.9979 (3) | 0.7767 (4) | 0.5243 (3) | 0.0875 (17) | |
| C7 | 1.27223 (15) | 0.4387 (3) | 0.94375 (16) | 0.0441 (8) | |
| C8 | 1.27906 (17) | 0.5571 (3) | 1.00242 (16) | 0.0473 (9) | |
| C9 | 1.3311 (2) | 0.5232 (3) | 1.09034 (17) | 0.0586 (11) | |
| C10 | 1.3434 (3) | 0.6466 (4) | 1.1477 (2) | 0.0795 (14) | |
| H2 | 1.06210 | 0.50880 | 0.71950 | 0.0510* | |
| H3 | 1.25650 | 0.50710 | 0.83120 | 0.0490* | |
| H3A | 1.19600 | 0.48500 | 0.68630 | 0.0660* | |
| H3B | 1.19580 | 0.63660 | 0.72020 | 0.0660* | |
| H4A | 1.13530 | 0.62230 | 0.57470 | 0.0640* | |
| H4B | 1.06550 | 0.52970 | 0.58410 | 0.0640* | |
| H5A | 1.09240 | 0.80930 | 0.63420 | 0.0760* | |
| H5B | 1.02240 | 0.71650 | 0.64330 | 0.0760* | |
| H6A | 1.02880 | 0.78550 | 0.48910 | 0.1310* | |
| H6B | 0.97300 | 0.86460 | 0.52750 | 0.1310* | |
| H6C | 0.95580 | 0.70750 | 0.50240 | 0.1310* | |
| H7A | 1.32710 | 0.40780 | 0.95010 | 0.0530* | |
| H7B | 1.24430 | 0.36120 | 0.95810 | 0.0530* | |
| H8A | 1.22430 | 0.58250 | 0.99950 | 0.0570* | |
| H8B | 1.30250 | 0.63730 | 0.98510 | 0.0570* | |
| H9A | 1.38450 | 0.49040 | 1.09270 | 0.0700* | |
| H9B | 1.30520 | 0.44820 | 1.10920 | 0.0700* | |
| H10A | 1.36760 | 0.72220 | 1.12850 | 0.1190* | |
| H10B | 1.37910 | 0.62040 | 1.20210 | 0.1190* | |
| H10C | 1.29110 | 0.67540 | 1.14870 | 0.1190* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Hg1 | 0.0323 (1) | 0.0459 (1) | 0.0478 (1) | 0.0000 | 0.0199 (1) | 0.0000 |
| S1 | 0.0359 (3) | 0.0566 (4) | 0.0340 (3) | −0.0115 (3) | 0.0154 (3) | −0.0005 (3) |
| N1 | 0.0516 (14) | 0.104 (2) | 0.0668 (17) | −0.0297 (15) | 0.0300 (13) | −0.0046 (17) |
| N2 | 0.0326 (10) | 0.0594 (14) | 0.0352 (12) | −0.0068 (9) | 0.0133 (9) | 0.0057 (11) |
| N3 | 0.0313 (10) | 0.0545 (13) | 0.0383 (12) | −0.0043 (9) | 0.0136 (9) | 0.0051 (10) |
| C1 | 0.0385 (13) | 0.0553 (16) | 0.0463 (16) | −0.0125 (12) | 0.0126 (12) | −0.0037 (14) |
| C2 | 0.0330 (11) | 0.0369 (13) | 0.0340 (14) | −0.0030 (9) | 0.0142 (10) | −0.0015 (11) |
| C3 | 0.0473 (15) | 0.076 (2) | 0.0491 (17) | −0.0018 (14) | 0.0270 (14) | 0.0144 (15) |
| C4 | 0.0563 (16) | 0.069 (2) | 0.0396 (16) | −0.0019 (14) | 0.0232 (13) | 0.0039 (15) |
| C5 | 0.076 (2) | 0.066 (2) | 0.052 (2) | 0.0065 (17) | 0.0285 (17) | 0.0103 (16) |
| C6 | 0.084 (3) | 0.101 (3) | 0.074 (3) | 0.026 (2) | 0.025 (2) | 0.020 (2) |
| C7 | 0.0353 (12) | 0.0476 (15) | 0.0446 (16) | 0.0040 (11) | 0.0089 (11) | 0.0054 (13) |
| C8 | 0.0477 (14) | 0.0466 (15) | 0.0427 (16) | 0.0038 (12) | 0.0110 (12) | 0.0064 (13) |
| C9 | 0.0665 (19) | 0.0565 (19) | 0.0433 (17) | 0.0044 (15) | 0.0090 (15) | 0.0050 (15) |
| C10 | 0.107 (3) | 0.066 (2) | 0.051 (2) | −0.005 (2) | 0.012 (2) | −0.0008 (19) |
Geometric parameters (Å, °)
| Hg1—S1 | 2.7424 (7) | C3—H3A | 0.9700 |
| Hg1—C1 | 2.072 (3) | C3—H3B | 0.9700 |
| Hg1—S1i | 2.7424 (7) | C4—H4A | 0.9700 |
| Hg1—C1i | 2.072 (3) | C4—H4B | 0.9700 |
| S1—C2 | 1.724 (2) | C5—H5A | 0.9700 |
| N1—C1 | 1.125 (4) | C5—H5B | 0.9700 |
| N2—C2 | 1.316 (3) | C6—H6A | 0.9600 |
| N2—C3 | 1.465 (4) | C6—H6B | 0.9600 |
| N3—C2 | 1.324 (3) | C6—H6C | 0.9600 |
| N3—C7 | 1.449 (3) | C7—H7A | 0.9700 |
| N2—H2 | 0.8600 | C7—H7B | 0.9700 |
| N3—H3 | 0.8600 | C8—H8A | 0.9700 |
| C3—C4 | 1.500 (4) | C8—H8B | 0.9700 |
| C4—C5 | 1.497 (5) | C9—H9A | 0.9700 |
| C5—C6 | 1.512 (6) | C9—H9B | 0.9700 |
| C7—C8 | 1.505 (4) | C10—H10A | 0.9600 |
| C8—C9 | 1.505 (4) | C10—H10B | 0.9600 |
| C9—C10 | 1.514 (5) | C10—H10C | 0.9600 |
| S1···C1 | 3.693 (3) | H3A···N3 | 2.8500 |
| S1···C8 | 3.684 (3) | H3A···H3 | 2.3700 |
| S1···N2i | 3.479 (2) | H3A···H10Cvi | 2.5200 |
| S1···H7B | 2.6700 | H3B···N3 | 2.7400 |
| S1···H2i | 2.6800 | H3B···H3 | 2.2200 |
| S1···H6Aii | 3.1900 | H3B···H5A | 2.5000 |
| N1···N3iii | 2.991 (3) | H3B···N1iv | 2.7600 |
| N1···C3iii | 3.431 (4) | H4A···H6A | 2.4700 |
| N2···S1i | 3.479 (2) | H4B···H2 | 2.4000 |
| N3···N1iv | 2.991 (3) | H4B···H6C | 2.5700 |
| N1···H3Biii | 2.7600 | H5A···H3B | 2.5000 |
| N1···H3iii | 2.2000 | H5A···H7Avii | 2.5600 |
| N2···H5B | 2.7400 | H5B···N2 | 2.7400 |
| N3···H3A | 2.8500 | H5B···H2 | 2.3500 |
| N3···H3B | 2.7400 | H6A···H4A | 2.4700 |
| C1···S1 | 3.693 (3) | H6A···S1vi | 3.1900 |
| C1···C2i | 3.574 (4) | H6C···H4B | 2.5700 |
| C3···N1iv | 3.431 (4) | H7A···H9A | 2.4500 |
| C8···S1 | 3.684 (3) | H7A···H5Aviii | 2.5600 |
| C1···H10Bv | 3.0100 | H7B···S1 | 2.6700 |
| C3···H3 | 2.4400 | H7B···H9B | 2.6000 |
| C5···H2 | 2.8600 | H7B···H7Bix | 2.5500 |
| H2···C5 | 2.8600 | H8A···H10C | 2.5900 |
| H2···H4B | 2.4000 | H8B···H10A | 2.4800 |
| H2···H5B | 2.3500 | H9A···H7A | 2.4500 |
| H2···S1i | 2.6800 | H9B···H7B | 2.6000 |
| H3···C3 | 2.4400 | H10A···H8B | 2.4800 |
| H3···H3A | 2.3700 | H10B···C1x | 3.0100 |
| H3···H3B | 2.2200 | H10C···H8A | 2.5900 |
| H3···N1iv | 2.2000 | H10C···H3Aii | 2.5200 |
| S1—Hg1—C1 | 99.25 (8) | C4—C5—H5A | 109.00 |
| S1—Hg1—S1i | 95.55 (2) | C4—C5—H5B | 109.00 |
| S1—Hg1—C1i | 100.45 (8) | C6—C5—H5A | 109.00 |
| S1i—Hg1—C1 | 100.45 (8) | C6—C5—H5B | 109.00 |
| C1—Hg1—C1i | 150.51 (11) | H5A—C5—H5B | 108.00 |
| S1i—Hg1—C1i | 99.25 (8) | C5—C6—H6A | 109.00 |
| Hg1—S1—C2 | 99.56 (8) | C5—C6—H6B | 109.00 |
| C2—N2—C3 | 125.5 (2) | C5—C6—H6C | 109.00 |
| C2—N3—C7 | 125.6 (2) | H6A—C6—H6B | 109.00 |
| C2—N2—H2 | 117.00 | H6A—C6—H6C | 110.00 |
| C3—N2—H2 | 117.00 | H6B—C6—H6C | 109.00 |
| C2—N3—H3 | 117.00 | N3—C7—H7A | 109.00 |
| C7—N3—H3 | 117.00 | N3—C7—H7B | 109.00 |
| Hg1—C1—N1 | 177.4 (3) | C8—C7—H7A | 109.00 |
| S1—C2—N2 | 119.84 (19) | C8—C7—H7B | 109.00 |
| S1—C2—N3 | 120.95 (18) | H7A—C7—H7B | 108.00 |
| N2—C2—N3 | 119.2 (2) | C7—C8—H8A | 109.00 |
| N2—C3—C4 | 110.8 (2) | C7—C8—H8B | 109.00 |
| C3—C4—C5 | 114.6 (2) | C9—C8—H8A | 109.00 |
| C4—C5—C6 | 113.0 (3) | C9—C8—H8B | 109.00 |
| N3—C7—C8 | 113.2 (2) | H8A—C8—H8B | 108.00 |
| C7—C8—C9 | 113.5 (2) | C8—C9—H9A | 109.00 |
| C8—C9—C10 | 113.1 (3) | C8—C9—H9B | 109.00 |
| N2—C3—H3A | 109.00 | C10—C9—H9A | 109.00 |
| N2—C3—H3B | 109.00 | C10—C9—H9B | 109.00 |
| C4—C3—H3A | 109.00 | H9A—C9—H9B | 108.00 |
| C4—C3—H3B | 109.00 | C9—C10—H10A | 109.00 |
| H3A—C3—H3B | 108.00 | C9—C10—H10B | 109.00 |
| C3—C4—H4A | 109.00 | C9—C10—H10C | 109.00 |
| C3—C4—H4B | 109.00 | H10A—C10—H10B | 110.00 |
| C5—C4—H4A | 109.00 | H10A—C10—H10C | 109.00 |
| C5—C4—H4B | 109.00 | H10B—C10—H10C | 110.00 |
| H4A—C4—H4B | 108.00 | ||
| C1—Hg1—S1—C2 | −169.87 (11) | C7—N3—C2—S1 | −2.8 (3) |
| S1i—Hg1—S1—C2 | −68.30 (8) | C7—N3—C2—N2 | 176.7 (2) |
| C1i—Hg1—S1—C2 | 32.19 (11) | C2—N3—C7—C8 | −88.9 (3) |
| Hg1—S1—C2—N2 | 51.24 (18) | N2—C3—C4—C5 | 67.9 (3) |
| Hg1—S1—C2—N3 | −129.28 (17) | C3—C4—C5—C6 | 179.8 (3) |
| C3—N2—C2—S1 | −174.74 (19) | N3—C7—C8—C9 | −175.0 (2) |
| C3—N2—C2—N3 | 5.8 (3) | C7—C8—C9—C10 | 175.2 (3) |
| C2—N2—C3—C4 | −178.1 (2) |
Symmetry codes: (i) −x+2, y, −z+3/2; (ii) x, −y+1, z+1/2; (iii) x−1/2, y−1/2, z; (iv) x+1/2, y+1/2, z; (v) x−1/2, −y+1/2, z−1/2; (vi) x, −y+1, z−1/2; (vii) −x+5/2, y+1/2, −z+3/2; (viii) −x+5/2, y−1/2, −z+3/2; (ix) −x+5/2, −y+1/2, −z+2; (x) x+1/2, −y+1/2, z+1/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2···S1i | 0.86 | 2.68 | 3.479 (2) | 155 |
| N3—H3···N1iv | 0.86 | 2.20 | 2.991 (3) | 153 |
| C7—H7B···S1 | 0.97 | 2.67 | 3.070 (3) | 105 |
Symmetry codes: (i) −x+2, y, −z+3/2; (iv) x+1/2, y+1/2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5052).
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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/S1600536809035594/bt5052sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809035594/bt5052Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


