Abstract
The SnIV atom in the title diorganotin dithiocarbamate, [Sn(C4H9)2Cl(C10H12NS2)], is pentacoordinated by an asymmetrically coordinating dithiocarbamate ligand, a Cl and two C atoms of the Sn-bound tert-butyl groups. The resulting C2ClS2 donor set defines a coordination geometry intermediate between square pyramidal and trigonal bipyramidal with a slight tendency towards the former. In the crystal structure, C—H⋯π contacts link centrosymmetrically related molecules into dimeric aggregates.
Related literature
For a review on the applications and structural chemistry of tin dithiocarbamates, see: Tiekink (2008 ▶). For additional structural analysis, see: Addison et al. (1984 ▶); Spek (2009 ▶). For a recently reported related structure, see: Abdul Muthalib et al. (2010 ▶).
Experimental
Crystal data
[Sn(C4H9)2Cl(C10H12NS2)]
M r = 478.69
Triclinic,
a = 8.6140 (2) Å
b = 10.9604 (3) Å
c = 11.4765 (3) Å
α = 91.858 (2)°
β = 96.193 (2)°
γ = 96.011 (2)°
V = 1070.24 (5) Å3
Z = 2
Mo Kα radiation
μ = 1.51 mm−1
T = 150 K
0.30 × 0.23 × 0.16 mm
Data collection
Oxford Diffraction Xcaliber Eos Gemini diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010 ▶) T min = 0.935, T max = 1.000
26998 measured reflections
4865 independent reflections
4707 reflections with I > 2σ(I)
R int = 0.034
Refinement
R[F 2 > 2σ(F 2)] = 0.018
wR(F 2) = 0.046
S = 1.11
4865 reflections
215 parameters
H-atom parameters constrained
Δρmax = 0.29 e Å−3
Δρmin = −0.50 e Å−3
Data collection: CrysAlis PRO (Oxford Diffraction, 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/S1600536811006398/zs2099sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006398/zs2099Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Sn—Cl1 | 2.4847 (4) |
| Sn—S1 | 2.4760 (4) |
| Sn—S2 | 2.7409 (4) |
| Sn—C11 | 2.1884 (14) |
| Sn—C15 | 2.1879 (15) |
Table 2. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the C5–C10 ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C3—H3a⋯Cg1 | 0.98 | 2.78 | 3.6491 (18) | 149 |
| C13—H13b⋯Cg1i | 0.98 | 2.96 | 3.5401 (18) | 119 |
Symmetry code: (i)
.
Acknowledgments
The authors thank Universiti Kebangsaan Malaysia (UKM-GUP-NBT-08–27-111), the Ministry of Higher Education (UKM-ST-06-FRGS0092–2010), Universiti Putra Malaysia and the University of Malaya for supporting this study.
supplementary crystallographic information
Comment
Organotin dithiocarbamates attract attention as they exhibit properties suggesting their potential as anti-cancer agents, anti-microbials and insecticides (Tiekink, 2008). Motivated by these and in continuation of structural studies of these systems (Abdul Muthalib et al., 2010), the analysis of the title compound, (I), was undertaken.
The SnIV atom in (I) is five-coordinated, being chelated by an asymmetrically coordinating dithiocarbamate ligand, a Cl and two C atoms of the Sn-bound tert-butyl groups (Fig. 1 and Table 1). The asymmetric chelating mode of the non-symmetric dithiocarbamate ligand is reflected in the non-equivalence of the associated C≐S bond distances (Table 1). The coordination geometry is intermediate between square pyramidal and trigonal bi-pyramidal with a leaning towards the former. This assignment is based on the value calculated for τ of 0.45 for the Sn atom, which compares to the τ values of 0.0 and 1.0 for ideal square pyramidal and trigonal bi-pyramidal geometries, respectively (Spek, 2009; Addison et al., 1984). The mode of coordination of the dithiocarbamate ligand, the disposition of the ligand donor set, and the intermediate coordination geometry observed for (I) matches with the literature precedents (Tiekink, 2008).
The most prominent feature of the crystal packing is the presence of C–H···π interactions (Table 2). As shown in Fig. 2, these lead to dimeric aggregates. It is also noted that intramolecular C–H···π contacts are present so that the benzene ring participates in two such interactions (Table 2, Fig. 2). The dimeric aggregates stack into columns along the a axis (Fig. 3).
Experimental
The dithiocarbamate ligand was prepared by the addition of carbon disulfide (0.01 mol) to an ethanolic solution (20 ml) of ethylbenzylamine (0.01 mol). The mixture was stirred for 1 h at 277 K, after which the solution was added drop wise to a solution of di-tert-butyltin(IV) dichloride (0.005 mol) in ethanol (20 ml). The resulting mixture was stirred for 1 h. The white precipitate was filtered, washed with cold ethanol and dried in a desiccator. Crystallization was carried out by using an ethanol:chloroform (1:2) mixture. Yield 76%; m.p. 451–453 K. Elemental analysis. Found (calculated) for C18H30ClNS2Sn: C, 44.81 (45.16); H 6.27 (6.32), N 2.72 (2.93), S 13.23 (13.40); Sn 23.98 (24.80) %. UV (CHCl3) λmax 244 (L(π) →L(π*)). IR (KBr): ν(C—H) 2933m, 2958m; ν(C≐N) 1496m; ν(N—C) 1185 s; ν(C≐S) 950 s; ν(Sn—S) 351 s cm-1.
Refinement
Carbon-bound H-atoms were placed in calculated positions (C—H = 0.95 to 0.99 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2 to 1.5Ueq(C).
Figures
Fig. 1.
The molecular structure of of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.
Fig. 2.
A view of the dimeric aggregate in (I) showing the intra- and intermolecular C–H···π contacts as purple dashed lines.
Fig. 3.
A view in projection down the a axis of (I) showing columns of dimeric aggregates along a. The intermolecular C–H···π contacts are shown as purple dashed lines.
Crystal data
| [Sn(C4H9)2Cl(C10H12NS2)] | Z = 2 |
| Mr = 478.69 | F(000) = 488 |
| Triclinic, P1 | Dx = 1.485 Mg m−3 |
| Hall symbol: -P 1 | Melting point = 451–453 K |
| a = 8.6140 (2) Å | Mo Kα radiation, λ = 0.71073 Å |
| b = 10.9604 (3) Å | Cell parameters from 22888 reflections |
| c = 11.4765 (3) Å | θ = 2.4–28.8° |
| α = 91.858 (2)° | µ = 1.51 mm−1 |
| β = 96.193 (2)° | T = 150 K |
| γ = 96.011 (2)° | Block, colourless |
| V = 1070.24 (5) Å3 | 0.30 × 0.23 × 0.16 mm |
Data collection
| Oxford Diffraction Xcaliber Eos Gemini diffractometer | 4865 independent reflections |
| Radiation source: fine-focus sealed tube | 4707 reflections with I > 2σ(I) |
| graphite | Rint = 0.034 |
| Detector resolution: 16.1952 pixels mm-1 | θmax = 27.5°, θmin = 2.4° |
| ω scans | h = −11→11 |
| Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) | k = −13→13 |
| Tmin = 0.935, Tmax = 1.000 | l = −14→14 |
| 26998 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)] = 0.018 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.046 | H-atom parameters constrained |
| S = 1.11 | w = 1/[σ2(Fo2) + (0.0236P)2 + 0.279P] where P = (Fo2 + 2Fc2)/3 |
| 4865 reflections | (Δ/σ)max = 0.003 |
| 215 parameters | Δρmax = 0.29 e Å−3 |
| 0 restraints | Δρmin = −0.50 e Å−3 |
Special details
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
| Sn | 0.908142 (10) | 0.227855 (8) | 0.757926 (8) | 0.01355 (4) | |
| Cl1 | 1.09329 (4) | 0.40294 (3) | 0.84821 (3) | 0.02158 (8) | |
| S1 | 0.88193 (4) | 0.35904 (3) | 0.58681 (3) | 0.01801 (8) | |
| S2 | 0.70139 (5) | 0.11432 (3) | 0.57914 (3) | 0.02180 (8) | |
| N1 | 0.69363 (14) | 0.26534 (11) | 0.39968 (10) | 0.0152 (2) | |
| C1 | 0.74996 (17) | 0.24573 (13) | 0.50861 (12) | 0.0154 (3) | |
| C2 | 0.73841 (18) | 0.38150 (14) | 0.34275 (13) | 0.0192 (3) | |
| H2A | 0.7233 | 0.3660 | 0.2566 | 0.023* | |
| H2B | 0.8514 | 0.4073 | 0.3659 | 0.023* | |
| C3 | 0.6448 (2) | 0.48595 (15) | 0.37411 (15) | 0.0248 (3) | |
| H3A | 0.5338 | 0.4643 | 0.3450 | 0.037* | |
| H3B | 0.6849 | 0.5609 | 0.3380 | 0.037* | |
| H3C | 0.6555 | 0.4998 | 0.4595 | 0.037* | |
| C4 | 0.58006 (18) | 0.17438 (14) | 0.32856 (13) | 0.0185 (3) | |
| H4A | 0.5613 | 0.0996 | 0.3734 | 0.022* | |
| H4B | 0.6243 | 0.1508 | 0.2560 | 0.022* | |
| C5 | 0.42662 (17) | 0.22668 (13) | 0.29687 (13) | 0.0162 (3) | |
| C6 | 0.38063 (18) | 0.25643 (15) | 0.18239 (13) | 0.0206 (3) | |
| H6 | 0.4422 | 0.2374 | 0.1217 | 0.025* | |
| C7 | 0.24535 (19) | 0.31377 (15) | 0.15584 (14) | 0.0248 (3) | |
| H7 | 0.2146 | 0.3341 | 0.0775 | 0.030* | |
| C8 | 0.15570 (19) | 0.34106 (14) | 0.24459 (15) | 0.0244 (3) | |
| H8 | 0.0644 | 0.3818 | 0.2273 | 0.029* | |
| C9 | 0.19895 (18) | 0.30901 (15) | 0.35845 (15) | 0.0230 (3) | |
| H9 | 0.1362 | 0.3265 | 0.4188 | 0.028* | |
| C10 | 0.33337 (17) | 0.25166 (14) | 0.38442 (13) | 0.0185 (3) | |
| H10 | 0.3621 | 0.2293 | 0.4624 | 0.022* | |
| C11 | 1.08251 (17) | 0.09669 (13) | 0.75357 (13) | 0.0182 (3) | |
| C12 | 1.1743 (2) | 0.09891 (18) | 0.87481 (16) | 0.0344 (4) | |
| H12A | 1.2538 | 0.0413 | 0.8745 | 0.052* | |
| H12B | 1.1022 | 0.0749 | 0.9326 | 0.052* | |
| H12C | 1.2258 | 0.1820 | 0.8954 | 0.052* | |
| C13 | 1.0023 (2) | −0.03233 (15) | 0.7207 (2) | 0.0351 (4) | |
| H13A | 0.9457 | −0.0337 | 0.6418 | 0.053* | |
| H13B | 0.9280 | −0.0558 | 0.7771 | 0.053* | |
| H13C | 1.0816 | −0.0903 | 0.7221 | 0.053* | |
| C14 | 1.1918 (2) | 0.13760 (17) | 0.66298 (17) | 0.0334 (4) | |
| H14A | 1.2413 | 0.2211 | 0.6843 | 0.050* | |
| H14B | 1.1312 | 0.1364 | 0.5855 | 0.050* | |
| H14C | 1.2731 | 0.0816 | 0.6609 | 0.050* | |
| C15 | 0.72963 (18) | 0.22899 (15) | 0.87978 (13) | 0.0210 (3) | |
| C16 | 0.6414 (2) | 0.10044 (16) | 0.87739 (15) | 0.0283 (4) | |
| H16A | 0.5648 | 0.0983 | 0.9347 | 0.042* | |
| H16B | 0.7162 | 0.0408 | 0.8971 | 0.042* | |
| H16C | 0.5866 | 0.0797 | 0.7988 | 0.042* | |
| C17 | 0.8116 (2) | 0.2629 (2) | 1.00325 (15) | 0.0356 (4) | |
| H17A | 0.8685 | 0.3453 | 1.0046 | 0.053* | |
| H17B | 0.8857 | 0.2034 | 1.0253 | 0.053* | |
| H17C | 0.7330 | 0.2618 | 1.0590 | 0.053* | |
| C18 | 0.6177 (2) | 0.32236 (19) | 0.8403 (2) | 0.0390 (5) | |
| H18A | 0.5717 | 0.3013 | 0.7594 | 0.059* | |
| H18B | 0.6756 | 0.4045 | 0.8444 | 0.059* | |
| H18C | 0.5339 | 0.3212 | 0.8918 | 0.059* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Sn | 0.01353 (6) | 0.01384 (6) | 0.01283 (6) | 0.00071 (4) | −0.00031 (4) | 0.00204 (4) |
| Cl1 | 0.02389 (18) | 0.01842 (18) | 0.01980 (17) | −0.00371 (14) | −0.00377 (14) | 0.00095 (13) |
| S1 | 0.02071 (18) | 0.01593 (17) | 0.01529 (16) | −0.00302 (13) | −0.00340 (13) | 0.00330 (13) |
| S2 | 0.0271 (2) | 0.01675 (18) | 0.01827 (17) | −0.00533 (15) | −0.00567 (15) | 0.00382 (14) |
| N1 | 0.0147 (6) | 0.0160 (6) | 0.0144 (6) | 0.0026 (5) | −0.0006 (5) | 0.0002 (5) |
| C1 | 0.0146 (6) | 0.0164 (7) | 0.0150 (6) | 0.0026 (5) | 0.0005 (5) | −0.0010 (5) |
| C2 | 0.0198 (7) | 0.0232 (8) | 0.0148 (7) | 0.0010 (6) | 0.0023 (6) | 0.0058 (6) |
| C3 | 0.0268 (8) | 0.0179 (8) | 0.0292 (8) | 0.0013 (6) | 0.0012 (7) | 0.0057 (6) |
| C4 | 0.0196 (7) | 0.0188 (7) | 0.0160 (7) | 0.0042 (6) | −0.0031 (6) | −0.0051 (5) |
| C5 | 0.0170 (7) | 0.0143 (7) | 0.0160 (7) | −0.0001 (5) | −0.0019 (5) | −0.0014 (5) |
| C6 | 0.0218 (7) | 0.0247 (8) | 0.0152 (7) | 0.0028 (6) | 0.0007 (6) | −0.0009 (6) |
| C7 | 0.0262 (8) | 0.0254 (8) | 0.0210 (8) | 0.0038 (6) | −0.0069 (6) | 0.0033 (6) |
| C8 | 0.0190 (7) | 0.0183 (8) | 0.0351 (9) | 0.0048 (6) | −0.0032 (7) | −0.0005 (7) |
| C9 | 0.0199 (7) | 0.0220 (8) | 0.0267 (8) | −0.0005 (6) | 0.0054 (6) | −0.0057 (6) |
| C10 | 0.0198 (7) | 0.0197 (7) | 0.0151 (7) | −0.0009 (6) | 0.0008 (6) | −0.0003 (5) |
| C11 | 0.0173 (7) | 0.0152 (7) | 0.0225 (7) | 0.0034 (5) | 0.0018 (6) | 0.0023 (6) |
| C12 | 0.0352 (10) | 0.0406 (11) | 0.0287 (9) | 0.0197 (8) | −0.0058 (8) | 0.0024 (8) |
| C13 | 0.0275 (9) | 0.0155 (8) | 0.0613 (13) | 0.0039 (7) | −0.0013 (9) | 0.0013 (8) |
| C14 | 0.0362 (10) | 0.0296 (10) | 0.0402 (10) | 0.0125 (8) | 0.0202 (8) | 0.0069 (8) |
| C15 | 0.0190 (7) | 0.0236 (8) | 0.0206 (7) | −0.0001 (6) | 0.0057 (6) | 0.0004 (6) |
| C16 | 0.0277 (9) | 0.0297 (9) | 0.0263 (8) | −0.0070 (7) | 0.0070 (7) | 0.0042 (7) |
| C17 | 0.0345 (10) | 0.0516 (12) | 0.0187 (8) | −0.0090 (8) | 0.0097 (7) | −0.0082 (8) |
| C18 | 0.0289 (9) | 0.0360 (11) | 0.0577 (13) | 0.0138 (8) | 0.0180 (9) | 0.0095 (9) |
Geometric parameters (Å, °)
| Sn—Cl1 | 2.4847 (4) | C9—C10 | 1.384 (2) |
| Sn—S1 | 2.4760 (4) | C9—H9 | 0.9500 |
| Sn—S2 | 2.7409 (4) | C10—H10 | 0.9500 |
| Sn—C11 | 2.1884 (14) | C11—C12 | 1.522 (2) |
| Sn—C15 | 2.1879 (15) | C11—C14 | 1.523 (2) |
| S1—C1 | 1.7470 (15) | C11—C13 | 1.524 (2) |
| S2—C1 | 1.7109 (15) | C12—H12A | 0.9800 |
| N1—C1 | 1.3240 (18) | C12—H12B | 0.9800 |
| N1—C4 | 1.4791 (18) | C12—H12C | 0.9800 |
| N1—C2 | 1.4839 (19) | C13—H13A | 0.9800 |
| C2—C3 | 1.523 (2) | C13—H13B | 0.9800 |
| C2—H2A | 0.9900 | C13—H13C | 0.9800 |
| C2—H2B | 0.9900 | C14—H14A | 0.9800 |
| C3—H3A | 0.9800 | C14—H14B | 0.9800 |
| C3—H3B | 0.9800 | C14—H14C | 0.9800 |
| C3—H3C | 0.9800 | C15—C18 | 1.525 (2) |
| C4—C5 | 1.509 (2) | C15—C16 | 1.527 (2) |
| C4—H4A | 0.9900 | C15—C17 | 1.530 (2) |
| C4—H4B | 0.9900 | C16—H16A | 0.9800 |
| C5—C10 | 1.390 (2) | C16—H16B | 0.9800 |
| C5—C6 | 1.390 (2) | C16—H16C | 0.9800 |
| C6—C7 | 1.391 (2) | C17—H17A | 0.9800 |
| C6—H6 | 0.9500 | C17—H17B | 0.9800 |
| C7—C8 | 1.386 (2) | C17—H17C | 0.9800 |
| C7—H7 | 0.9500 | C18—H18A | 0.9800 |
| C8—C9 | 1.386 (2) | C18—H18B | 0.9800 |
| C8—H8 | 0.9500 | C18—H18C | 0.9800 |
| C15—Sn—C11 | 125.79 (6) | C9—C10—C5 | 120.31 (14) |
| C15—Sn—S1 | 117.55 (4) | C9—C10—H10 | 119.8 |
| C11—Sn—S1 | 115.59 (4) | C5—C10—H10 | 119.8 |
| C15—Sn—Cl1 | 98.77 (4) | C12—C11—C14 | 110.27 (15) |
| C11—Sn—Cl1 | 96.17 (4) | C12—C11—C13 | 109.80 (14) |
| S1—Sn—Cl1 | 84.342 (12) | C14—C11—C13 | 110.21 (14) |
| C15—Sn—S2 | 93.43 (4) | C12—C11—Sn | 108.21 (10) |
| C11—Sn—S2 | 96.04 (4) | C14—C11—Sn | 107.78 (10) |
| S1—Sn—S2 | 68.654 (12) | C13—C11—Sn | 110.52 (10) |
| Cl1—Sn—S2 | 152.989 (12) | C11—C12—H12A | 109.5 |
| C1—S1—Sn | 91.00 (5) | C11—C12—H12B | 109.5 |
| C1—S2—Sn | 83.22 (5) | H12A—C12—H12B | 109.5 |
| C1—N1—C4 | 122.17 (12) | C11—C12—H12C | 109.5 |
| C1—N1—C2 | 121.73 (12) | H12A—C12—H12C | 109.5 |
| C4—N1—C2 | 116.09 (11) | H12B—C12—H12C | 109.5 |
| N1—C1—S2 | 123.80 (11) | C11—C13—H13A | 109.5 |
| N1—C1—S1 | 119.10 (11) | C11—C13—H13B | 109.5 |
| S2—C1—S1 | 117.10 (8) | H13A—C13—H13B | 109.5 |
| N1—C2—C3 | 113.75 (12) | C11—C13—H13C | 109.5 |
| N1—C2—H2A | 108.8 | H13A—C13—H13C | 109.5 |
| C3—C2—H2A | 108.8 | H13B—C13—H13C | 109.5 |
| N1—C2—H2B | 108.8 | C11—C14—H14A | 109.5 |
| C3—C2—H2B | 108.8 | C11—C14—H14B | 109.5 |
| H2A—C2—H2B | 107.7 | H14A—C14—H14B | 109.5 |
| C2—C3—H3A | 109.5 | C11—C14—H14C | 109.5 |
| C2—C3—H3B | 109.5 | H14A—C14—H14C | 109.5 |
| H3A—C3—H3B | 109.5 | H14B—C14—H14C | 109.5 |
| C2—C3—H3C | 109.5 | C18—C15—C16 | 110.55 (15) |
| H3A—C3—H3C | 109.5 | C18—C15—C17 | 111.09 (15) |
| H3B—C3—H3C | 109.5 | C16—C15—C17 | 109.57 (14) |
| N1—C4—C5 | 110.67 (12) | C18—C15—Sn | 108.38 (11) |
| N1—C4—H4A | 109.5 | C16—C15—Sn | 108.51 (10) |
| C5—C4—H4A | 109.5 | C17—C15—Sn | 108.66 (10) |
| N1—C4—H4B | 109.5 | C15—C16—H16A | 109.5 |
| C5—C4—H4B | 109.5 | C15—C16—H16B | 109.5 |
| H4A—C4—H4B | 108.1 | H16A—C16—H16B | 109.5 |
| C10—C5—C6 | 119.24 (14) | C15—C16—H16C | 109.5 |
| C10—C5—C4 | 119.60 (13) | H16A—C16—H16C | 109.5 |
| C6—C5—C4 | 121.08 (14) | H16B—C16—H16C | 109.5 |
| C5—C6—C7 | 120.61 (15) | C15—C17—H17A | 109.5 |
| C5—C6—H6 | 119.7 | C15—C17—H17B | 109.5 |
| C7—C6—H6 | 119.7 | H17A—C17—H17B | 109.5 |
| C8—C7—C6 | 119.51 (15) | C15—C17—H17C | 109.5 |
| C8—C7—H7 | 120.2 | H17A—C17—H17C | 109.5 |
| C6—C7—H7 | 120.2 | H17B—C17—H17C | 109.5 |
| C9—C8—C7 | 120.14 (15) | C15—C18—H18A | 109.5 |
| C9—C8—H8 | 119.9 | C15—C18—H18B | 109.5 |
| C7—C8—H8 | 119.9 | H18A—C18—H18B | 109.5 |
| C10—C9—C8 | 120.15 (14) | C15—C18—H18C | 109.5 |
| C10—C9—H9 | 119.9 | H18A—C18—H18C | 109.5 |
| C8—C9—H9 | 119.9 | H18B—C18—H18C | 109.5 |
| C15—Sn—S1—C1 | −83.40 (7) | C8—C9—C10—C5 | 0.5 (2) |
| C11—Sn—S1—C1 | 85.49 (6) | C6—C5—C10—C9 | −2.0 (2) |
| Cl1—Sn—S1—C1 | 179.64 (5) | C4—C5—C10—C9 | 174.62 (14) |
| S2—Sn—S1—C1 | −0.96 (5) | C15—Sn—C11—C12 | −55.53 (13) |
| C15—Sn—S2—C1 | 119.28 (6) | S1—Sn—C11—C12 | 136.63 (11) |
| C11—Sn—S2—C1 | −114.17 (6) | Cl1—Sn—C11—C12 | 49.96 (11) |
| S1—Sn—S2—C1 | 0.98 (5) | S2—Sn—C11—C12 | −154.18 (11) |
| Cl1—Sn—S2—C1 | 2.29 (6) | C15—Sn—C11—C14 | −174.77 (11) |
| C4—N1—C1—S2 | 0.84 (19) | S1—Sn—C11—C14 | 17.39 (12) |
| C2—N1—C1—S2 | 179.45 (10) | Cl1—Sn—C11—C14 | −69.28 (11) |
| C4—N1—C1—S1 | −179.25 (10) | S2—Sn—C11—C14 | 86.58 (11) |
| C2—N1—C1—S1 | −0.64 (18) | C15—Sn—C11—C13 | 64.74 (14) |
| Sn—S2—C1—N1 | 178.46 (13) | S1—Sn—C11—C13 | −103.11 (12) |
| Sn—S2—C1—S1 | −1.46 (7) | Cl1—Sn—C11—C13 | 170.23 (12) |
| Sn—S1—C1—N1 | −178.32 (11) | S2—Sn—C11—C13 | −33.91 (12) |
| Sn—S1—C1—S2 | 1.60 (8) | C11—Sn—C15—C18 | −171.31 (11) |
| C1—N1—C2—C3 | −82.33 (17) | S1—Sn—C15—C18 | −3.68 (13) |
| C4—N1—C2—C3 | 96.36 (15) | Cl1—Sn—C15—C18 | 84.49 (12) |
| C1—N1—C4—C5 | 117.52 (15) | S2—Sn—C15—C18 | −71.34 (12) |
| C2—N1—C4—C5 | −61.16 (16) | C11—Sn—C15—C16 | −51.22 (13) |
| N1—C4—C5—C10 | −67.27 (17) | S1—Sn—C15—C16 | 116.41 (10) |
| N1—C4—C5—C6 | 109.31 (16) | Cl1—Sn—C15—C16 | −155.42 (10) |
| C10—C5—C6—C7 | 1.8 (2) | S2—Sn—C15—C16 | 48.75 (11) |
| C4—C5—C6—C7 | −174.75 (14) | C11—Sn—C15—C17 | 67.86 (14) |
| C5—C6—C7—C8 | −0.2 (2) | S1—Sn—C15—C17 | −124.51 (11) |
| C6—C7—C8—C9 | −1.4 (2) | Cl1—Sn—C15—C17 | −36.34 (12) |
| C7—C8—C9—C10 | 1.2 (2) | S2—Sn—C15—C17 | 167.83 (12) |
Hydrogen-bond geometry (Å, °)
| Cg1 is the centroid of the C5–C10 ring. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C3—H3a···Cg1 | 0.98 | 2.78 | 3.6491 (18) | 149 |
| C13—H13b···Cg1i | 0.98 | 2.96 | 3.5401 (18) | 119 |
Symmetry codes: (i) −x+1, −y, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZS2099).
References
- Abdul Muthalib, A. F., Baba, I., Mohamed Tahir, M. I., Ng, S. W. & Tiekink, E. R. T. (2010). Acta Cryst. E66, m1087. [DOI] [PMC free article] [PubMed]
- Addison, A. W., Rao, T. N., Reedijk, J., van Rijn, J. & Verschoor, G. C. (1984). J. Chem. Soc. Dalton Trans. pp. 1349–1356.
- Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Oxford Diffraction (2010). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
- Tiekink, E. R. T. (2008). Appl. Organomet. Chem. 22, 533–550.
- 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/S1600536811006398/zs2099sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006398/zs2099Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



