Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Feb 26;67(Pt 3):m372–m373. doi: 10.1107/S1600536811006398

(N-Benzyl-N-ethyl­dithio­carbamato)di-tert-butyl­chloridotin(IV)

Amirah Faizah Abdul Muthalib a, Ibrahim Baba a,‡, Mohamed Ibrahim Mohamed Tahir b, Edward R T Tiekink c,*
PMCID: PMC3051941  PMID: 21522295

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 ▶).graphic file with name e-67-0m372-scheme1.jpg

Experimental

Crystal data

  • [Sn(C4H9)2Cl(C10H12NS2)]

  • M r = 478.69

  • Triclinic, Inline graphic

  • 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

e-67-0m372-sup1.cif (22.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006398/zs2099Isup2.hkl

e-67-0m372-Isup2.hkl (233.4KB, 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) Inline graphic.

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.

Fig. 1.

The molecular structure of of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.

Fig. 2.

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.

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

  1. 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]
  2. Addison, A. W., Rao, T. N., Reedijk, J., van Rijn, J. & Verschoor, G. C. (1984). J. Chem. Soc. Dalton Trans. pp. 1349–1356.
  3. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  4. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  5. Oxford Diffraction (2010). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  8. Tiekink, E. R. T. (2008). Appl. Organomet. Chem. 22, 533–550.
  9. 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

e-67-0m372-sup1.cif (22.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006398/zs2099Isup2.hkl

e-67-0m372-Isup2.hkl (233.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES