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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 7;67(Pt 5):m551–m552. doi: 10.1107/S1600536811012414

(2,2′-Bipyridine-κ2 N,N′)bis­(N-isopropyl-N-methyl­dithio­carbamato-κ2 S,S′)cadmium

Nor Asiken Abdul Wahab a, Ibrahim Baba a,, Mohamed Ibrahim Mohamed Tahir b, Edward R T Tiekink c,*
PMCID: PMC3089361  PMID: 21754287

Abstract

The CdII atom in the title compound, [Cd(C5H10NS2)2(C10H8N2)], exists in an N2S4 donor set defined by two chelating dithio­carbamate anions as well as a 2,2′-bipyridine ligand. The coordination geometry approximates a trigonal prism. The crystal packing features weak C—H⋯S inter­actions, leading to linear supra­molecular chains along the a axis. The primary connections between these are by π–π stacking inter­actions [ring centroid distance between centrosymmetrically related pyridyl rings = 3.7455 (10) Å]. Overall, the crystal structure may be described as comprising double layers of mol­ecules that stack along the b axis.

Related literature

For related structures of pyridyl adducts of cadmium dithio­carbamtes, see: Song & Tiekink (2009); Broker & Tiekink (2011); Jamaluddin et al. (2011).graphic file with name e-67-0m551-scheme1.jpg

Experimental

Crystal data

  • [Cd(C5H10NS2)2(C10H8N2)]

  • M r = 565.10

  • Monoclinic, Inline graphic

  • a = 9.6061 (2) Å

  • b = 28.6277 (4) Å

  • c = 9.8187 (2) Å

  • β = 112.860 (2)°

  • V = 2488.07 (8) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.23 mm−1

  • T = 150 K

  • 0.17 × 0.13 × 0.05 mm

Data collection

  • Oxford Diffraction Xcaliber Eos Gemini diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.853, T max = 0.941

  • 53095 measured reflections

  • 5700 independent reflections

  • 5013 reflections with I > 2σ(I)

  • R int = 0.048

Refinement

  • R[F 2 > 2σ(F 2)] = 0.022

  • wR(F 2) = 0.053

  • S = 1.03

  • 5700 reflections

  • 268 parameters

  • H-atom parameters constrained

  • Δρmax = 0.42 e Å−3

  • Δρmin = −0.30 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/S1600536811012414/hb5834sup1.cif

e-67-0m551-sup1.cif (24.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811012414/hb5834Isup2.hkl

e-67-0m551-Isup2.hkl (273.5KB, hkl)

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

Table 1. Selected bond lengths (Å).

Cd—S1 2.6463 (5)
Cd—S2 2.7128 (5)
Cd—S3 2.6518 (5)
Cd—S4 2.6490 (5)
Cd—N3 2.4122 (14)
Cd—N4 2.4191 (15)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C18—H18⋯S2i 0.95 2.78 3.712 (2) 167

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

In continuation of systematic structural studies of various pyridyl adducts of cadmium dithiocarbamates (Song & Tiekink, 2009; Broker & Tiekink, 2011; Jamaluddin et al., 2011), the title compound Cd[S2CN(Me)iPr)2]2(2,2'-bipyridine), (I), was investigated. The CdII atom is coordinated by two dithiocarbamate ligands, each essentially forming symmetric Cd—S bonds, and a symmetrically chelating 2,2'-bipyridine ligand, Fig. 1 and Table 1. The equivalence in the Cd—S bond distances is reflected in the narrow range of associated C≐S bond distances, i.e. 1.7168 (18) to 1.7290 (17) Å. A small twist is noted between the pyridyl rings of the 2,2'-bipyridine ligand as seen in the dihedral angle of 9.25 (9) ° formed between the rings. The N2S4 donor set defines a distorted trigonal prismatic geometry.

The crystal packing of (I) features linear supramolecular chains along the a axis that are sustained by C—H···S interactions, Fig. 2 and Table 2. Chains lie in the ac plane and inter-digitate viaπ–π interactions with centrosymmetrically related layers to form a double layer [ring centroid(N3-pyridyl)···ring centroid(N3-centroid)i = 3.7455 (10) Å for i: 2 - x, 1 - y, 1 - z]. Double layers stack along the b axis and are separated by hydrophobic interactions, Fig. 3.

Experimental

The title compound was prepared using an in situ method by the addition of carbon disulfide (0.02 mol) to an ethanolic solution (20 ml) of methylisopropropylamine (0.02 mol) and 2,2-bipyridine (0.01 mol) in ethanol (20 ml). The mixture was stirred for 1 h at 277 K. The resulting solution was added drop-wise to a solution of cadmium(II) dichloride (0.01 mol) in ethanol (20 ml). The mixture was stirred 3 h. The yellowish precipitate was filtered, washed with cold ethanol and dried in a desiccator. Recrystallization was from ethanol:chloroform (1:2 v/v) to yield yellow prisms of (I). M.pt. 473.6–475.2 K. Elemental analysis. Found (calculated) for C22H32CdN4S4: C, 42.63 (42.51); H 4.48 (4.99); N 10.74 (9.91); S 21.80 (22.70) %. UV (CHCl3) λmax 283.5 and 261.0 nm (L(π) →L(π*)). IR (KBr): ν(C—H) 2928 s; ν(C≐N) 1565 s; ν(N—C) 1468 m; ν(C≐S) 970 s; ν(Cd—S) 381 s cm-1.

Refinement

Carbon-bound H-atoms were placed in calculated positions (C—H 0.95 to 1.00 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2 to 1.5Uequiv(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

A view of the linear supramolecular chain long the a axis in (I) mediated by C—H···S interactions (orange dashed lines) along the a axis.

Fig. 3.

Fig. 3.

A view in projection down the a axis of the crystal packing in (I) highlighting the π–π interactions (shown as purple dashed lines).

Crystal data

[Cd(C5H10NS2)2(C10H8N2)] F(000) = 1152
Mr = 565.10 Dx = 1.509 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 26576 reflections
a = 9.6061 (2) Å θ = 2–29°
b = 28.6277 (4) Å µ = 1.23 mm1
c = 9.8187 (2) Å T = 150 K
β = 112.860 (2)° Prism, yellow
V = 2488.07 (8) Å3 0.17 × 0.13 × 0.05 mm
Z = 4

Data collection

Oxford Diffraction Xcaliber Eos Gemini diffractometer 5700 independent reflections
Radiation source: fine-focus sealed tube 5013 reflections with I > 2σ(I)
graphite Rint = 0.048
Detector resolution: 16.1952 pixels mm-1 θmax = 27.5°, θmin = 2.4°
ω scans h = −12→12
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) k = −37→37
Tmin = 0.853, Tmax = 0.941 l = −12→12
53095 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)] = 0.022 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.053 H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.023P)2 + 0.9719P] where P = (Fo2 + 2Fc2)/3
5700 reflections (Δ/σ)max = 0.002
268 parameters Δρmax = 0.42 e Å3
0 restraints Δρmin = −0.30 e Å3

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
Cd 1.074719 (14) 0.619541 (4) 0.837624 (13) 0.02469 (5)
S1 1.13178 (5) 0.638504 (17) 1.11803 (5) 0.02979 (10)
S2 1.37352 (5) 0.615697 (17) 1.01159 (5) 0.03243 (10)
S3 0.88132 (5) 0.688040 (16) 0.71256 (5) 0.03348 (11)
S4 1.10292 (5) 0.651618 (17) 0.59657 (5) 0.03368 (11)
N1 1.42420 (16) 0.63344 (5) 1.29241 (16) 0.0285 (3)
N2 0.91865 (17) 0.72387 (5) 0.47972 (17) 0.0313 (3)
N3 1.09345 (17) 0.54076 (5) 0.75929 (16) 0.0282 (3)
N4 0.87517 (16) 0.56931 (5) 0.84481 (16) 0.0292 (3)
C1 1.32019 (19) 0.62947 (6) 1.15504 (19) 0.0254 (3)
C2 1.5853 (2) 0.63217 (9) 1.3206 (2) 0.0448 (5)
H2A 1.6125 0.6009 1.2987 0.067*
H2B 1.6444 0.6397 1.4245 0.067*
H2C 1.6070 0.6551 1.2573 0.067*
C3 1.3829 (2) 0.64480 (7) 1.41991 (19) 0.0296 (4)
H3 1.2720 0.6392 1.3881 0.036*
C4 1.4639 (3) 0.61310 (9) 1.5506 (3) 0.0521 (6)
H4A 1.4428 0.5804 1.5198 0.078*
H4B 1.4281 0.6196 1.6296 0.078*
H4C 1.5729 0.6188 1.5870 0.078*
C5 1.4115 (2) 0.69603 (7) 1.4595 (2) 0.0414 (5)
H5A 1.5206 0.7020 1.5016 0.062*
H5B 1.3688 0.7042 1.5322 0.062*
H5C 1.3637 0.7151 1.3705 0.062*
C6 0.96267 (19) 0.69114 (6) 0.58500 (19) 0.0253 (3)
C7 0.7956 (2) 0.75621 (7) 0.4673 (3) 0.0439 (5)
H7A 0.7009 0.7388 0.4401 0.066*
H7B 0.7853 0.7796 0.3912 0.066*
H7C 0.8185 0.7718 0.5624 0.066*
C8 0.9824 (2) 0.72780 (7) 0.3644 (2) 0.0374 (5)
H8 1.0722 0.7067 0.3931 0.045*
C9 1.0361 (3) 0.77737 (8) 0.3560 (2) 0.0491 (6)
H9A 0.9485 0.7980 0.3128 0.074*
H9B 1.0953 0.7777 0.2942 0.074*
H9C 1.0991 0.7883 0.4557 0.074*
C10 0.8681 (3) 0.71105 (8) 0.2173 (2) 0.0455 (5)
H10A 0.8415 0.6785 0.2264 0.068*
H10B 0.9116 0.7133 0.1423 0.068*
H10C 0.7772 0.7305 0.1880 0.068*
C11 1.1989 (2) 0.52925 (7) 0.7083 (2) 0.0359 (4)
H11 1.2712 0.5522 0.7104 0.043*
C12 1.2078 (2) 0.48551 (7) 0.6527 (2) 0.0405 (5)
H12 1.2837 0.4786 0.6162 0.049*
C13 1.1038 (2) 0.45225 (7) 0.6515 (2) 0.0405 (5)
H13 1.1069 0.4218 0.6140 0.049*
C14 0.9948 (2) 0.46353 (6) 0.7053 (2) 0.0349 (4)
H14 0.9226 0.4409 0.7059 0.042*
C15 0.99217 (19) 0.50838 (6) 0.75862 (18) 0.0269 (4)
C16 0.87718 (19) 0.52370 (6) 0.81662 (18) 0.0265 (4)
C17 0.7754 (2) 0.58528 (7) 0.8983 (2) 0.0355 (4)
H17 0.7746 0.6177 0.9183 0.043*
C18 0.6735 (2) 0.55653 (8) 0.9256 (2) 0.0394 (5)
H18 0.6034 0.5689 0.9627 0.047*
C19 0.6762 (2) 0.50964 (8) 0.8977 (2) 0.0436 (5)
H19 0.6081 0.4890 0.9161 0.052*
C20 0.7787 (2) 0.49272 (7) 0.8427 (2) 0.0387 (4)
H20 0.7819 0.4603 0.8230 0.046*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cd 0.02824 (7) 0.02325 (7) 0.02276 (7) 0.00063 (5) 0.01010 (5) 0.00100 (5)
S1 0.0242 (2) 0.0389 (3) 0.0253 (2) 0.00347 (18) 0.00845 (17) −0.00182 (18)
S2 0.0316 (2) 0.0385 (3) 0.0299 (2) 0.00315 (19) 0.01483 (19) −0.00517 (19)
S3 0.0408 (3) 0.0309 (2) 0.0352 (3) 0.0088 (2) 0.0218 (2) 0.00636 (19)
S4 0.0373 (2) 0.0349 (2) 0.0347 (2) 0.01276 (19) 0.0204 (2) 0.01318 (19)
N1 0.0226 (7) 0.0347 (8) 0.0274 (8) −0.0005 (6) 0.0089 (6) −0.0037 (6)
N2 0.0307 (8) 0.0292 (8) 0.0381 (9) 0.0075 (6) 0.0177 (7) 0.0115 (6)
N3 0.0329 (8) 0.0267 (8) 0.0280 (8) 0.0006 (6) 0.0150 (6) 0.0020 (6)
N4 0.0288 (8) 0.0293 (8) 0.0291 (8) 0.0015 (6) 0.0108 (6) 0.0016 (6)
C1 0.0267 (8) 0.0203 (8) 0.0291 (9) −0.0001 (6) 0.0109 (7) 0.0008 (6)
C2 0.0228 (9) 0.0629 (14) 0.0460 (12) 0.0012 (9) 0.0103 (9) −0.0117 (10)
C3 0.0255 (8) 0.0390 (10) 0.0239 (9) 0.0000 (7) 0.0091 (7) 0.0016 (7)
C4 0.0520 (14) 0.0628 (15) 0.0412 (13) 0.0102 (11) 0.0177 (11) 0.0200 (11)
C5 0.0482 (12) 0.0441 (12) 0.0366 (11) −0.0062 (9) 0.0217 (9) −0.0101 (9)
C6 0.0257 (8) 0.0213 (8) 0.0284 (9) −0.0028 (6) 0.0099 (7) −0.0003 (7)
C7 0.0452 (12) 0.0355 (11) 0.0595 (14) 0.0161 (9) 0.0297 (11) 0.0192 (10)
C8 0.0332 (10) 0.0431 (11) 0.0405 (11) 0.0109 (8) 0.0191 (9) 0.0195 (9)
C9 0.0434 (12) 0.0626 (15) 0.0373 (12) −0.0150 (11) 0.0115 (10) 0.0146 (10)
C10 0.0553 (13) 0.0397 (12) 0.0475 (13) 0.0006 (10) 0.0265 (11) 0.0006 (9)
C11 0.0420 (11) 0.0308 (10) 0.0415 (11) 0.0001 (8) 0.0234 (9) 0.0012 (8)
C12 0.0468 (12) 0.0376 (11) 0.0445 (12) 0.0083 (9) 0.0259 (10) 0.0009 (9)
C13 0.0465 (12) 0.0287 (10) 0.0446 (12) 0.0072 (9) 0.0160 (10) −0.0030 (8)
C14 0.0350 (10) 0.0259 (9) 0.0404 (11) −0.0001 (8) 0.0110 (8) −0.0009 (8)
C15 0.0291 (9) 0.0249 (9) 0.0231 (8) 0.0017 (7) 0.0061 (7) 0.0044 (7)
C16 0.0248 (8) 0.0267 (9) 0.0248 (9) 0.0025 (7) 0.0062 (7) 0.0052 (7)
C17 0.0343 (10) 0.0365 (10) 0.0370 (11) 0.0046 (8) 0.0154 (8) 0.0001 (8)
C18 0.0298 (10) 0.0513 (13) 0.0397 (11) 0.0089 (9) 0.0164 (8) 0.0089 (9)
C19 0.0337 (10) 0.0461 (12) 0.0551 (13) 0.0011 (9) 0.0216 (10) 0.0161 (10)
C20 0.0355 (10) 0.0303 (10) 0.0513 (12) 0.0015 (8) 0.0181 (9) 0.0084 (9)

Geometric parameters (Å, °)

Cd—S1 2.6463 (5) C5—H5C 0.9800
Cd—S2 2.7128 (5) C7—H7A 0.9800
Cd—S3 2.6518 (5) C7—H7B 0.9800
Cd—S4 2.6490 (5) C7—H7C 0.9800
Cd—N3 2.4122 (14) C8—C10 1.512 (3)
Cd—N4 2.4191 (15) C8—C9 1.523 (3)
S1—C1 1.7215 (18) C8—H8 1.0000
S2—C1 1.7212 (18) C9—H9A 0.9800
S3—C6 1.7168 (18) C9—H9B 0.9800
S4—C6 1.7290 (17) C9—H9C 0.9800
N1—C1 1.335 (2) C10—H10A 0.9800
N1—C2 1.463 (2) C10—H10B 0.9800
N1—C3 1.488 (2) C10—H10C 0.9800
N2—C6 1.336 (2) C11—C12 1.382 (3)
N2—C7 1.469 (2) C11—H11 0.9500
N2—C8 1.486 (2) C12—C13 1.377 (3)
N3—C11 1.334 (2) C12—H12 0.9500
N3—C15 1.342 (2) C13—C14 1.382 (3)
N4—C16 1.337 (2) C13—H13 0.9500
N4—C17 1.340 (2) C14—C15 1.390 (2)
C2—H2A 0.9800 C14—H14 0.9500
C2—H2B 0.9800 C15—C16 1.492 (2)
C2—H2C 0.9800 C16—C20 1.391 (3)
C3—C5 1.515 (3) C17—C18 1.382 (3)
C3—C4 1.516 (3) C17—H17 0.9500
C3—H3 1.0000 C18—C19 1.372 (3)
C4—H4A 0.9800 C18—H18 0.9500
C4—H4B 0.9800 C19—C20 1.382 (3)
C4—H4C 0.9800 C19—H19 0.9500
C5—H5A 0.9800 C20—H20 0.9500
C5—H5B 0.9800
N3—Cd—N4 67.15 (5) N2—C6—S3 120.24 (13)
N3—Cd—S1 120.84 (4) N2—C6—S4 120.93 (13)
N4—Cd—S1 86.43 (4) S3—C6—S4 118.83 (10)
N3—Cd—S4 89.60 (4) N2—C7—H7A 109.5
N4—Cd—S4 126.11 (4) N2—C7—H7B 109.5
S1—Cd—S4 143.780 (17) H7A—C7—H7B 109.5
N3—Cd—S3 132.02 (4) N2—C7—H7C 109.5
N4—Cd—S3 91.86 (4) H7A—C7—H7C 109.5
S1—Cd—S3 98.905 (15) H7B—C7—H7C 109.5
S4—Cd—S3 68.057 (14) N2—C8—C10 110.03 (16)
N3—Cd—S2 88.34 (4) N2—C8—C9 111.10 (17)
N4—Cd—S2 127.89 (4) C10—C8—C9 112.31 (16)
S1—Cd—S2 67.192 (14) N2—C8—H8 107.7
S4—Cd—S2 97.251 (15) C10—C8—H8 107.7
S3—Cd—S2 134.517 (16) C9—C8—H8 107.7
C1—S1—Cd 87.98 (6) C8—C9—H9A 109.5
C1—S2—Cd 85.84 (6) C8—C9—H9B 109.5
C6—S3—Cd 86.59 (6) H9A—C9—H9B 109.5
C6—S4—Cd 86.44 (6) C8—C9—H9C 109.5
C1—N1—C2 120.67 (15) H9A—C9—H9C 109.5
C1—N1—C3 121.93 (14) H9B—C9—H9C 109.5
C2—N1—C3 117.02 (14) C8—C10—H10A 109.5
C6—N2—C7 120.58 (15) C8—C10—H10B 109.5
C6—N2—C8 122.85 (15) H10A—C10—H10B 109.5
C7—N2—C8 116.46 (14) C8—C10—H10C 109.5
C11—N3—C15 118.85 (16) H10A—C10—H10C 109.5
C11—N3—Cd 120.81 (12) H10B—C10—H10C 109.5
C15—N3—Cd 120.24 (11) N3—C11—C12 123.01 (18)
C16—N4—C17 118.99 (16) N3—C11—H11 118.5
C16—N4—Cd 119.95 (11) C12—C11—H11 118.5
C17—N4—Cd 120.30 (12) C13—C12—C11 118.27 (19)
N1—C1—S2 120.15 (13) C13—C12—H12 120.9
N1—C1—S1 120.87 (13) C11—C12—H12 120.9
S2—C1—S1 118.97 (10) C12—C13—C14 119.36 (18)
N1—C2—H2A 109.5 C12—C13—H13 120.3
N1—C2—H2B 109.5 C14—C13—H13 120.3
H2A—C2—H2B 109.5 C13—C14—C15 119.15 (18)
N1—C2—H2C 109.5 C13—C14—H14 120.4
H2A—C2—H2C 109.5 C15—C14—H14 120.4
H2B—C2—H2C 109.5 N3—C15—C14 121.37 (17)
N1—C3—C5 110.28 (15) N3—C15—C16 115.97 (15)
N1—C3—C4 111.39 (16) C14—C15—C16 122.66 (16)
C5—C3—C4 112.32 (17) N4—C16—C20 121.27 (17)
N1—C3—H3 107.5 N4—C16—C15 116.02 (15)
C5—C3—H3 107.5 C20—C16—C15 122.70 (16)
C4—C3—H3 107.5 N4—C17—C18 122.76 (19)
C3—C4—H4A 109.5 N4—C17—H17 118.6
C3—C4—H4B 109.5 C18—C17—H17 118.6
H4A—C4—H4B 109.5 C19—C18—C17 118.32 (19)
C3—C4—H4C 109.5 C19—C18—H18 120.8
H4A—C4—H4C 109.5 C17—C18—H18 120.8
H4B—C4—H4C 109.5 C18—C19—C20 119.48 (19)
C3—C5—H5A 109.5 C18—C19—H19 120.3
C3—C5—H5B 109.5 C20—C19—H19 120.3
H5A—C5—H5B 109.5 C19—C20—C16 119.17 (19)
C3—C5—H5C 109.5 C19—C20—H20 120.4
H5A—C5—H5C 109.5 C16—C20—H20 120.4
H5B—C5—H5C 109.5
N3—Cd—S1—C1 72.53 (7) Cd—S2—C1—S1 −1.23 (9)
N4—Cd—S1—C1 133.16 (7) Cd—S1—C1—N1 −179.36 (14)
S4—Cd—S1—C1 −70.74 (6) Cd—S1—C1—S2 1.26 (9)
S3—Cd—S1—C1 −135.51 (6) C1—N1—C3—C5 −100.74 (19)
S2—Cd—S1—C1 −0.76 (6) C2—N1—C3—C5 72.2 (2)
N3—Cd—S2—C1 −123.88 (7) C1—N1—C3—C4 133.84 (18)
N4—Cd—S2—C1 −64.86 (7) C2—N1—C3—C4 −53.2 (2)
S1—Cd—S2—C1 0.76 (6) C7—N2—C6—S3 −2.8 (2)
S4—Cd—S2—C1 146.73 (6) C8—N2—C6—S3 −178.74 (14)
S3—Cd—S2—C1 80.51 (6) C7—N2—C6—S4 177.74 (15)
N3—Cd—S3—C6 −69.81 (7) C8—N2—C6—S4 1.8 (2)
N4—Cd—S3—C6 −130.23 (7) Cd—S3—C6—N2 −176.65 (14)
S1—Cd—S3—C6 143.09 (6) Cd—S3—C6—S4 2.79 (9)
S4—Cd—S3—C6 −1.72 (6) Cd—S4—C6—N2 176.64 (14)
S2—Cd—S3—C6 76.43 (6) Cd—S4—C6—S3 −2.79 (9)
N3—Cd—S4—C6 138.13 (7) C6—N2—C8—C10 106.5 (2)
N4—Cd—S4—C6 77.20 (7) C7—N2—C8—C10 −69.5 (2)
S1—Cd—S4—C6 −72.77 (6) C6—N2—C8—C9 −128.48 (19)
S3—Cd—S4—C6 1.71 (6) C7—N2—C8—C9 55.5 (2)
S2—Cd—S4—C6 −133.59 (6) C15—N3—C11—C12 0.9 (3)
N4—Cd—N3—C11 175.46 (15) Cd—N3—C11—C12 −175.40 (15)
S1—Cd—N3—C11 −113.83 (13) N3—C11—C12—C13 −0.7 (3)
S4—Cd—N3—C11 45.48 (14) C11—C12—C13—C14 0.0 (3)
S3—Cd—N3—C11 104.86 (14) C12—C13—C14—C15 0.4 (3)
S2—Cd—N3—C11 −51.79 (14) C11—N3—C15—C14 −0.4 (3)
N4—Cd—N3—C15 −0.80 (12) Cd—N3—C15—C14 175.94 (13)
S1—Cd—N3—C15 69.92 (13) C11—N3—C15—C16 −179.77 (16)
S4—Cd—N3—C15 −130.78 (12) Cd—N3—C15—C16 −3.45 (19)
S3—Cd—N3—C15 −71.39 (13) C13—C14—C15—N3 −0.3 (3)
S2—Cd—N3—C15 131.96 (12) C13—C14—C15—C16 179.07 (17)
N3—Cd—N4—C16 5.64 (12) C17—N4—C16—C20 −0.5 (3)
S1—Cd—N4—C16 −120.06 (12) Cd—N4—C16—C20 169.56 (13)
S4—Cd—N4—C16 77.17 (13) C17—N4—C16—C15 −179.46 (15)
S3—Cd—N4—C16 141.13 (12) Cd—N4—C16—C15 −9.43 (19)
S2—Cd—N4—C16 −62.79 (14) N3—C15—C16—N4 8.4 (2)
N3—Cd—N4—C17 175.54 (15) C14—C15—C16—N4 −171.00 (16)
S1—Cd—N4—C17 49.84 (13) N3—C15—C16—C20 −170.60 (16)
S4—Cd—N4—C17 −112.93 (13) C14—C15—C16—C20 10.0 (3)
S3—Cd—N4—C17 −48.97 (14) C16—N4—C17—C18 −0.1 (3)
S2—Cd—N4—C17 107.11 (13) Cd—N4—C17—C18 −170.09 (14)
C2—N1—C1—S2 7.9 (2) N4—C17—C18—C19 0.6 (3)
C3—N1—C1—S2 −179.35 (13) C17—C18—C19—C20 −0.5 (3)
C2—N1—C1—S1 −171.46 (15) C18—C19—C20—C16 −0.1 (3)
C3—N1—C1—S1 1.3 (2) N4—C16—C20—C19 0.5 (3)
Cd—S2—C1—N1 179.38 (14) C15—C16—C20—C19 179.47 (18)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C18—H18···S2i 0.95 2.78 3.712 (2) 167

Symmetry codes: (i) x−1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB5834).

References

  1. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  2. Broker, G. A. & Tiekink, E. R. T. (2011). Acta Cryst. E67, m320–m321. [DOI] [PMC free article] [PubMed]
  3. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  4. Jamaluddin, N. A., Baba, I., Mohamed Tahir, M. I. & Tiekink, E. R. T. (2011). Acta Cryst. E67, m384–m385. [DOI] [PMC free article] [PubMed]
  5. Oxford Diffraction (2010). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
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  7. Song, J. C. & Tiekink, E. R. T. (2009). Acta Cryst. E65, m1669–m1670. [DOI] [PMC free article] [PubMed]
  8. 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/S1600536811012414/hb5834sup1.cif

e-67-0m551-sup1.cif (24.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811012414/hb5834Isup2.hkl

e-67-0m551-Isup2.hkl (273.5KB, hkl)

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


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