metal-organic compounds
catena-Poly[[trimethyl(4-sulfanylphenyl)azanium] [(chloridocadmate)-di-μ-chlorido]]
aCollege of Chemistry & Materials Engineering, Jiangsu Laboratory of Advanced Functional Materials, Changshu Institute of Technology, Changshu, 215500, Jiangsu, People's Republic of China, and bKey Laboratory of Organic Synthesis of Jiangsu Province, School of Chemistry and Chemical Engineering, Suzhou Uinversity, Suzhou 215123, Jiangsu, People's Republic of China
*Correspondence e-mail: chemxytang@hotmail.com
The title compound, {(C9H14NS)[CdCl3]}n, consists of a linear [CdCl3]nn− polyanion and a trimethyl(4-sulfanylphenyl)azanium cation. The CdII atom is pentacoordinated by four μ2-Cl atoms and one terminal Cl atom in a trigonal–bipyramidal geometry. The trigonal–bipyramidal units are linked by two opposite shared faces, giving rise to infinite [CdCl3]n chains parallel to the a axis. The cations surround the chain and are linked to them by S—H⋯Cl and C—H⋯Cl hydrogen bonds, forming a three-dimensional network.
Related literature
For the synthesis of trimethylammoniumphenyl-4-thiol hexafluoridophosphate, see: DePamphilis et al. (1974).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku/MSC, 2001); cell CrystalClear; data reduction: CrystalStructure (Rigaku/MSC, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.
Supporting information
https://doi.org/10.1107/S1600536811050513/ng5241sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536811050513/ng5241Isup2.hkl
The synthesis of trimethylammoniumphenyl-4-thiol hexafluorophosphate was according to the literature procedure (DePamphilis et al., 1974). To a suspension containing TabHPF6 (0.125 mg, 0.4 mmol) in MeOH (15 ml) was added Et3N (0.5 ml). The resulting colorless solution was then treated with a solution of CdCl2.2.5H2O (0.091 g, 0.4 mmol) in MeOH (10 ml). The mixture was stirred at room temperature for 1 h and treated with HCl to adjust the pH to 3, and then filtered. Diethyl ether (20 ml) was allowed to diffuse onto the filtrate. After standing it at ambient temperature for one week, colorless block crystals of (I) were formed. Yield: 0.100 g (65% based on Cd). The crystal used for the
determination was obtained directly from the above preparation. Analysis, found: C, 27.52; H, 3.31; N, 4.02%. calculated. for C9H14NSCdCl3: C, 27.93; H, 3.65; N, 3.62%.Carbon-bond H atoms were positioned geometrically (C—H = 0.94 Å for methylene group and C—H = 0.97 Å for methyl group), and were included in the
in the riding mode approximation, with Uiso(H) = 1.2Ueq(C)for methylene group and Uiso(H) = 1.5Ueq(C)for methyl group. The H atom attached to atom S1 was located in a difference Fourier map and refined isotropically without constraints with Uiso(H) values fixed at 1.2Ueq(S)].For the synthesis of trimethylammoniumphenyl-4-thiol hexafluorophosphate, see: DePamphilis et al. (1974).
Data collection: CrystalClear (Rigaku/MSC, 2001); cell
CrystalClear (Rigaku/MSC, 2001); data reduction: CrystalStructure (Rigaku/MSC, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).(C9H14NS)[CdCl3] | F(000) = 760 |
Mr = 387.04 | Dx = 1.883 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 3007 reflections |
a = 7.3207 (15) Å | θ = 3.0–25.4° |
b = 20.971 (4) Å | µ = 2.31 mm−1 |
c = 9.1613 (18) Å | T = 223 K |
β = 103.96 (3)° | Block, colorless |
V = 1364.9 (5) Å3 | 0.50 × 0.30 × 0.20 mm |
Z = 4 |
Rigaku Mercury diffractometer | 2491 independent reflections |
Radiation source: fine-focus sealed tube | 2424 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.027 |
ω scans | θmax = 25.4°, θmin = 3.0° |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC2001) | h = −8→7 |
Tmin = 0.442, Tmax = 0.635 | k = −22→25 |
12984 measured reflections | l = −11→11 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.026 | H-atom parameters constrained |
wR(F2) = 0.069 | w = 1/[σ2(Fo2) + (0.038P)2 + 0.9902P] where P = (Fo2 + 2Fc2)/3 |
S = 1.11 | (Δ/σ)max < 0.001 |
2491 reflections | Δρmax = 0.56 e Å−3 |
137 parameters | Δρmin = −0.79 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0059 (5) |
(C9H14NS)[CdCl3] | V = 1364.9 (5) Å3 |
Mr = 387.04 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 7.3207 (15) Å | µ = 2.31 mm−1 |
b = 20.971 (4) Å | T = 223 K |
c = 9.1613 (18) Å | 0.50 × 0.30 × 0.20 mm |
β = 103.96 (3)° |
Rigaku Mercury diffractometer | 2491 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC2001) | 2424 reflections with I > 2σ(I) |
Tmin = 0.442, Tmax = 0.635 | Rint = 0.027 |
12984 measured reflections |
R[F2 > 2σ(F2)] = 0.026 | 0 restraints |
wR(F2) = 0.069 | H-atom parameters constrained |
S = 1.11 | Δρmax = 0.56 e Å−3 |
2491 reflections | Δρmin = −0.79 e Å−3 |
137 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cd1 | 0.73386 (3) | 0.993777 (10) | 0.92593 (2) | 0.02485 (11) | |
Cl1 | 0.95247 (10) | 1.08537 (3) | 0.99446 (8) | 0.02873 (17) | |
Cl2 | 0.68785 (10) | 0.96938 (3) | 0.66114 (7) | 0.03076 (18) | |
Cl3 | 0.59419 (8) | 0.93630 (3) | 1.11069 (7) | 0.03094 (18) | |
S1 | 0.67638 (8) | 0.79389 (3) | 0.84461 (7) | 0.0484 (2) | |
H1 | 0.7952 | 0.8326 | 0.8962 | 0.058* | |
C1 | 0.5039 (4) | 0.74912 (14) | 0.9045 (3) | 0.0285 (6) | |
C2 | 0.3807 (4) | 0.77654 (14) | 0.9805 (3) | 0.0319 (6) | |
H2 | 0.3876 | 0.8205 | 1.0016 | 0.038* | |
C3 | 0.2478 (4) | 0.73917 (14) | 1.0253 (3) | 0.0303 (6) | |
H3 | 0.1638 | 0.7577 | 1.0760 | 0.036* | |
C4 | 0.2392 (4) | 0.67468 (13) | 0.9952 (3) | 0.0238 (6) | |
C5 | 0.3603 (4) | 0.64695 (14) | 0.9182 (3) | 0.0278 (6) | |
H5 | 0.3540 | 0.6030 | 0.8977 | 0.033* | |
C6 | 0.4898 (4) | 0.68458 (14) | 0.8721 (3) | 0.0301 (6) | |
H6 | 0.5700 | 0.6662 | 0.8177 | 0.036* | |
C7 | 0.2022 (4) | 0.58027 (15) | 1.1450 (4) | 0.0350 (7) | |
H7A | 0.2689 | 0.5534 | 1.0889 | 0.053* | |
H7B | 0.1119 | 0.5548 | 1.1813 | 0.053* | |
H7C | 0.2914 | 0.5991 | 1.2297 | 0.053* | |
C8 | −0.0195 (4) | 0.66781 (15) | 1.1295 (3) | 0.0342 (7) | |
H8A | 0.0607 | 0.6878 | 1.2174 | 0.051* | |
H8B | −0.1042 | 0.6381 | 1.1610 | 0.051* | |
H8C | −0.0922 | 0.7003 | 1.0654 | 0.051* | |
C9 | −0.0285 (4) | 0.60310 (16) | 0.9076 (3) | 0.0357 (7) | |
H9A | −0.0869 | 0.6365 | 0.8389 | 0.054* | |
H9B | −0.1251 | 0.5785 | 0.9381 | 0.054* | |
H9C | 0.0436 | 0.5754 | 0.8578 | 0.054* | |
N1 | 0.1003 (3) | 0.63245 (11) | 1.0439 (2) | 0.0250 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cd1 | 0.02433 (16) | 0.02926 (16) | 0.02258 (16) | −0.00438 (7) | 0.00880 (10) | −0.00082 (7) |
Cl1 | 0.0240 (3) | 0.0261 (4) | 0.0358 (4) | −0.0021 (3) | 0.0065 (3) | −0.0020 (3) |
Cl2 | 0.0328 (4) | 0.0364 (4) | 0.0230 (3) | 0.0030 (3) | 0.0066 (3) | −0.0025 (3) |
Cl3 | 0.0280 (4) | 0.0330 (4) | 0.0359 (4) | 0.0061 (3) | 0.0157 (3) | 0.0131 (3) |
S1 | 0.0499 (5) | 0.0405 (5) | 0.0632 (6) | −0.0145 (4) | 0.0301 (4) | 0.0025 (4) |
C1 | 0.0287 (15) | 0.0301 (15) | 0.0267 (14) | −0.0036 (11) | 0.0066 (11) | 0.0032 (11) |
C2 | 0.0352 (16) | 0.0247 (15) | 0.0366 (16) | −0.0010 (12) | 0.0105 (12) | −0.0012 (12) |
C3 | 0.0336 (16) | 0.0282 (16) | 0.0322 (15) | 0.0008 (12) | 0.0141 (12) | −0.0046 (12) |
C4 | 0.0220 (13) | 0.0257 (14) | 0.0240 (14) | −0.0025 (11) | 0.0065 (10) | 0.0012 (11) |
C5 | 0.0310 (15) | 0.0246 (15) | 0.0297 (15) | −0.0001 (11) | 0.0112 (12) | −0.0034 (11) |
C6 | 0.0296 (15) | 0.0310 (16) | 0.0337 (16) | 0.0005 (12) | 0.0152 (12) | −0.0025 (12) |
C7 | 0.0374 (17) | 0.0319 (17) | 0.0379 (17) | 0.0022 (13) | 0.0133 (13) | 0.0094 (13) |
C8 | 0.0333 (16) | 0.0372 (17) | 0.0377 (17) | −0.0009 (13) | 0.0197 (13) | −0.0029 (13) |
C9 | 0.0304 (16) | 0.0440 (18) | 0.0339 (16) | −0.0111 (13) | 0.0101 (12) | −0.0082 (13) |
N1 | 0.0265 (12) | 0.0262 (12) | 0.0245 (11) | −0.0007 (9) | 0.0102 (9) | 0.0000 (9) |
Cd1—Cl2 | 2.4219 (8) | C4—N1 | 1.496 (3) |
Cd1—Cl1 | 2.4819 (8) | C5—C6 | 1.375 (4) |
Cd1—Cl3 | 2.4896 (7) | C5—H5 | 0.9400 |
Cd1—Cl3i | 2.7643 (7) | C6—H6 | 0.9400 |
Cd1—Cl1ii | 2.7842 (9) | C7—N1 | 1.509 (4) |
Cl1—Cd1ii | 2.7842 (9) | C7—H7A | 0.9700 |
Cl3—Cd1i | 2.7643 (7) | C7—H7B | 0.9700 |
S1—C1 | 1.764 (3) | C7—H7C | 0.9700 |
S1—H1 | 1.1999 | C8—N1 | 1.505 (4) |
C1—C6 | 1.384 (4) | C8—H8A | 0.9700 |
C1—C2 | 1.390 (4) | C8—H8B | 0.9700 |
C2—C3 | 1.386 (4) | C8—H8C | 0.9700 |
C2—H2 | 0.9400 | C9—N1 | 1.503 (4) |
C3—C4 | 1.379 (4) | C9—H9A | 0.9700 |
C3—H3 | 0.9400 | C9—H9B | 0.9700 |
C4—C5 | 1.387 (4) | C9—H9C | 0.9700 |
Cl2—Cd1—Cl1 | 110.02 (3) | C5—C6—C1 | 121.1 (3) |
Cl2—Cd1—Cl3 | 126.73 (3) | C5—C6—H6 | 119.4 |
Cl1—Cd1—Cl3 | 123.24 (3) | C1—C6—H6 | 119.4 |
Cl2—Cd1—Cl3i | 94.80 (3) | N1—C7—H7A | 109.5 |
Cl1—Cd1—Cl3i | 96.23 (3) | N1—C7—H7B | 109.5 |
Cl3—Cd1—Cl3i | 81.49 (3) | H7A—C7—H7B | 109.5 |
Cl2—Cd1—Cl1ii | 92.47 (3) | N1—C7—H7C | 109.5 |
Cl1—Cd1—Cl1ii | 87.38 (3) | H7A—C7—H7C | 109.5 |
Cl3—Cd1—Cl1ii | 88.93 (3) | H7B—C7—H7C | 109.5 |
Cl3i—Cd1—Cl1ii | 170.23 (2) | N1—C8—H8A | 109.5 |
Cd1—Cl1—Cd1ii | 92.62 (3) | N1—C8—H8B | 109.5 |
Cd1—Cl3—Cd1i | 98.51 (3) | H8A—C8—H8B | 109.5 |
C1—S1—H1 | 138.0 | N1—C8—H8C | 109.5 |
C6—C1—C2 | 119.2 (3) | H8A—C8—H8C | 109.5 |
C6—C1—S1 | 118.4 (2) | H8B—C8—H8C | 109.5 |
C2—C1—S1 | 122.4 (2) | N1—C9—H9A | 109.5 |
C3—C2—C1 | 120.1 (3) | N1—C9—H9B | 109.5 |
C3—C2—H2 | 120.0 | H9A—C9—H9B | 109.5 |
C1—C2—H2 | 120.0 | N1—C9—H9C | 109.5 |
C4—C3—C2 | 119.8 (3) | H9A—C9—H9C | 109.5 |
C4—C3—H3 | 120.1 | H9B—C9—H9C | 109.5 |
C2—C3—H3 | 120.1 | C4—N1—C9 | 109.2 (2) |
C3—C4—C5 | 120.6 (3) | C4—N1—C8 | 112.8 (2) |
C3—C4—N1 | 121.5 (2) | C9—N1—C8 | 107.9 (2) |
C5—C4—N1 | 117.9 (2) | C4—N1—C7 | 109.9 (2) |
C6—C5—C4 | 119.2 (3) | C9—N1—C7 | 109.3 (2) |
C6—C5—H5 | 120.4 | C8—N1—C7 | 107.6 (2) |
C4—C5—H5 | 120.4 |
Symmetry codes: (i) −x+1, −y+2, −z+2; (ii) −x+2, −y+2, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
S1—H1···Cl1ii | 1.20 | 2.55 | 3.746 | 180 |
C8—H8B···Cl2iii | 0.97 | 2.72 | 3.640 (3) | 158 |
Symmetry codes: (ii) −x+2, −y+2, −z+2; (iii) x−1, −y+3/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | (C9H14NS)[CdCl3] |
Mr | 387.04 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 223 |
a, b, c (Å) | 7.3207 (15), 20.971 (4), 9.1613 (18) |
β (°) | 103.96 (3) |
V (Å3) | 1364.9 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 2.31 |
Crystal size (mm) | 0.50 × 0.30 × 0.20 |
Data collection | |
Diffractometer | Rigaku Mercury |
Absorption correction | Multi-scan (CrystalClear; Rigaku/MSC2001) |
Tmin, Tmax | 0.442, 0.635 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12984, 2491, 2424 |
Rint | 0.027 |
(sin θ/λ)max (Å−1) | 0.602 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.026, 0.069, 1.11 |
No. of reflections | 2491 |
No. of parameters | 137 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.56, −0.79 |
Computer programs: CrystalClear (Rigaku/MSC, 2001), CrystalStructure (Rigaku/MSC, 2004), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
S1—H1···Cl1i | 1.20 | 2.55 | 3.746 | 180.0 |
C8—H8B···Cl2ii | 0.97 | 2.72 | 3.640 (3) | 158.4 |
Symmetry codes: (i) −x+2, −y+2, −z+2; (ii) x−1, −y+3/2, z+1/2. |
Acknowledgements
This work was supported by the Natural Science Foundation of the Education Commission of Jiangsu Province of China (No.11KJB150001) and a start-up grant from Changshu Institute of Technology (No. ky2009069).
References
DePamphilis, B. V., Averill, B. A., Herskovitz, T., Que, L. & Holm, R. H. (1974). J. Am. Chem. Soc. 96, 4159–4167. CrossRef CAS PubMed Web of Science Google Scholar
Rigaku/MSC (2001). CrystalClear. Rigaku and Rigaku/MSC, The Woodlands, Texas, USA. Google Scholar
Rigaku/MSC (2004). CrystalStructure. Rigaku and Rigaku/MSC, The Woodlands, Texas, USA. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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