Literature DB >> 21753993

catena-Poly[[bis-(pyridine-κN)cadmium]-di-μ(2)-thio-cyanato-κN:S;κS:N].

Jan Boeckmann1, Inke Jess, Christian Näther.   

Abstract

The asymmetric unit of the title compound, [Cd(NCS)(2)(C(5)H(5)N)(2)](n), consists of two crystallographically independent Cd(II) cations, four thio-cyanato anions and four pyridine ligands. The Cd(II) atoms are each coordinated by four N atoms from two pyridine ligands and two thio-cyanato anions, each in a mutually cis orientation, and by two S atoms from two adjacent thio-cyanato anions within a slightly distorted octa-hedral coordination environment. The Cd(II) atoms are μ-1,3-bridged via the thio-cyanato anions into polymeric chains parallel to [001]. The Cd(II)Cd(II) intra-chain separations range between 5.9688 (6) and 6.0195 (6) Å, whereas the shortest Cd(II)Cd(II) inter-chain separations are 7.8272 (7) and 8.6312 (6) Å.

Entities:  

Year:  2011        PMID: 21753993      PMCID: PMC3099960          DOI: 10.1107/S1600536811009871

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For related structures see: Boeckmann & Näther (2010 ▶); Chen et al. (2005 ▶ ); Foner et al. (1975 ▶); Marsh et al. (2002 ▶); Porai-Koshits & Tishchenko (1960 ▶); Reller & Oswald (1986 ▶); Taniguchi et al. (1987 ▶); Zhu et al. (2008 ▶).

Experimental

Crystal data

[Cd(NCS)2(C5H5N)2] M = 386.76 Triclinic, a = 7.8272 (4) Å b = 8.6242 (4) Å c = 23.705 (1) Å α = 84.890 (3)° β = 89.520 (4)° γ = 63.070 (3)° V = 1420.06 (11) Å3 Z = 4 Mo Kα radiation μ = 1.82 mm−1 T = 293 K 0.15 × 0.11 × 0.07 mm

Data collection

Stoe IPDS-2 diffractometer Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) ▶ T min = 0.779, T max = 0.874 21468 measured reflections 5998 independent reflections 4613 reflections with I > 2σ(I) R int = 0.071

Refinement

R[F 2 > 2σ(F 2)] = 0.052 wR(F 2) = 0.083 S = 1.17 5998 reflections 343 parameters H-atom parameters constrained Δρmax = 0.60 e Å−3 Δρmin = −0.75 e Å−3 Data collection: X-AREA (Stoe & Cie, 2008) ▶; cell refinement: X-AREA ▶; data reduction: X-AREA ▶; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP in SHELXTL (Sheldrick, 2008 ▶) and DIAMOND (Brandenburg, 2011 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811009871/bt5493sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009871/bt5493Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Cd(NCS)2(C5H5N)2]Z = 4
Mr = 386.76F(000) = 760
Triclinic, P1Dx = 1.809 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.8272 (4) ÅCell parameters from 21468 reflections
b = 8.6242 (4) Åθ = 1.7–26.8°
c = 23.705 (1) ŵ = 1.82 mm1
α = 84.890 (3)°T = 293 K
β = 89.520 (4)°Needle, colourless
γ = 63.070 (3)°0.15 × 0.11 × 0.07 mm
V = 1420.06 (11) Å3
Stoe IPDS-2 diffractometer5998 independent reflections
Radiation source: fine-focus sealed tube4613 reflections with I > 2σ(I)
graphiteRint = 0.071
ω scansθmax = 26.8°, θmin = 1.7°
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008)h = −9→9
Tmin = 0.779, Tmax = 0.874k = −10→10
21468 measured reflectionsl = −29→29
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.083H-atom parameters constrained
S = 1.17w = 1/[σ2(Fo2) + (0.0176P)2 + 0.9412P] where P = (Fo2 + 2Fc2)/3
5998 reflections(Δ/σ)max < 0.001
343 parametersΔρmax = 0.60 e Å3
0 restraintsΔρmin = −0.75 e Å3
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.
xyzUiso*/Ueq
Cd10.55905 (5)0.97050 (4)0.375033 (15)0.03786 (11)
Cd20.44978 (6)0.99144 (5)0.125075 (15)0.03970 (11)
S10.8352 (2)0.93622 (19)0.45431 (6)0.0470 (3)
S30.2004 (2)0.9601 (2)0.20176 (6)0.0542 (4)
S20.8141 (2)0.9986 (2)0.29930 (6)0.0479 (3)
S40.1714 (2)1.0203 (2)0.04890 (7)0.0542 (4)
N10.6266 (7)1.0543 (6)0.5514 (2)0.0483 (11)
N30.3481 (7)0.9946 (6)0.3040 (2)0.0501 (12)
N20.6584 (7)0.9716 (6)0.1968 (2)0.0512 (12)
N110.4113 (6)1.2780 (5)0.37531 (19)0.0424 (10)
N210.7184 (7)0.6634 (5)0.3729 (2)0.0452 (11)
N310.2874 (7)1.2985 (6)0.1265 (2)0.0494 (12)
N410.5944 (7)0.6842 (6)0.1253 (2)0.0511 (12)
C10.7117 (7)1.0078 (6)0.5111 (2)0.0371 (11)
C30.2885 (7)0.9809 (6)0.2618 (2)0.0380 (11)
C20.7225 (7)0.9828 (6)0.2393 (2)0.0382 (11)
C40.2834 (8)1.0002 (6)−0.0110 (2)0.0386 (11)
C110.3248 (9)1.3573 (7)0.4204 (3)0.0548 (15)
H110.31991.28900.45240.066*
C130.2505 (10)1.6376 (7)0.3758 (3)0.0653 (18)
H130.19911.75800.37640.078*
C140.3353 (10)1.5601 (8)0.3289 (3)0.0614 (17)
H140.33961.62720.29640.074*
C150.4150 (9)1.3809 (7)0.3299 (3)0.0538 (14)
H150.47381.32900.29760.065*
C210.8169 (9)0.5864 (7)0.3292 (3)0.0543 (15)
H210.81850.65660.29720.065*
C220.9167 (10)0.4081 (8)0.3286 (3)0.0624 (17)
H220.98400.35970.29690.075*
C230.9157 (9)0.3043 (8)0.3745 (3)0.0623 (17)
H230.98420.18350.37510.075*
C240.8136 (11)0.3782 (8)0.4199 (3)0.0664 (18)
H240.80910.30920.45180.080*
C250.7165 (10)0.5588 (7)0.4175 (3)0.0561 (15)
H250.64660.60940.44860.067*
C310.2529 (10)1.3725 (8)0.1749 (3)0.0601 (16)
H310.30171.30170.20860.072*
C330.0767 (10)1.6554 (8)0.1281 (4)0.0691 (19)
H330.00631.77570.12870.083*
C340.1113 (11)1.5804 (8)0.0782 (3)0.075 (2)
H340.06471.64880.04390.090*
C350.2159 (10)1.4025 (8)0.0794 (3)0.0636 (17)
H350.23771.35250.04530.076*
C410.6102 (10)0.6087 (8)0.0777 (3)0.0619 (17)
H410.57150.67880.04350.074*
C420.6816 (11)0.4304 (9)0.0770 (3)0.074 (2)
H420.68850.38190.04300.088*
C430.7418 (10)0.3267 (8)0.1266 (4)0.0678 (19)
H430.79210.20610.12700.081*
C440.7273 (12)0.4020 (9)0.1756 (4)0.075 (2)
H440.76530.33400.21020.090*
C450.6555 (10)0.5800 (8)0.1730 (3)0.0624 (17)
H450.64940.63030.20660.075*
C320.1479 (12)1.5493 (8)0.1769 (4)0.074 (2)
H320.12541.59650.21160.088*
C120.2420 (10)1.5359 (8)0.4219 (3)0.0677 (19)
H120.18101.58630.45410.081*
N40.3589 (8)0.9870 (7)−0.0535 (2)0.0531 (12)
U11U22U33U12U13U23
Cd10.0446 (2)0.03687 (19)0.0315 (2)−0.01765 (16)0.00348 (18)−0.00516 (15)
Cd20.0456 (3)0.0426 (2)0.0309 (2)−0.01997 (17)0.00095 (18)−0.00324 (16)
S10.0417 (8)0.0603 (8)0.0370 (8)−0.0204 (6)0.0045 (6)−0.0103 (6)
S30.0585 (10)0.0841 (10)0.0350 (8)−0.0451 (8)0.0040 (7)−0.0085 (7)
S20.0482 (8)0.0707 (9)0.0340 (8)−0.0345 (7)0.0035 (6)−0.0085 (6)
S40.0474 (9)0.0867 (10)0.0348 (8)−0.0355 (8)0.0032 (7)−0.0087 (7)
N10.050 (3)0.062 (3)0.039 (3)−0.030 (2)0.005 (2)−0.007 (2)
N30.053 (3)0.068 (3)0.036 (3)−0.033 (2)0.001 (2)−0.007 (2)
N20.051 (3)0.069 (3)0.037 (3)−0.031 (2)−0.003 (2)−0.004 (2)
N110.042 (3)0.043 (2)0.039 (3)−0.0169 (19)−0.001 (2)−0.0019 (18)
N210.052 (3)0.040 (2)0.043 (3)−0.020 (2)0.000 (2)−0.0059 (19)
N310.052 (3)0.044 (2)0.050 (3)−0.020 (2)0.001 (2)−0.003 (2)
N410.050 (3)0.043 (2)0.056 (3)−0.018 (2)0.003 (3)−0.002 (2)
C10.038 (3)0.033 (2)0.040 (3)−0.018 (2)−0.003 (2)0.003 (2)
C30.037 (3)0.037 (2)0.037 (3)−0.014 (2)0.006 (2)−0.002 (2)
C20.035 (3)0.037 (2)0.042 (3)−0.016 (2)0.009 (2)−0.001 (2)
C40.040 (3)0.039 (2)0.039 (3)−0.019 (2)−0.008 (2)−0.001 (2)
C110.060 (4)0.049 (3)0.047 (3)−0.017 (3)0.007 (3)−0.004 (2)
C130.064 (4)0.034 (3)0.086 (5)−0.014 (3)−0.007 (4)0.001 (3)
C140.069 (4)0.048 (3)0.066 (4)−0.028 (3)−0.006 (3)0.014 (3)
C150.057 (4)0.052 (3)0.048 (4)−0.021 (3)0.004 (3)0.002 (2)
C210.063 (4)0.049 (3)0.050 (4)−0.024 (3)0.007 (3)−0.009 (3)
C220.067 (4)0.051 (3)0.069 (5)−0.023 (3)0.011 (3)−0.023 (3)
C230.055 (4)0.044 (3)0.082 (5)−0.016 (3)−0.006 (3)−0.013 (3)
C240.089 (5)0.045 (3)0.059 (4)−0.027 (3)−0.006 (4)0.005 (3)
C250.072 (4)0.050 (3)0.043 (3)−0.024 (3)0.002 (3)−0.005 (2)
C310.071 (4)0.051 (3)0.054 (4)−0.024 (3)−0.005 (3)−0.006 (3)
C330.066 (4)0.046 (3)0.093 (6)−0.023 (3)0.001 (4)−0.008 (4)
C340.081 (5)0.052 (4)0.073 (5)−0.018 (3)−0.009 (4)0.015 (3)
C350.074 (4)0.055 (4)0.052 (4)−0.021 (3)−0.001 (3)−0.001 (3)
C410.075 (4)0.048 (3)0.052 (4)−0.018 (3)0.004 (3)−0.007 (3)
C420.080 (5)0.063 (4)0.072 (5)−0.025 (4)0.010 (4)−0.025 (4)
C430.062 (4)0.048 (3)0.090 (6)−0.024 (3)0.005 (4)0.002 (3)
C440.091 (6)0.058 (4)0.068 (5)−0.029 (4)−0.006 (4)0.012 (3)
C450.074 (5)0.052 (3)0.057 (4)−0.026 (3)−0.008 (3)0.001 (3)
C320.093 (6)0.050 (4)0.074 (5)−0.027 (4)0.006 (4)−0.019 (3)
C120.076 (5)0.046 (3)0.064 (5)−0.011 (3)0.004 (4)−0.011 (3)
N40.054 (3)0.076 (3)0.035 (3)−0.035 (2)0.007 (2)−0.008 (2)
Cd1—N32.298 (5)C13—H130.9300
Cd1—N1i2.317 (5)C14—C151.378 (8)
Cd1—N112.365 (4)C14—H140.9300
Cd1—N212.367 (4)C15—H150.9300
Cd1—S22.7508 (15)C21—C221.375 (8)
Cd1—S12.7715 (16)C21—H210.9300
Cd2—N4ii2.303 (5)C22—C231.349 (10)
Cd2—N22.309 (5)C22—H220.9300
Cd2—N412.363 (4)C23—C241.361 (9)
Cd2—N312.366 (4)C23—H230.9300
Cd2—S32.7416 (16)C24—C251.385 (8)
Cd2—S42.7503 (17)C24—H240.9300
S1—C11.647 (5)C25—H250.9300
S3—C31.646 (6)C31—C321.371 (9)
S2—C21.642 (6)C31—H310.9300
S4—C41.643 (6)C33—C321.360 (11)
N1—C11.156 (6)C33—C341.365 (11)
N1—Cd1i2.317 (5)C33—H330.9300
N3—C31.144 (7)C34—C351.371 (9)
N2—C21.159 (7)C34—H340.9300
N11—C111.329 (7)C35—H350.9300
N11—C151.342 (7)C41—C421.379 (8)
N21—C211.326 (7)C41—H410.9300
N21—C251.332 (7)C42—C431.358 (11)
N31—C351.318 (8)C42—H420.9300
N31—C311.329 (8)C43—C441.360 (11)
N41—C451.324 (8)C43—H430.9300
N41—C411.331 (8)C44—C451.370 (9)
C4—N41.153 (7)C44—H440.9300
C11—C121.378 (8)C45—H450.9300
C11—H110.9300C32—H320.9300
C13—C141.357 (10)C12—H120.9300
C13—C121.360 (10)N4—Cd2ii2.303 (5)
N3—Cd1—N1i95.37 (17)C14—C13—H13120.6
N3—Cd1—N1190.26 (17)C12—C13—H13120.6
N1i—Cd1—N1191.19 (16)C13—C14—C15119.2 (6)
N3—Cd1—N2190.51 (17)C13—C14—H14120.4
N1i—Cd1—N2191.07 (16)C15—C14—H14120.4
N11—Cd1—N21177.54 (15)N11—C15—C14122.9 (6)
N3—Cd1—S292.60 (12)N11—C15—H15118.6
N1i—Cd1—S2172.02 (13)C14—C15—H15118.6
N11—Cd1—S288.36 (11)N21—C21—C22123.3 (6)
N21—Cd1—S289.27 (12)N21—C21—H21118.3
N3—Cd1—S1175.47 (12)C22—C21—H21118.3
N1i—Cd1—S189.01 (13)C23—C22—C21119.1 (6)
N11—Cd1—S190.83 (12)C23—C22—H22120.4
N21—Cd1—S188.23 (12)C21—C22—H22120.4
S2—Cd1—S183.03 (4)C22—C23—C24119.3 (6)
N4ii—Cd2—N294.30 (17)C22—C23—H23120.3
N4ii—Cd2—N4191.31 (18)C24—C23—H23120.3
N2—Cd2—N4191.26 (18)C23—C24—C25118.4 (6)
N4ii—Cd2—N3191.68 (17)C23—C24—H24120.8
N2—Cd2—N3190.34 (17)C25—C24—H24120.8
N41—Cd2—N31176.50 (16)N21—C25—C24123.2 (6)
N4ii—Cd2—S3174.04 (13)N21—C25—H25118.4
N2—Cd2—S391.52 (13)C24—C25—H25118.4
N41—Cd2—S387.27 (13)N31—C31—C32122.4 (7)
N31—Cd2—S389.57 (12)N31—C31—H31118.8
N4ii—Cd2—S492.06 (14)C32—C31—H31118.8
N2—Cd2—S4173.51 (13)C32—C33—C34118.1 (6)
N41—Cd2—S489.88 (14)C32—C33—H33120.9
N31—Cd2—S488.19 (13)C34—C33—H33120.9
S3—Cd2—S482.16 (5)C33—C34—C35118.8 (7)
C1—S1—Cd1103.53 (19)C33—C34—H34120.6
C3—S3—Cd2101.98 (18)C35—C34—H34120.6
C2—S2—Cd1101.04 (17)N31—C35—C34123.6 (6)
C4—S4—Cd2101.36 (19)N31—C35—H35118.2
C1—N1—Cd1i152.4 (4)C34—C35—H35118.2
C3—N3—Cd1161.5 (4)N41—C41—C42122.6 (6)
C2—N2—Cd2163.6 (4)N41—C41—H41118.7
C11—N11—C15116.7 (5)C42—C41—H41118.7
C11—N11—Cd1122.2 (4)C43—C42—C41119.1 (7)
C15—N11—Cd1121.1 (4)C43—C42—H42120.5
C21—N21—C25116.7 (5)C41—C42—H42120.5
C21—N21—Cd1123.0 (4)C42—C43—C44119.0 (6)
C25—N21—Cd1120.3 (4)C42—C43—H43120.5
C35—N31—C31117.2 (5)C44—C43—H43120.5
C35—N31—Cd2121.2 (4)C43—C44—C45118.7 (7)
C31—N31—Cd2121.4 (4)C43—C44—H44120.7
C45—N41—C41117.1 (5)C45—C44—H44120.7
C45—N41—Cd2121.6 (4)N41—C45—C44123.6 (7)
C41—N41—Cd2121.3 (4)N41—C45—H45118.2
N1—C1—S1178.5 (4)C44—C45—H45118.2
N3—C3—S3179.1 (5)C33—C32—C31119.8 (7)
N2—C2—S2179.7 (5)C33—C32—H32120.1
N4—C4—S4178.8 (5)C31—C32—H32120.1
N11—C11—C12123.2 (6)C13—C12—C11119.2 (6)
N11—C11—H11118.4C13—C12—H12120.4
C12—C11—H11118.4C11—C12—H12120.4
C14—C13—C12118.8 (5)C4—N4—Cd2ii162.1 (4)
Table 1

Selected bond angles (°)

N1—C1—S1178.5 (4)
N3—C3—S3179.1 (5)
N2—C2—S2179.7 (5)
N4—C4—S4178.8 (5)
  3 in total

1.  Some 60 new space-group corrections.

Authors:  Richard E Marsh; Moshe Kapon; Shengzhi Hu; Frank H Herbstein
Journal:  Acta Crystallogr B       Date:  2001-01-24

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

3.  Solid-state transformation of [Co(NCS)2(pyridine)4] into [Co(NCS)2(pyridine)2]n: from Curie-Weiss paramagnetism to single chain magnetic behaviour.

Authors:  Jan Boeckmann; Christian Näther
Journal:  Dalton Trans       Date:  2010-10-14       Impact factor: 4.390

  3 in total

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