Literature DB >> 21582384

catena-Poly[[bis-(4-methyl-benzene-thiol-ato)cadium(II)]-μ-1,3-di-4-pyridylpropane].

Yan Zhang1, Yan Zhou, Lei Han.   

Abstract

In the title compound, [Cd(C(7)H(7)S)(2)(C(13)H(14)N(2))](n), the unique Cd(II) ion, located on a twofold rotation axis, is coordinated by two S atoms and two N atoms in a slightly distorted tetra-hedral environment. Symmetry-related Cd(II) ions are linked via bridging 1,3-di-4-pyridylpropane ligands, forming a zig-zag chain-structure parallel to [001]. In the crystal structure, there are weak intra-chain π-π stacking inter-actions between benzene rings, with a centroid-centroid distance of 3.825 (7) Å, and pairs of chains are inter-digitated with respect to the 4-methyl-benzene-thiol-ate groups.

Entities:  

Year:  2009        PMID: 21582384      PMCID: PMC2968951          DOI: 10.1107/S1600536809010447

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


Related literature

For background information on coordination polymers, see: James (2003 ▶); Wang et al. (2005 ▶); Cheng et al. (2007 ▶); Han & Zhou (2008 ▶). For information on the 1,3-bis­(4-pyrid­yl)propane ligand, see: Han et al. (2007 ▶); Carlucci et al. (2002 ▶). For the synthetic procedure, see: Dance et al. (1987 ▶).

Experimental

Crystal data

[Cd(C7H7S)2(C13H14N2)] M = 557.03 Monoclinic, a = 11.922 (2) Å b = 16.792 (3) Å c = 12.862 (3) Å β = 91.06 (3)° V = 2574.5 (9) Å3 Z = 4 Mo Kα radiation μ = 1.03 mm−1 T = 298 K 0.45 × 0.25 × 0.18 mm

Data collection

Rigaku R-AXIS RAPID diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.655, T max = 0.837 12609 measured reflections 2948 independent reflections 2587 reflections with I > 2σ(I) R int = 0.046

Refinement

R[F 2 > 2σ(F 2)] = 0.036 wR(F 2) = 0.090 S = 1.09 2948 reflections 150 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.53 e Å−3 Δρmin = −0.90 e Å−3 Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-AUTO; 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 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809010447/lh2791sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809010447/lh2791Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Cd(C7H7S)2(C13H14N2)]F(000) = 1136
Mr = 557.03Dx = 1.437 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 1774 reflections
a = 11.922 (2) Åθ = 3.2–27.5°
b = 16.792 (3) ŵ = 1.03 mm1
c = 12.862 (3) ÅT = 298 K
β = 91.06 (3)°Block, colorless
V = 2574.5 (9) Å30.45 × 0.25 × 0.18 mm
Z = 4
Rigaku R-AXIS RAPID diffractometer2948 independent reflections
Radiation source: fine-focus sealed tube2587 reflections with I > 2σ(I)
graphiteRint = 0.046
Detector resolution: 0 pixels mm-1θmax = 27.5°, θmin = 3.2°
ω scansh = −15→15
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)k = −21→21
Tmin = 0.655, Tmax = 0.837l = −16→14
12609 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.036Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090H atoms treated by a mixture of independent and constrained refinement
S = 1.09w = 1/[σ2(Fo2) + (0.0411P)2 + 2.0003P] where P = (Fo2 + 2Fc2)/3
2948 reflections(Δ/σ)max = 0.001
150 parametersΔρmax = 0.53 e Å3
0 restraintsΔρmin = −0.90 e Å3
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
Cd10.00000.295756 (15)0.25000.04791 (11)
S10.18408 (7)0.35512 (5)0.22501 (8)0.0677 (2)
N1−0.0143 (2)0.20104 (12)0.11914 (17)0.0485 (5)
C10.00000.1037 (2)−0.25000.0464 (8)
H10.065 (2)0.1374 (16)−0.243 (2)0.050 (8)*
C2−0.0111 (3)0.05267 (16)−0.1528 (2)0.0579 (7)
H2A−0.07990.0219−0.15790.070*
H2B0.05120.0156−0.14850.070*
C3−0.0126 (3)0.10235 (14)−0.05565 (19)0.0486 (6)
C4−0.1082 (3)0.14257 (19)−0.0269 (2)0.0615 (7)
H4A−0.17410.1373−0.06620.074*
C5−0.1060 (3)0.19035 (19)0.0598 (3)0.0607 (8)
H5A−0.17160.21650.07790.073*
C60.0779 (3)0.16210 (17)0.0914 (2)0.0545 (7)
H6A0.14250.16820.13220.065*
C70.0822 (3)0.11328 (16)0.0054 (2)0.0551 (7)
H7A0.14880.0879−0.01130.066*
C80.1615 (2)0.45217 (16)0.2756 (2)0.0511 (6)
C90.1277 (3)0.46512 (18)0.3764 (2)0.0589 (7)
H9A0.11520.42180.41970.071*
C100.1120 (3)0.54131 (18)0.4140 (3)0.0621 (7)
H10A0.08980.54820.48230.075*
C110.1812 (3)0.51806 (19)0.2143 (2)0.0643 (8)
H11A0.20560.51140.14670.077*
C120.1646 (3)0.59429 (19)0.2530 (3)0.0686 (9)
H12A0.17820.63790.21050.082*
C130.1286 (3)0.60699 (18)0.3527 (3)0.0626 (8)
C140.1075 (4)0.6900 (2)0.3939 (4)0.0969 (14)
H14A0.08360.68670.46460.145*
H14B0.05020.71520.35220.145*
H14C0.17540.72050.39090.145*
U11U22U33U12U13U23
Cd10.05340 (18)0.04305 (16)0.04712 (17)0.000−0.00332 (12)0.000
S10.0523 (4)0.0585 (4)0.0927 (6)−0.0030 (3)0.0129 (4)−0.0238 (4)
N10.0573 (14)0.0480 (12)0.0402 (11)−0.0044 (10)−0.0019 (10)0.0000 (9)
C10.059 (2)0.0403 (18)0.0402 (18)0.000−0.0002 (17)0.000
C20.089 (2)0.0427 (13)0.0418 (13)−0.0028 (14)−0.0010 (14)0.0013 (11)
C30.0688 (17)0.0394 (12)0.0375 (12)−0.0064 (11)0.0005 (12)0.0058 (9)
C40.0559 (17)0.077 (2)0.0511 (16)−0.0052 (14)−0.0066 (14)−0.0122 (14)
C50.0511 (16)0.076 (2)0.0546 (17)−0.0011 (14)0.0006 (14)−0.0139 (14)
C60.0584 (16)0.0524 (15)0.0521 (15)0.0013 (13)−0.0132 (13)−0.0013 (12)
C70.0625 (17)0.0493 (14)0.0533 (16)0.0088 (13)−0.0032 (14)0.0000 (12)
C80.0407 (13)0.0525 (14)0.0600 (16)−0.0043 (11)−0.0002 (12)−0.0093 (12)
C90.0627 (18)0.0524 (16)0.0621 (17)−0.0018 (13)0.0115 (15)0.0004 (13)
C100.0635 (18)0.0632 (18)0.0601 (17)−0.0012 (14)0.0091 (15)−0.0109 (14)
C110.069 (2)0.0673 (19)0.0569 (17)−0.0094 (15)0.0043 (15)−0.0023 (14)
C120.075 (2)0.0543 (17)0.076 (2)−0.0070 (15)0.0042 (18)0.0067 (15)
C130.0561 (17)0.0512 (16)0.080 (2)−0.0032 (13)0.0031 (16)−0.0113 (14)
C140.098 (3)0.058 (2)0.136 (4)0.0021 (19)0.023 (3)−0.020 (2)
Cd1—N12.320 (2)C6—C71.379 (4)
Cd1—N1i2.320 (2)C6—H6A0.9300
Cd1—S12.4370 (9)C7—H7A0.9300
Cd1—S1i2.4370 (9)C8—C111.381 (4)
S1—C81.777 (3)C8—C91.383 (4)
N1—C61.333 (4)C9—C101.381 (4)
N1—C51.334 (4)C9—H9A0.9300
C1—C2ii1.523 (3)C10—C131.372 (4)
C1—C21.523 (3)C10—H10A0.9300
C1—H10.97 (3)C11—C121.389 (4)
C2—C31.503 (4)C11—H11A0.9300
C2—H2A0.9700C12—C131.376 (5)
C2—H2B0.9700C12—H12A0.9300
C3—C71.377 (4)C13—C141.513 (4)
C3—C41.381 (4)C14—H14A0.9600
C4—C51.373 (4)C14—H14B0.9600
C4—H4A0.9300C14—H14C0.9600
C5—H5A0.9300
N1—Cd1—N1i93.43 (11)N1—C6—H6A118.3
N1—Cd1—S1103.83 (7)C7—C6—H6A118.3
N1i—Cd1—S1108.77 (7)C3—C7—C6119.6 (3)
N1—Cd1—S1i108.77 (7)C3—C7—H7A120.2
N1i—Cd1—S1i103.83 (7)C6—C7—H7A120.2
S1—Cd1—S1i131.71 (4)C11—C8—C9117.7 (3)
C8—S1—Cd1100.62 (9)C11—C8—S1119.9 (2)
C6—N1—C5116.9 (2)C9—C8—S1122.4 (2)
C6—N1—Cd1118.72 (19)C10—C9—C8121.1 (3)
C5—N1—Cd1123.8 (2)C10—C9—H9A119.4
C2ii—C1—C2111.6 (3)C8—C9—H9A119.4
C2ii—C1—H1109.0 (17)C13—C10—C9121.5 (3)
C2—C1—H1109.5 (16)C13—C10—H10A119.3
C3—C2—C1111.9 (2)C9—C10—H10A119.3
C3—C2—H2A109.2C8—C11—C12120.5 (3)
C1—C2—H2A109.2C8—C11—H11A119.8
C3—C2—H2B109.2C12—C11—H11A119.8
C1—C2—H2B109.2C13—C12—C11121.7 (3)
H2A—C2—H2B107.9C13—C12—H12A119.1
C7—C3—C4117.1 (2)C11—C12—H12A119.1
C7—C3—C2121.7 (3)C10—C13—C12117.5 (3)
C4—C3—C2121.1 (3)C10—C13—C14120.9 (3)
C5—C4—C3120.0 (3)C12—C13—C14121.7 (3)
C5—C4—H4A120.0C13—C14—H14A109.5
C3—C4—H4A120.0C13—C14—H14B109.5
N1—C5—C4123.1 (3)H14A—C14—H14B109.5
N1—C5—H5A118.5C13—C14—H14C109.5
C4—C5—H5A118.5H14A—C14—H14C109.5
N1—C6—C7123.3 (3)H14B—C14—H14C109.5
Cd1—N12.320 (2)
Cd1—S12.4370 (9)
N1—Cd1—N1i93.43 (11)
N1—Cd1—S1103.83 (7)
N1i—Cd1—S1108.77 (7)
S1—Cd1—S1i131.71 (4)

Symmetry code: (i) .

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