Abstract
The crystal structure of the title complex, [Zn(C7H6NO2S)2(H2O)]n, consists of extended layers parallel to (001) with 2-(pyridin-4-ylsulfanyl)acetate ligands bridging the ZnII atoms. The ZnII atom shows a distorted pentagonal–bipyramidal coordination environment. The ZnII and one O atom are situated on a crystallographic twofold rotation axis. In the crystal, intralayer O—H⋯O hydrogen-bond interactions help to consolidate the coordination layer.
Related literature
For metal complexes with polycarboxylate aromatic ligands and their applications, see: Yang et al. (2007 ▶, 2010 ▶); Yu et al. (2010 ▶). For solid-state structures of metal complexes with pyridine-4-sulfanyl-acetate ligands, see Wang et al. (2011 ▶); Kondo et al. (2002 ▶).
Experimental
Crystal data
[Zn(C7H6NO2S)2(H2O)]
M r = 419.76
Monoclinic,
a = 16.057 (3) Å
b = 6.3709 (10) Å
c = 15.630 (3) Å
β = 95.393 (4)°
V = 1591.8 (5) Å3
Z = 4
Mo Kα radiation
μ = 1.83 mm−1
T = 296 K
0.20 × 0.17 × 0.16 mm
Data collection
Bruker APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.711, T max = 0.758
3842 measured reflections
1403 independent reflections
1308 reflections with I > 2σ(I)
R int = 0.016
Refinement
R[F 2 > 2σ(F 2)] = 0.028
wR(F 2) = 0.072
S = 1.04
1403 reflections
110 parameters
H-atom parameters constrained
Δρmax = 0.57 e Å−3
Δρmin = −0.34 e Å−3
Data collection: APEX2 (Bruker, 2003 ▶); cell refinement: SAINT (Bruker, 2001 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶) and DIAMOND (Brandenburg & Berndt, 1999 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811024512/im2292sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811024512/im2292Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O3—H3′⋯O1i | 0.82 | 2.18 | 2.754 (3) | 128 |
Symmetry code: (i)
.
Acknowledgments
The authors gratefully acknowledge financial support from Tianjin Normal University.
supplementary crystallographic information
Comment
Recently, metal complexes constructed from aromatic polycarboxylate ligands and transition metal ions have received more and more interest due to their interesting architectures, amazing topologies and potentially technological applications in magnetism (Yang et al. 2010), luminesence (Yang et al. 2007) and gas storage (Yu et al. 2010). The anionic pyridine-4-sulfanyl-acetate ligand has three different potential binding sites upon coordination with metal ions and has exhibited various binding modes through the pyridyl N atom or carboxylate O donors. As a result, diverse complexes with discrete mononuclear (Wang et al. 2011), polymeric one-dimensional chains or two-dimensional layers (Kondo et al. 2002) have been obtained up to date. As a continuation of this research the crystal structure of a ZnII complex with pyridine-4-sulfanyl-acetate ligands, (I), is reported herein.
A cut-out of the polymeric structure of the title compound showing one ZnII atom in it's complete coordination environment is shown in Fig. 1. The ZnII atom exhibits a distorted pentagonal bipyramidal coordination environment involving two pyridyl N atoms from two separate pyridine-4-sulfanyl-acetate ligands in trans-position, four O atoms from a pair of chelating carboxylate groups of pyridine-4-sulfanyl-acetate ligands and one O atom of a terminal water molecule. Each anionic pyridine-4-sulfanyl-acetate ligand acts as a ditopic connector to bridge adjacent ZnII ions by a pyridyl N donor and a bidentate chelating carboxylate to generate a two-dimensional (4, 4) coordination layer with a Zn··· Zn distance of 6.3709 (10) Å. Additionally, O—H ···O hydrogen bonds between the coordinated water molecule and the deprotonated carboxylate (Table 1) help to consolidate the two-dimensional covalent layer (Fig. 2).
Experimental
A methanolic solution of pyridine-4-sulfanyl-acetic acid (50.6 mg, 0.2 mmol) was carefully layered onto a buffer layer of ethyl acetate (2.0 ml) in a straight glass tube below which an aqueous solution containing Zn(NO3)2.6 H2O (44.6 mg, 0.15 mmol) was placed. The test tube was left in air at room temperature. Colorless block-shaped crystals were harvested within three weeks. Yield: 40% based on ZnII salt. Anal. Calcd. for C14H14ZnN2O5S2: C, 40.06; H, 3.36; N, 6.67%. Found: C, 40.12; H, 3.26; N, 6.73%.
Refinement
H atoms could be located from difference Fourier maps, but were subsequently placed in calculated positions and treated as riding, with C–H = 0.93 (aromatic), 0.97 (methylene) and O–H = 0.82 Å. All H atoms were allocated displacement parameters related to those of their parent atoms [Uiso(H) = 1.2 Ueq(C, O)].
Figures
Fig. 1.
A portion of the two-dimensional structure of the title comlex. Displacement ellipsoids are drawn at the 30% probablity level. [Symmetry code: (A) 1 – x, y, 0.5 – z; (B) 1/2 + x, y, 0.5 – z; (C) 1/2 - x, 1/2 + y, 0.5 – z]
Fig. 2.
Part of the two-dimensional chain of (I), with hydrogen bonds shown as dashed lines.
Crystal data
| [Zn(C7H6NO2S)2(H2O)] | F(000) = 856 |
| Mr = 419.76 | Dx = 1.752 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 3018 reflections |
| a = 16.057 (3) Å | θ = 2.6–27.8° |
| b = 6.3709 (10) Å | µ = 1.83 mm−1 |
| c = 15.630 (3) Å | T = 296 K |
| β = 95.393 (4)° | Block, colourless |
| V = 1591.8 (5) Å3 | 0.20 × 0.17 × 0.16 mm |
| Z = 4 |
Data collection
| Bruker APEXII CCD area-detector diffractometer | 1403 independent reflections |
| Radiation source: fine-focus sealed tube | 1308 reflections with I > 2σ(I) |
| graphite | Rint = 0.016 |
| φ and ω scans | θmax = 25.0°, θmin = 2.6° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −18→8 |
| Tmin = 0.711, Tmax = 0.758 | k = −7→7 |
| 3842 measured reflections | l = −17→18 |
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)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.072 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0333P)2 + 2.8608P] where P = (Fo2 + 2Fc2)/3 |
| 1403 reflections | (Δ/σ)max < 0.001 |
| 110 parameters | Δρmax = 0.57 e Å−3 |
| 0 restraints | Δρmin = −0.34 e Å−3 |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| Zn1 | 0.5000 | 0.96825 (6) | 0.2500 | 0.03315 (15) | |
| S1 | 0.12091 (5) | 0.98792 (11) | 0.03086 (5) | 0.0547 (2) | |
| N1 | 0.37305 (12) | 0.9762 (3) | 0.19086 (13) | 0.0350 (4) | |
| O1 | 0.03140 (13) | 0.7681 (4) | 0.16602 (14) | 0.0766 (7) | |
| O2 | 0.05159 (15) | 0.4525 (4) | 0.12413 (14) | 0.0710 (7) | |
| O3 | 0.5000 | 0.6356 (4) | 0.2500 | 0.0511 (7) | |
| H3' | 0.4845 | 0.5927 | 0.2954 | 0.077* | |
| C1 | 0.21478 (15) | 0.9755 (4) | 0.09745 (16) | 0.0366 (5) | |
| C2 | 0.24687 (15) | 0.7966 (4) | 0.13868 (17) | 0.0429 (6) | |
| H2 | 0.2162 | 0.6726 | 0.1360 | 0.051* | |
| C3 | 0.32493 (15) | 0.8043 (4) | 0.18384 (17) | 0.0445 (6) | |
| H3 | 0.3454 | 0.6825 | 0.2111 | 0.053* | |
| C4 | 0.34017 (16) | 1.1504 (4) | 0.15408 (17) | 0.0432 (6) | |
| H4 | 0.3713 | 1.2735 | 0.1597 | 0.052* | |
| C5 | 0.26277 (16) | 1.1574 (4) | 0.10832 (18) | 0.0458 (6) | |
| H5 | 0.2425 | 1.2835 | 0.0846 | 0.055* | |
| C6 | 0.08449 (15) | 0.7230 (4) | 0.02936 (15) | 0.0384 (5) | |
| H6A | 0.0389 | 0.7099 | −0.0156 | 0.046* | |
| H6B | 0.1294 | 0.6325 | 0.0142 | 0.046* | |
| C7 | 0.05446 (15) | 0.6435 (5) | 0.11276 (16) | 0.0481 (7) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Zn1 | 0.0299 (2) | 0.0337 (2) | 0.0348 (2) | 0.000 | −0.00208 (15) | 0.000 |
| S1 | 0.0409 (4) | 0.0454 (4) | 0.0725 (5) | −0.0058 (3) | −0.0227 (3) | 0.0140 (3) |
| N1 | 0.0325 (10) | 0.0370 (11) | 0.0346 (10) | −0.0009 (8) | −0.0018 (8) | 0.0017 (8) |
| O1 | 0.0574 (13) | 0.121 (2) | 0.0539 (12) | −0.0035 (13) | 0.0178 (10) | −0.0277 (13) |
| O2 | 0.0762 (16) | 0.0738 (16) | 0.0580 (13) | −0.0330 (13) | −0.0205 (11) | 0.0193 (11) |
| O3 | 0.0532 (16) | 0.0350 (13) | 0.0644 (17) | 0.000 | 0.0022 (13) | 0.000 |
| C1 | 0.0305 (12) | 0.0402 (13) | 0.0383 (12) | −0.0005 (10) | −0.0013 (10) | 0.0013 (10) |
| C2 | 0.0331 (13) | 0.0370 (14) | 0.0574 (15) | −0.0068 (10) | −0.0020 (11) | 0.0082 (12) |
| C3 | 0.0362 (13) | 0.0403 (14) | 0.0554 (15) | −0.0010 (11) | −0.0040 (11) | 0.0138 (12) |
| C4 | 0.0401 (13) | 0.0344 (13) | 0.0529 (15) | −0.0055 (11) | −0.0067 (11) | 0.0005 (11) |
| C5 | 0.0428 (14) | 0.0321 (13) | 0.0598 (16) | 0.0004 (11) | −0.0101 (12) | 0.0059 (12) |
| C6 | 0.0336 (12) | 0.0466 (14) | 0.0341 (12) | −0.0047 (11) | −0.0023 (9) | −0.0056 (10) |
| C7 | 0.0284 (12) | 0.077 (2) | 0.0368 (13) | −0.0153 (13) | −0.0071 (10) | −0.0071 (14) |
Geometric parameters (Å, °)
| Zn1—O3 | 2.119 (3) | O2—Zn1iv | 2.208 (3) |
| Zn1—N1 | 2.158 (2) | O3—H3' | 0.8200 |
| Zn1—N1i | 2.158 (2) | C1—C2 | 1.384 (3) |
| Zn1—O2ii | 2.208 (3) | C1—C5 | 1.393 (3) |
| Zn1—O2iii | 2.208 (3) | C2—C3 | 1.380 (3) |
| Zn1—O1ii | 2.398 (3) | C2—H2 | 0.9300 |
| Zn1—O1iii | 2.398 (3) | C3—H3 | 0.9300 |
| S1—C1 | 1.751 (2) | C4—C5 | 1.375 (4) |
| S1—C6 | 1.786 (3) | C4—H4 | 0.9300 |
| N1—C4 | 1.336 (3) | C5—H5 | 0.9300 |
| N1—C3 | 1.338 (3) | C6—C7 | 1.519 (4) |
| O1—C7 | 1.232 (4) | C6—H6A | 0.9700 |
| O1—Zn1iv | 2.398 (3) | C6—H6B | 0.9700 |
| O2—C7 | 1.231 (4) | ||
| O3—Zn1—N1 | 91.34 (5) | C7—O2—Zn1iv | 96.1 (2) |
| O3—Zn1—N1i | 91.34 (5) | Zn1—O3—H3' | 109.5 |
| N1—Zn1—N1i | 177.32 (10) | C2—C1—C5 | 116.8 (2) |
| O3—Zn1—O2ii | 87.40 (6) | C2—C1—S1 | 125.16 (19) |
| N1—Zn1—O2ii | 87.95 (8) | C5—C1—S1 | 118.04 (19) |
| N1i—Zn1—O2ii | 92.17 (8) | C3—C2—C1 | 119.3 (2) |
| O3—Zn1—O2iii | 87.40 (6) | C3—C2—H2 | 120.4 |
| N1—Zn1—O2iii | 92.17 (8) | C1—C2—H2 | 120.4 |
| N1i—Zn1—O2iii | 87.96 (8) | N1—C3—C2 | 124.1 (2) |
| O2ii—Zn1—O2iii | 174.79 (13) | N1—C3—H3 | 118.0 |
| O3—Zn1—O1ii | 142.81 (5) | C2—C3—H3 | 118.0 |
| N1—Zn1—O1ii | 88.69 (8) | N1—C4—C5 | 123.5 (2) |
| N1i—Zn1—O1ii | 89.18 (7) | N1—C4—H4 | 118.2 |
| O2ii—Zn1—O1ii | 55.43 (8) | C5—C4—H4 | 118.2 |
| O2iii—Zn1—O1ii | 129.77 (8) | C4—C5—C1 | 119.9 (2) |
| O3—Zn1—O1iii | 142.81 (5) | C4—C5—H5 | 120.0 |
| N1—Zn1—O1iii | 89.18 (7) | C1—C5—H5 | 120.0 |
| N1i—Zn1—O1iii | 88.69 (8) | C7—C6—S1 | 115.73 (18) |
| O2ii—Zn1—O1iii | 129.78 (8) | C7—C6—H6A | 108.3 |
| O2iii—Zn1—O1iii | 55.43 (8) | S1—C6—H6A | 108.3 |
| O1ii—Zn1—O1iii | 74.38 (11) | C7—C6—H6B | 108.3 |
| C1—S1—C6 | 103.16 (11) | S1—C6—H6B | 108.3 |
| C4—N1—C3 | 116.3 (2) | H6A—C6—H6B | 107.4 |
| C4—N1—Zn1 | 121.53 (16) | O2—C7—O1 | 121.4 (3) |
| C3—N1—Zn1 | 122.05 (16) | O2—C7—C6 | 118.2 (3) |
| C7—O1—Zn1iv | 87.0 (2) | O1—C7—C6 | 120.3 (3) |
| O3—Zn1—N1—C4 | −163.91 (19) | C4—N1—C3—C2 | 2.8 (4) |
| N1i—Zn1—N1—C4 | 16.09 (19) | Zn1—N1—C3—C2 | −172.8 (2) |
| O2ii—Zn1—N1—C4 | 108.7 (2) | C1—C2—C3—N1 | 0.0 (4) |
| O2iii—Zn1—N1—C4 | −76.5 (2) | C3—N1—C4—C5 | −2.4 (4) |
| O1ii—Zn1—N1—C4 | 53.3 (2) | Zn1—N1—C4—C5 | 173.3 (2) |
| O1iii—Zn1—N1—C4 | −21.1 (2) | N1—C4—C5—C1 | −0.9 (4) |
| O3—Zn1—N1—C3 | 11.5 (2) | C2—C1—C5—C4 | 3.7 (4) |
| N1i—Zn1—N1—C3 | −168.5 (2) | S1—C1—C5—C4 | −174.5 (2) |
| O2ii—Zn1—N1—C3 | −75.8 (2) | C1—S1—C6—C7 | 70.1 (2) |
| O2iii—Zn1—N1—C3 | 99.0 (2) | Zn1iv—O2—C7—O1 | −0.1 (3) |
| O1ii—Zn1—N1—C3 | −131.3 (2) | Zn1iv—O2—C7—C6 | −177.97 (17) |
| O1iii—Zn1—N1—C3 | 154.3 (2) | Zn1iv—O1—C7—O2 | 0.1 (3) |
| C6—S1—C1—C2 | −1.8 (3) | Zn1iv—O1—C7—C6 | 177.9 (2) |
| C6—S1—C1—C5 | 176.2 (2) | S1—C6—C7—O2 | −159.5 (2) |
| C5—C1—C2—C3 | −3.2 (4) | S1—C6—C7—O1 | 22.6 (3) |
| S1—C1—C2—C3 | 174.8 (2) |
Symmetry codes: (i) −x+1, y, −z+1/2; (ii) −x+1/2, y+1/2, −z+1/2; (iii) x+1/2, y+1/2, z; (iv) x−1/2, y−1/2, z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O3—H3'···O1v | 0.82 | 2.18 | 2.754 (3) | 128 |
Symmetry codes: (v) −x+1/2, y−1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2292).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811024512/im2292sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811024512/im2292Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


