metal-organic compounds
Polymeric potassium triformatocobalt(II)
aInstitut für Anorganische Chemie, Christian-Albrechts-Universität Kiel, Max-Eyth-Strasse 2, 24118 Kiel, Germany, and bDepartement of Chemistry, Texas A&M University, College Station, Texas 77843, USA
*Correspondence e-mail: swoehlert@ac.uni-kiel.de
In the μ-formato-cobalt(II)potassium], [CoK(CHO2)3]n the Co2+ cations are coordinated by six O-bonded formate anions in an octahedral coordination mode and the K+ cations are eightfold coordinated by seven O-bonded formate anions within irregular polyhedra. The Co2+ cations are connected by bridging formate anions into a three-dimensional coordination network in which the K+ cations are embedded. The consits of one Co2+ cation located on a center of inversion, one K+ cation located on a twofold axis and two crystallographically independent formato anions, of which one is located on a twofold axis and the other occupies a general position.
of the title compound, poly[tri-Related literature
For background to this work see: Boeckmann et al. (2010); Wriedt & Näther (2010); Wriedt et al. (2009). For structures of bimetallic compounds based on potassium formate, see: Antsyshkina et al. (1983); Leontiev et al. (1988). For a description of the Cambridge Structural Database, see: Allen (2002).
Experimental
Crystal data
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Refinement
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Data collection: X-AREA (Stoe & Cie, 2008); cell 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, 1999); software used to prepare material for publication: XCIF in SHELXTL.
Supporting information
10.1107/S1600536811008737/kj2172sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811008737/kj2172Isup2.hkl
Potassium formate (KCHOO) and pyrazine were obtained from Alfa Aesar and cobalt(II) chloride was obtained from Acros Organics. All chemicals were used without further purification. 0.25 mmol (32.5 mg) CoCl2, 0.5 mmol (42.1 mg) KCHOO and 0.5 mmol (40 mg) pyrazine were reacted with 1 ml acetonitrile in a closed test-tube at 120°C for three days. On cooling block-shaped single crystals of the title compound were obtained in a mixture with an unknown phase. It must be noted, that the reaction under similar conditions without pyrazine does not lead to the formation of the title compound.
The H atoms were positioned with idealized geometry and were refined isotropic with Uiso(H) = 1.2Ueq(C) and C—H distances of 0.93 Å using a riding model.
Data collection: X-AREA (Stoe & Cie, 2008); cell
X-AREA (Stoe & Cie, 2008); data reduction: X-AREA (Stoe & Cie, 2008); 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, 1999); software used to prepare material for publication: XCIF in SHELXTL (Sheldrick, 2008).[CoK(CHO2)3] | F(000) = 460 |
Mr = 233.08 | Dx = 2.353 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 6120 reflections |
a = 10.7244 (8) Å | θ = 3.0–29.2° |
b = 8.9653 (6) Å | µ = 3.22 mm−1 |
c = 6.8742 (5) Å | T = 293 K |
β = 95.539 (6)° | Block, light blue |
V = 657.85 (8) Å3 | 0.16 × 0.09 × 0.06 mm |
Z = 4 |
Stoe IPDS-2 diffractometer | 892 independent reflections |
Radiation source: fine-focus sealed tube | 853 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.031 |
ω scans | θmax = 29.2°, θmin = 3.0° |
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) | h = −14→14 |
Tmin = 0.711, Tmax = 0.817 | k = −12→12 |
6120 measured reflections | l = −9→9 |
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)] = 0.020 | H-atom parameters constrained |
wR(F2) = 0.046 | w = 1/[σ2(Fo2) + (0.0276P)2 + 0.1263P] where P = (Fo2 + 2Fc2)/3 |
S = 1.15 | (Δ/σ)max < 0.001 |
892 reflections | Δρmax = 0.25 e Å−3 |
54 parameters | Δρmin = −0.57 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: 0.0126 (12) |
[CoK(CHO2)3] | V = 657.85 (8) Å3 |
Mr = 233.08 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 10.7244 (8) Å | µ = 3.22 mm−1 |
b = 8.9653 (6) Å | T = 293 K |
c = 6.8742 (5) Å | 0.16 × 0.09 × 0.06 mm |
β = 95.539 (6)° |
Stoe IPDS-2 diffractometer | 892 independent reflections |
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) | 853 reflections with I > 2σ(I) |
Tmin = 0.711, Tmax = 0.817 | Rint = 0.031 |
6120 measured reflections |
R[F2 > 2σ(F2)] = 0.020 | 0 restraints |
wR(F2) = 0.046 | H-atom parameters constrained |
S = 1.15 | Δρmax = 0.25 e Å−3 |
892 reflections | Δρmin = −0.57 e Å−3 |
54 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
K1 | 0.0000 | 0.10357 (5) | 0.2500 | 0.02582 (12) | |
Co1 | 0.2500 | 0.2500 | 0.0000 | 0.01561 (10) | |
O1 | 0.16793 (10) | 0.33291 (11) | 0.24238 (15) | 0.0274 (2) | |
O2 | 0.25445 (9) | 0.54804 (11) | 0.34563 (15) | 0.0271 (2) | |
C1 | 0.18397 (13) | 0.44031 (15) | 0.3568 (2) | 0.0244 (3) | |
H1 | 0.1371 | 0.4392 | 0.4638 | 0.029* | |
O11 | 0.43048 (9) | 0.31029 (12) | 0.12114 (14) | 0.0260 (2) | |
C11 | 0.5000 | 0.2478 (2) | 0.2500 | 0.0271 (4) | |
H11 | 0.5000 | 0.1441 | 0.2500 | 0.033* |
U11 | U22 | U33 | U12 | U13 | U23 | |
K1 | 0.0278 (2) | 0.01932 (19) | 0.0318 (2) | 0.000 | 0.01004 (16) | 0.000 |
Co1 | 0.01611 (14) | 0.01374 (14) | 0.01648 (14) | −0.00041 (8) | −0.00102 (8) | 0.00122 (8) |
O1 | 0.0332 (5) | 0.0223 (5) | 0.0277 (5) | −0.0087 (4) | 0.0091 (4) | −0.0093 (4) |
O2 | 0.0300 (5) | 0.0204 (4) | 0.0318 (5) | −0.0063 (4) | 0.0076 (4) | −0.0089 (4) |
C1 | 0.0312 (6) | 0.0213 (6) | 0.0215 (6) | −0.0042 (5) | 0.0069 (5) | −0.0037 (5) |
O11 | 0.0215 (4) | 0.0303 (5) | 0.0245 (5) | −0.0036 (4) | −0.0063 (4) | 0.0033 (4) |
C11 | 0.0270 (9) | 0.0217 (9) | 0.0310 (10) | 0.000 | −0.0057 (8) | 0.000 |
K1—O1 | 2.7371 (10) | Co1—O11iv | 2.1026 (9) |
K1—O2i | 2.8193 (10) | O1—C1 | 1.2448 (17) |
K1—O11ii | 2.8335 (10) | O2—C1 | 1.2335 (17) |
K1—O11i | 2.8507 (11) | C1—H1 | 0.9300 |
K1—C11i | 3.189 (2) | O11—C11 | 1.2356 (13) |
Co1—O1 | 2.0943 (10) | C11—H11 | 0.9300 |
Co1—O2iii | 2.1015 (10) | ||
O1—K1—O1v | 82.62 (5) | O1—Co1—O11iv | 87.99 (4) |
O1—K1—O2i | 140.19 (3) | O1iv—Co1—O11iv | 92.01 (4) |
O1v—K1—O2i | 59.81 (3) | O2iii—Co1—O11iv | 94.96 (4) |
O2i—K1—O2vi | 159.66 (4) | O2vi—Co1—O11iv | 85.04 (4) |
O1—K1—O11ii | 92.48 (3) | O11iv—Co1—O11 | 180.00 (6) |
O1v—K1—O11ii | 63.08 (3) | C1—O1—Co1 | 137.25 (9) |
O2i—K1—O11ii | 60.35 (3) | C1—O1—K1 | 128.31 (9) |
O2vi—K1—O11ii | 126.22 (3) | Co1—O1—K1 | 94.38 (3) |
O11ii—K1—O11iv | 148.37 (5) | C1—O2—Co1vii | 126.81 (9) |
O1—K1—O11i | 147.11 (3) | C1—O2—K1viii | 138.13 (9) |
O1v—K1—O11i | 123.09 (3) | Co1vii—O2—K1viii | 91.88 (3) |
O2i—K1—O11i | 71.79 (3) | O2—C1—O1 | 127.90 (13) |
O2vi—K1—O11i | 89.25 (3) | O2—C1—H1 | 116.0 |
O11ii—K1—O11i | 116.58 (3) | O1—C1—H1 | 116.0 |
O11iv—K1—O11i | 93.17 (3) | C11—O11—Co1 | 129.50 (9) |
O11i—K1—O11vi | 45.45 (4) | C11—O11—K1iv | 125.17 (6) |
O1—K1—C11i | 138.69 (2) | Co1—O11—K1iv | 91.47 (3) |
O2i—K1—C11i | 79.83 (2) | C11—O11—K1viii | 94.23 (9) |
O11ii—K1—C11i | 105.81 (2) | Co1—O11—K1viii | 124.29 (4) |
O11i—K1—C11i | 22.727 (19) | K1iv—O11—K1viii | 86.83 (3) |
O1—Co1—O1iv | 180.0 | O11ix—C11—O11 | 126.09 (18) |
O1—Co1—O2iii | 97.34 (4) | O11ix—C11—K1viii | 63.04 (9) |
O1iv—Co1—O2iii | 82.66 (4) | O11—C11—H11 | 117.0 |
O2iii—Co1—O2vi | 180.00 (3) | K1viii—C11—H11 | 180.0 |
Symmetry codes: (i) x−1/2, y−1/2, z; (ii) x−1/2, −y+1/2, z+1/2; (iii) x, −y+1, z−1/2; (iv) −x+1/2, −y+1/2, −z; (v) −x, y, −z+1/2; (vi) −x+1/2, y−1/2, −z+1/2; (vii) −x+1/2, y+1/2, −z+1/2; (viii) x+1/2, y+1/2, z; (ix) −x+1, y, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [CoK(CHO2)3] |
Mr | 233.08 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 293 |
a, b, c (Å) | 10.7244 (8), 8.9653 (6), 6.8742 (5) |
β (°) | 95.539 (6) |
V (Å3) | 657.85 (8) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.22 |
Crystal size (mm) | 0.16 × 0.09 × 0.06 |
Data collection | |
Diffractometer | Stoe IPDS2 diffractometer |
Absorption correction | Numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) |
Tmin, Tmax | 0.711, 0.817 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6120, 892, 853 |
Rint | 0.031 |
(sin θ/λ)max (Å−1) | 0.686 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.020, 0.046, 1.15 |
No. of reflections | 892 |
No. of parameters | 54 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.25, −0.57 |
Computer programs: X-AREA (Stoe & Cie, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), XP in SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 1999), XCIF in SHELXTL (Sheldrick, 2008).
K1—O1 | 2.7371 (10) | Co1—O1 | 2.0943 (10) |
K1—O2i | 2.8193 (10) | Co1—O2ii | 2.1015 (10) |
K1—O11i | 2.8507 (11) | Co1—O11iii | 2.1026 (9) |
Symmetry codes: (i) x−1/2, y−1/2, z; (ii) x, −y+1, z−1/2; (iii) −x+1/2, −y+1/2, −z. |
Acknowledgements
We gratefully acknowledge financial support by the DFG (project number NA 720/3-1) and the State of Schleswig-Holstein. We thank Professor Dr Bensch for access to his experimental facility.
References
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In our current investigation on the synthesis, structures and properties of new coordination polymers based on paramagnetic transition metal, small-sized anions and N-donor ligands, we have shown that thermal decomposition reactions are an elegante route for the discovery and preparation of new ligand-deficient coordination polymers (Boeckmann et al., 2010; Wriedt & Näther, 2010; Wriedt et al., 2009). Within this project we tried to prepare new ligand-rich precursor compounds based on cobalt formate and pyrazine as coligand. However, reaction of cobalt(II) chloride, potassium formate and pyrazine in acteonitrile unexpectedly resulted in single crystals of the title compound.
In the crystal structure of the title compound, each cobalt(II) cation is coordinated by six bridging formato anions with Co—OCHO distances between 2.0943 (10) Å and 2.1026 (9) Å. The CoO6 octahedron is slightly distorted with angles ranging from 82.66 (4) ° to 97.34 (4) ° and 180° (Fig. 1 and Tab. 1). The K+ cations are coordinated by eight oxygen atoms belonging to seven formato anions within irregular polyhedra. The K—O distances ranges from 2.7371 (10) Å to 2.8507 (11) Å and the O—K—O angles are between 59.81 (3) ° and 147.11 (3) °. The cobalt cations are connected via µ-1,3 bridging formato anions into a three dimensional coordination network (Fig. 2). Within this networks cavities are formed in which the K+ cations are embedded (Fig 3). The shortest Co···Co distances amount to 5.6487 (3) Å and the shortest K···K distances are 3.9067 (4) Å).
According to a search in the CCDC database (ConQuest Ver.1.12.2010) (Allen, 2002) mixed cobalt and potassium formates are unkown but bimetallic compounds based on potassium formate are known with different metals (Antsyshkina et al., 1983 and Leontiev et al., 1988.