Abstract
In the title compound, [Ni(CHO2)2(C4H4N2)(H2O)], the nickel(II) cations are coordinated by three O-bonded-formato anions, two N-bonded-pyrazine ligands and one water molecule in an octahedral coordination mode. The nickel(II) cations are connected by μ-1,3-bridging formato anions and N,N′-bridging pyrazine ligands into a three dimensional coordination network. The asymmetric unit consists of one nickel(II) cation, one water molecule and two crystallographically independent formato anions in general positions as well as two crystallographically independent pyrazine ligands, which are located on centers of inversion.
Related literature
For background of this work, see: Boeckmann & Näther (2010 ▶), Wriedt et al. (2009) ▶; Boeckmann et al. (2010 ▶). For a related structure, see: Manson et al. (2003 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶).
Experimental
Crystal data
[Ni(CHO2)2(C4H4N2)(H2O)]
M r = 246.85
Monoclinic,
a = 7.8169 (4) Å
b = 7.0077 (3) Å
c = 15.6586 (7) Å
β = 98.971 (4)°
V = 847.26 (7) Å3
Z = 4
Mo Kα radiation
μ = 2.29 mm−1
T = 293 K
0.19 × 0.15 × 0.12 mm
Data collection
Stoe IPDS-2 diffractometer
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe, 2008 ▶) T min = 0.658, T max = 0.770
15596 measured reflections
2291 independent reflections
2091 reflections with I > 2σ(I)
R int = 0.036
Refinement
R[F 2 > 2σ(F 2)] = 0.025
wR(F 2) = 0.059
S = 1.10
2291 reflections
128 parameters
H-atom parameters constrained
Δρmax = 0.47 e Å−3
Δρmin = −0.30 e Å−3
Data collection: X-AREA (Stoe, 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 ▶); software used to prepare material for publication: XP in SHELXTL and DIAMOND (Brandenburg, 2011 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811011913/bt5501sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011913/bt5501Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Acknowledgments
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 facilities.
supplementary crystallographic information
Comment
In our recent work 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 new ligand-deficient coordination polymers based on transition metal thiocyanates and selenocyanates can be prepared by thermal decomposition reactions (Wriedt, Jess & Näther, 2009 and Boeckmann & Näther, 2010). Later we have shown that also metal formates can be prepared by this route (Boeckmann, Wriedt & Näther, 2010). Within this project we tried to prepare new ligand-rich precursor compounds based on nickel(II) formate and pyrazine which resulted in the formation of the title compound that were identified by single crystal X-ray diffraction.
In the crystal structure of the title compound, each nickel(II) cation is coordinated by three bridging formato anions, two bridging pyrazine ligands and one water molecule (Fig. 1). The NiO4N2 octahedron is slightly distorted with Ni—OCHO distances between 2.0378 (11) Å and 2.0643 (12) Å and one Ni—OH2 distance of 2.0420 (11) Å as well as two long Ni—N distances of 2.1066 (13) Å and 2.1171 (12) Å. The angles around the metal atoms range from 84.14 (5)° to 95.94 (5)° and from 173.18 (5)° to 179.19 (5)°. The nickel(II) cations are connected via µ-1,3 bridging formato anions into two dimensional Ni(O2CHO)2 layers that are further linked by the pyrazine ligands into a 3D coordination network (Fig. 2). The Ni—Ni distances between next neighboured Ni atoms ranges from 6.9770 (4) Å to 7.0689 (4) Å.
It must be noted that according to a search in the CCDC database (ConQuest Ver.1.12.) (Allen, 2002) compounds based on nickel(II) formate and pyrazine are unknown but with copper(II) formate one strcuture is reported (Manson et al., 2003).
Experimental
Nickel formate dihydrate [Ni(CHO2)2.H2O] and pyrazine were obtained from Alfa Aesar. All chemicals were used without further purification. 0.25 mmol (46 mg) Ni(CHO2)2.H2O and 0.5 mmol (40 mg) pyrazine were reacted in 2 ml water. Light blue block-shaped single crystals of the title compound were obtained after a few days at room temperature.
Refinement
The C-H 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. The O-H H atoms were located in difference map, their bond lengths were set to 0.82 Å and afterwards they were refined isotropic with Uiso(H) = 1.5Ueq(O) using a riding model.
Figures
Fig. 1.
: Crystal structure of the title compound with labelling and displacement ellipsoids drawn at the 50 % probability level. Symmetry codes: i = -x+1, y+1/2 i = -x+1,y+1/2,-z+3/2; ii = -x+1,-y,-z+1; iii = -x,-y+1,-z+1.
Fig. 2.
: Crystal structure of the title compound with view along the crystallographic a-axis.
Crystal data
| [Ni(CHO2)2(C4H4N2)(H2O)] | F(000) = 504 |
| Mr = 246.85 | Dx = 1.935 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 15596 reflections |
| a = 7.8169 (4) Å | θ = 2.6–29.3° |
| b = 7.0077 (3) Å | µ = 2.29 mm−1 |
| c = 15.6586 (7) Å | T = 293 K |
| β = 98.971 (4)° | Block, light blue |
| V = 847.26 (7) Å3 | 0.19 × 0.15 × 0.12 mm |
| Z = 4 |
Data collection
| Stoe IPDS-2 diffractometer | 2291 independent reflections |
| Radiation source: fine-focus sealed tube | 2091 reflections with I > 2σ(I) |
| graphite | Rint = 0.036 |
| ω scan | θmax = 29.3°, θmin = 2.6° |
| Absorption correction: numerical (X-SHAPE and X-RED32; Stoe, 2008) | h = −10→10 |
| Tmin = 0.658, Tmax = 0.770 | k = −9→9 |
| 15596 measured reflections | l = −21→21 |
Refinement
| 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)] = 0.025 | H-atom parameters constrained |
| wR(F2) = 0.059 | w = 1/[σ2(Fo2) + (0.025P)2 + 0.4622P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.10 | (Δ/σ)max = 0.001 |
| 2291 reflections | Δρmax = 0.47 e Å−3 |
| 128 parameters | Δρmin = −0.30 e Å−3 |
| 0 restraints | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0158 (13) |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| Ni1 | 0.30005 (2) | 0.25657 (3) | 0.649349 (11) | 0.01731 (8) | |
| N1 | 0.41659 (17) | 0.10169 (18) | 0.55756 (8) | 0.0205 (2) | |
| C1 | 0.3337 (2) | 0.0453 (2) | 0.48084 (10) | 0.0250 (3) | |
| H1 | 0.2169 | 0.0747 | 0.4654 | 0.030* | |
| C2 | 0.5831 (2) | 0.0558 (2) | 0.57642 (10) | 0.0257 (3) | |
| H2 | 0.6452 | 0.0925 | 0.6294 | 0.031* | |
| N11 | 0.12229 (17) | 0.39364 (18) | 0.55394 (8) | 0.0209 (2) | |
| C11 | −0.0463 (2) | 0.3831 (2) | 0.55924 (11) | 0.0241 (3) | |
| H11 | −0.0827 | 0.3027 | 0.6001 | 0.029* | |
| C12 | 0.1684 (2) | 0.5112 (2) | 0.49450 (10) | 0.0234 (3) | |
| H12 | 0.2847 | 0.5224 | 0.4891 | 0.028* | |
| O21 | 0.11734 (15) | 0.04433 (16) | 0.65066 (8) | 0.0275 (3) | |
| O22 | 0.0548 (2) | −0.25397 (17) | 0.67969 (12) | 0.0434 (4) | |
| C21 | 0.1545 (2) | −0.1280 (2) | 0.66185 (12) | 0.0279 (3) | |
| H21 | 0.2693 | −0.1604 | 0.6602 | 0.042* | |
| O31 | 0.46637 (15) | 0.11818 (18) | 0.74213 (8) | 0.0282 (3) | |
| O32 | 0.51992 (15) | −0.03704 (17) | 0.86756 (7) | 0.0260 (2) | |
| C31 | 0.4364 (2) | 0.0746 (2) | 0.81445 (11) | 0.0258 (3) | |
| H31 | 0.3479 | 0.1347 | 0.8375 | 0.039* | |
| O41 | 0.18980 (15) | 0.40396 (16) | 0.73925 (7) | 0.0241 (2) | |
| H1O | 0.1126 | 0.3547 | 0.7617 | 0.036* | |
| H2O | 0.1500 | 0.5093 | 0.7246 | 0.036* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Ni1 | 0.01857 (11) | 0.01683 (11) | 0.01653 (11) | 0.00177 (7) | 0.00272 (7) | 0.00092 (7) |
| N1 | 0.0220 (6) | 0.0203 (6) | 0.0198 (6) | 0.0012 (5) | 0.0049 (5) | −0.0023 (5) |
| C1 | 0.0200 (7) | 0.0306 (8) | 0.0238 (7) | 0.0045 (6) | 0.0020 (6) | −0.0043 (6) |
| C2 | 0.0230 (7) | 0.0321 (8) | 0.0212 (7) | 0.0019 (6) | 0.0007 (6) | −0.0070 (6) |
| N11 | 0.0214 (6) | 0.0199 (6) | 0.0206 (6) | 0.0019 (5) | 0.0007 (5) | 0.0018 (5) |
| C11 | 0.0233 (7) | 0.0245 (7) | 0.0243 (7) | 0.0000 (6) | 0.0030 (6) | 0.0059 (6) |
| C12 | 0.0194 (7) | 0.0258 (7) | 0.0248 (7) | 0.0013 (6) | 0.0029 (6) | 0.0035 (6) |
| O21 | 0.0261 (6) | 0.0184 (5) | 0.0390 (7) | −0.0001 (4) | 0.0077 (5) | 0.0045 (5) |
| O22 | 0.0477 (8) | 0.0184 (6) | 0.0720 (11) | 0.0009 (5) | 0.0340 (8) | 0.0041 (6) |
| C21 | 0.0283 (8) | 0.0206 (7) | 0.0372 (9) | 0.0027 (6) | 0.0128 (7) | 0.0011 (6) |
| O31 | 0.0273 (6) | 0.0356 (6) | 0.0218 (5) | 0.0097 (5) | 0.0043 (5) | 0.0080 (5) |
| O32 | 0.0296 (6) | 0.0276 (6) | 0.0208 (5) | 0.0089 (5) | 0.0039 (4) | 0.0040 (4) |
| C31 | 0.0286 (8) | 0.0266 (8) | 0.0227 (7) | 0.0087 (6) | 0.0054 (6) | 0.0020 (6) |
| O41 | 0.0264 (6) | 0.0208 (5) | 0.0271 (6) | 0.0015 (4) | 0.0101 (4) | −0.0002 (4) |
Geometric parameters (Å, °)
| Ni1—O31 | 2.0378 (11) | C11—C12iii | 1.385 (2) |
| Ni1—O41 | 2.0420 (11) | C11—H11 | 0.9300 |
| Ni1—O32i | 2.0636 (11) | C12—C11iii | 1.385 (2) |
| Ni1—O21 | 2.0643 (12) | C12—H12 | 0.9300 |
| Ni1—N11 | 2.1066 (13) | O21—C21 | 1.2479 (19) |
| Ni1—N1 | 2.1171 (12) | O22—C21 | 1.238 (2) |
| N1—C2 | 1.328 (2) | C21—H21 | 0.9300 |
| N1—C1 | 1.333 (2) | O31—C31 | 1.230 (2) |
| C1—C2ii | 1.382 (2) | O32—C31 | 1.2492 (19) |
| C1—H1 | 0.9300 | O32—Ni1iv | 2.0636 (11) |
| C2—C1ii | 1.382 (2) | C31—H31 | 0.9299 |
| C2—H2 | 0.9300 | O41—H1O | 0.8200 |
| N11—C12 | 1.334 (2) | O41—H2O | 0.8200 |
| N11—C11 | 1.335 (2) | ||
| O31—Ni1—O41 | 92.30 (5) | C1ii—C2—H2 | 119.2 |
| O31—Ni1—O32i | 93.04 (5) | C12—N11—C11 | 117.00 (13) |
| O41—Ni1—O32i | 95.94 (5) | C12—N11—Ni1 | 123.80 (11) |
| O31—Ni1—O21 | 90.89 (5) | C11—N11—Ni1 | 118.62 (10) |
| O41—Ni1—O21 | 89.46 (5) | N11—C11—C12iii | 121.75 (14) |
| O32i—Ni1—O21 | 173.18 (5) | N11—C11—H11 | 119.1 |
| O31—Ni1—N11 | 178.28 (5) | C12iii—C11—H11 | 119.1 |
| O41—Ni1—N11 | 87.46 (5) | N11—C12—C11iii | 121.25 (14) |
| O32i—Ni1—N11 | 88.68 (5) | N11—C12—H12 | 119.4 |
| O21—Ni1—N11 | 87.40 (5) | C11iii—C12—H12 | 119.4 |
| O31—Ni1—N1 | 86.89 (5) | C21—O21—Ni1 | 123.54 (11) |
| O41—Ni1—N1 | 179.19 (5) | O22—C21—O21 | 125.53 (16) |
| O32i—Ni1—N1 | 84.14 (5) | O22—C21—H21 | 118.4 |
| O21—Ni1—N1 | 90.52 (5) | O21—C21—H21 | 115.9 |
| N11—Ni1—N1 | 93.35 (5) | C31—O31—Ni1 | 125.64 (11) |
| C2—N1—C1 | 116.76 (13) | C31—O32—Ni1iv | 130.50 (10) |
| C2—N1—Ni1 | 118.93 (11) | O31—C31—O32 | 127.86 (15) |
| C1—N1—Ni1 | 124.31 (10) | O31—C31—H31 | 120.4 |
| N1—C1—C2ii | 121.65 (14) | O32—C31—H31 | 111.6 |
| N1—C1—H1 | 119.2 | Ni1—O41—H1O | 120.0 |
| C2ii—C1—H1 | 119.2 | Ni1—O41—H2O | 116.4 |
| N1—C2—C1ii | 121.59 (15) | H1O—O41—H2O | 103.1 |
| N1—C2—H2 | 119.2 |
Symmetry codes: (i) −x+1, y+1/2, −z+3/2; (ii) −x+1, −y, −z+1; (iii) −x, −y+1, −z+1; (iv) −x+1, y−1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5501).
References
- Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
- Boeckmann, J. & Näther, C. (2010). Dalton Trans. 39, 1119-1126. [DOI] [PubMed]
- Boeckmann, J., Wriedt, M. & Näther, C. (2010). Eur. J. Inorg. Chem. pp. 1820-1828.
- Brandenburg, K. (2011). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Manson, J. L., Lecher, J. G., Gu, J., Geiser, U., Schlueter, J. A., Henning, R., Wang, X., Schultz, A. J., Koo, H.-J. & Whangbo, M.-H. (2003). Dalton Trans. pp. 2905–2911.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Stoe (2008). X-AREA, X-RED32 and X-SHAPE Stoe & Cie, Darmstadt, Germany.
- Wriedt, M., Jess, I. & Näther, C. (2009). Eur. J. Inorg. Chem. pp. 1406–1413.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811011913/bt5501sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011913/bt5501Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


