
Acta Cryst. (2008). E64, m57 [ doi:10.1107/S1600536807062794 ]
2-4,4'-bipyridine-
2N:N'-
-p-phenylenedioxydiacetato-
2O:O']The title coordination polymer, [Ni(C10H8O6)(C10H8N2)(H2O)2]n, was obtained by the hydrothermal reaction of nickel(II) sulfate, benzene-1,4-dioxydiacetic acid (p-phenylenedioxydiacetic acid) and 4,4'-bipyridine (4,4'-bpy) in alkaline aqueous solution. Each NiII atom is coordinated by two O atoms from two benzene-1,4-dioxydiacetate ligands, two N atoms from two 4,4'-bpy ligands and two water molecules, and displays a distorted octahedral geometry. The NiII atom and benzene-1,4-dioxydiacetate and 4,4'-bpy moieties lie on inversion centres. The benzene-1,4-dioxydiacetate ligands bridge the NiII atoms to form infinite zigzag chains, which are further interconnected by 4,4'-bpy ligands to form a grid-like layer parallel to the (0
1) plane. Moreover, there are O-H
O hydrogen-bonding interactions within the grid-like layer between the coordinated water molecules and the carboxylate O atoms.
A mixture of NiSO4 (0.5 mmol), benzene-1,4-dioxydiacetic acid (0.5 mmol), 4,4'-bipyridine (0.5 mmol), NaOH (1 mmol) and H2O (12 ml) was placed in a 23 ml Teflon reactor, which was heated at 433 K for three days and then cooled to room temperature at a rate of 5 K h-1. Single crystals were obtained after washing with water and drying in air.
All H atoms attached to C atoms were fixed geometrically and treated as riding with C—H = 0.93 Å (aromatic) or 0.97 Å (methylene and Uiso(H) = 1.2Ueq(C). H atoms of water molecule were located in difference Fourier maps and included in the subsequent refinement using restraints (O—H = 0.82 (1) Å and H···H = 1.34 (2) Å) with Uiso(H) = 1.5Ueq(O). In the last stage of refinement, they were treated as riding on their parent O atoms.
Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPIII within PLATON (Spek, 2003) and CAMERON (Watkin et al., 1993); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).
| [Ni(C10H8O6)(C10H8N2)(H2O)2] | Z = 1 |
| Mr = 475.09 | F000 = 246 |
| Triclinic, P1 | Dx = 1.677 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation λ = 0.71073 Å |
| a = 5.7541 (1) Å | Cell parameters from 1800 reflections |
| b = 8.1704 (1) Å | θ = 1.4–28.0º |
| c = 10.6437 (2) Å | µ = 1.09 mm−1 |
| α = 106.157 (1)º | T = 293 (2) K |
| β = 96.818 (1)º | Block, green |
| γ = 97.341 (1)º | 0.26 × 0.23 × 0.19 mm |
| V = 470.40 (1) Å3 |
| Bruker APEXII area-detector diffractometer | 1952 independent reflections |
| Radiation source: fine-focus sealed tube | 1769 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.026 |
| T = 293(2) K | θmax = 26.5º |
| φ and ω scans | θmin = 2.0º |
| Absorption correction: multi-scan (SADABS; Bruker, 2004) | h = −7→7 |
| Tmin = 0.765, Tmax = 0.820 | k = −8→10 |
| 6907 measured reflections | l = −13→13 |
| 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)] = 0.034 | H-atom parameters constrained |
| wR(F2) = 0.086 | w = 1/[σ2(Fo2) + (0.0346P)2 + 0.4701P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.08 | (Δ/σ)max < 0.001 |
| 1952 reflections | Δρmax = 0.32 e Å−3 |
| 142 parameters | Δρmin = −0.38 e Å−3 |
| Primary atom site location: structure-invariant direct methods | Extinction correction: none |
| [Ni(C10H8O6)(C10H8N2)(H2O)2] | γ = 97.341 (1)º |
| Mr = 475.09 | V = 470.40 (1) Å3 |
| Triclinic, P1 | Z = 1 |
| a = 5.7541 (1) Å | Mo Kα |
| b = 8.1704 (1) Å | µ = 1.09 mm−1 |
| c = 10.6437 (2) Å | T = 293 (2) K |
| α = 106.157 (1)º | 0.26 × 0.23 × 0.19 mm |
| β = 96.818 (1)º |
| Bruker APEXII area-detector diffractometer | 1952 independent reflections |
| Absorption correction: multi-scan (SADABS; Bruker, 2004) | 1769 reflections with I > 2σ(I) |
| Tmin = 0.765, Tmax = 0.820 | Rint = 0.026 |
| 6907 measured reflections |
| R[F2 > 2σ(F2)] = 0.034 | 142 parameters |
| wR(F2) = 0.086 | H-atom parameters constrained |
| S = 1.08 | Δρmax = 0.32 e Å−3 |
| 1952 reflections | Δρmin = −0.38 e Å−3 |
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. |
| x | y | z | Uiso*/Ueq | ||
| C1 | 0.1666 (4) | 0.7074 (3) | 0.7930 (2) | 0.0318 (6) | |
| H1 | 0.2876 | 0.7217 | 0.8633 | 0.038* | |
| C2 | 0.1734 (4) | 0.5879 (3) | 0.6736 (2) | 0.0314 (6) | |
| H2 | 0.2965 | 0.5240 | 0.6655 | 0.038* | |
| C3 | −0.0019 (4) | 0.5624 (3) | 0.5655 (2) | 0.0201 (5) | |
| C4 | −0.1819 (4) | 0.6612 (3) | 0.5876 (2) | 0.0262 (5) | |
| H4 | −0.3058 | 0.6487 | 0.5192 | 0.031* | |
| C5 | −0.1772 (4) | 0.7772 (3) | 0.7101 (2) | 0.0264 (5) | |
| H5 | −0.3005 | 0.8405 | 0.7218 | 0.032* | |
| C6 | 0.1281 (4) | 0.7277 (3) | 1.1257 (2) | 0.0253 (5) | |
| C7 | 0.3161 (5) | 0.6440 (3) | 1.1868 (3) | 0.0327 (6) | |
| H7A | 0.2457 | 0.5854 | 1.2444 | 0.039* | |
| H7B | 0.3633 | 0.5572 | 1.1163 | 0.039* | |
| C8 | 0.5001 (4) | 0.8782 (3) | 1.3782 (2) | 0.0273 (5) | |
| C9 | 0.6973 (4) | 1.0042 (3) | 1.4391 (3) | 0.0315 (6) | |
| H9 | 0.8307 | 1.0079 | 1.3978 | 0.038* | |
| C10 | 0.6996 (4) | 1.1242 (3) | 1.5598 (3) | 0.0315 (6) | |
| H10 | 0.8344 | 1.2067 | 1.5997 | 0.038* | |
| N1 | −0.0044 (3) | 0.8038 (2) | 0.81332 (18) | 0.0227 (4) | |
| Ni1 | 0.0000 | 1.0000 | 1.0000 | 0.02315 (14) | |
| O1 | 0.2019 (3) | 0.8651 (2) | 1.09891 (15) | 0.0251 (4) | |
| O2 | −0.0799 (3) | 0.6527 (2) | 1.1047 (2) | 0.0427 (5) | |
| O3 | 0.5228 (3) | 0.7621 (2) | 1.26119 (17) | 0.0332 (4) | |
| O1W | 0.3239 (3) | 1.1425 (2) | 0.98244 (16) | 0.0289 (4) | |
| H1W | 0.2733 | 1.2183 | 0.9556 | 0.043* | |
| H2W | 0.4307 | 1.1122 | 0.9424 | 0.043* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0272 (12) | 0.0431 (15) | 0.0187 (12) | 0.0114 (11) | −0.0037 (9) | −0.0003 (11) |
| C2 | 0.0272 (12) | 0.0421 (15) | 0.0207 (12) | 0.0160 (11) | 0.0006 (9) | −0.0009 (11) |
| C3 | 0.0237 (11) | 0.0198 (11) | 0.0155 (11) | 0.0018 (9) | 0.0034 (9) | 0.0040 (9) |
| C4 | 0.0279 (12) | 0.0282 (12) | 0.0186 (11) | 0.0084 (9) | −0.0033 (9) | 0.0019 (9) |
| C5 | 0.0281 (12) | 0.0257 (12) | 0.0233 (12) | 0.0104 (9) | 0.0010 (9) | 0.0025 (10) |
| C6 | 0.0307 (12) | 0.0254 (12) | 0.0201 (11) | 0.0100 (10) | 0.0063 (9) | 0.0040 (9) |
| C7 | 0.0391 (14) | 0.0283 (13) | 0.0327 (14) | 0.0099 (11) | 0.0040 (11) | 0.0111 (11) |
| C8 | 0.0275 (11) | 0.0332 (13) | 0.0256 (12) | 0.0098 (10) | 0.0017 (9) | 0.0145 (10) |
| C9 | 0.0228 (11) | 0.0448 (15) | 0.0318 (14) | 0.0072 (10) | 0.0079 (10) | 0.0175 (12) |
| C10 | 0.0246 (11) | 0.0379 (14) | 0.0326 (14) | 0.0008 (10) | 0.0026 (10) | 0.0142 (11) |
| N1 | 0.0247 (9) | 0.0231 (10) | 0.0175 (9) | 0.0040 (8) | 0.0035 (8) | 0.0014 (8) |
| Ni1 | 0.0242 (2) | 0.0247 (2) | 0.0187 (2) | 0.00564 (16) | 0.00278 (16) | 0.00319 (17) |
| O1 | 0.0280 (8) | 0.0250 (9) | 0.0221 (8) | 0.0067 (7) | 0.0013 (7) | 0.0070 (7) |
| O2 | 0.0309 (10) | 0.0373 (11) | 0.0653 (14) | 0.0067 (8) | 0.0079 (9) | 0.0234 (10) |
| O3 | 0.0301 (9) | 0.0409 (11) | 0.0281 (9) | 0.0112 (8) | 0.0036 (7) | 0.0077 (8) |
| O1W | 0.0231 (8) | 0.0335 (9) | 0.0317 (9) | 0.0058 (7) | 0.0060 (7) | 0.0110 (8) |
| C1—N1 | 1.338 (3) | C7—H7B | 0.9700 |
| C1—C2 | 1.379 (3) | C8—O3 | 1.372 (3) |
| C1—H1 | 0.9300 | C8—C9 | 1.387 (3) |
| C2—C3 | 1.386 (3) | C8—C10ii | 1.392 (3) |
| C2—H2 | 0.9300 | C9—C10 | 1.380 (4) |
| C3—C4 | 1.395 (3) | C9—H9 | 0.9300 |
| C3—C3i | 1.486 (4) | C10—C8ii | 1.392 (3) |
| C4—C5 | 1.377 (3) | C10—H10 | 0.9300 |
| C4—H4 | 0.9300 | N1—Ni1 | 2.1735 (18) |
| C5—N1 | 1.340 (3) | Ni1—O1 | 2.0869 (15) |
| C5—H5 | 0.9300 | Ni1—O1iii | 2.0869 (15) |
| C6—O2 | 1.237 (3) | Ni1—O1Wiii | 2.1245 (16) |
| C6—O1 | 1.268 (3) | Ni1—O1W | 2.1245 (16) |
| C6—C7 | 1.526 (3) | Ni1—N1iii | 2.1735 (18) |
| C7—O3 | 1.425 (3) | O1W—H1W | 0.8206 |
| C7—H7A | 0.9700 | O1W—H2W | 0.8144 |
| N1—C1—C2 | 123.6 (2) | C10—C9—H9 | 119.3 |
| N1—C1—H1 | 118.2 | C8—C9—H9 | 119.3 |
| C2—C1—H1 | 118.2 | C9—C10—C8ii | 119.9 (2) |
| C1—C2—C3 | 120.4 (2) | C9—C10—H10 | 120.0 |
| C1—C2—H2 | 119.8 | C8ii—C10—H10 | 120.0 |
| C3—C2—H2 | 119.8 | C1—N1—C5 | 116.27 (19) |
| C2—C3—C4 | 115.8 (2) | C1—N1—Ni1 | 122.60 (15) |
| C2—C3—C3i | 122.1 (2) | C5—N1—Ni1 | 121.09 (15) |
| C4—C3—C3i | 122.1 (2) | O1—Ni1—O1iii | 180.000 (1) |
| C5—C4—C3 | 120.3 (2) | O1—Ni1—O1Wiii | 92.17 (6) |
| C5—C4—H4 | 119.8 | O1iii—Ni1—O1Wiii | 87.83 (6) |
| C3—C4—H4 | 119.8 | O1—Ni1—O1W | 87.83 (6) |
| N1—C5—C4 | 123.5 (2) | O1iii—Ni1—O1W | 92.17 (6) |
| N1—C5—H5 | 118.3 | O1Wiii—Ni1—O1W | 180.0 |
| C4—C5—H5 | 118.3 | O1—Ni1—N1iii | 90.23 (7) |
| O2—C6—O1 | 126.6 (2) | O1iii—Ni1—N1iii | 89.77 (7) |
| O2—C6—C7 | 116.8 (2) | O1Wiii—Ni1—N1iii | 91.96 (7) |
| O1—C6—C7 | 116.6 (2) | O1W—Ni1—N1iii | 88.04 (7) |
| O3—C7—C6 | 114.3 (2) | O1—Ni1—N1 | 89.77 (7) |
| O3—C7—H7A | 108.7 | O1iii—Ni1—N1 | 90.23 (7) |
| C6—C7—H7A | 108.7 | O1Wiii—Ni1—N1 | 88.04 (7) |
| O3—C7—H7B | 108.7 | O1W—Ni1—N1 | 91.96 (7) |
| C6—C7—H7B | 108.7 | N1iii—Ni1—N1 | 180.000 (1) |
| H7A—C7—H7B | 107.6 | C6—O1—Ni1 | 126.73 (15) |
| O3—C8—C9 | 115.9 (2) | C8—O3—C7 | 117.78 (19) |
| O3—C8—C10ii | 125.3 (2) | Ni1—O1W—H1W | 100.2 |
| C9—C8—C10ii | 118.8 (2) | Ni1—O1W—H2W | 131.1 |
| C10—C9—C8 | 121.3 (2) | H1W—O1W—H2W | 108.2 |
| Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x+1, −y+2, −z+3; (iii) −x, −y+2, −z+2. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1W—H1W···O2iii | 0.82 | 1.81 | 2.605 (2) | 163 |
| O1W—H2W···O1iv | 0.81 | 2.21 | 2.962 (2) | 155 |
| Symmetry codes: (iii) −x, −y+2, −z+2; (iv) −x+1, −y+2, −z+2. |
| N1—Ni1 | 2.1735 (18) | Ni1—O1W | 2.1245 (16) |
| Ni1—O1 | 2.0869 (15) | ||
| O1—Ni1—O1W | 87.83 (6) | O1W—Ni1—N1 | 91.96 (7) |
| O1—Ni1—N1 | 89.77 (7) |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1W—H1W···O2i | 0.82 | 1.81 | 2.605 (2) | 163 |
| O1W—H2W···O1ii | 0.81 | 2.21 | 2.962 (2) | 155 |
| Symmetry codes: (i) −x, −y+2, −z+2; (ii) −x+1, −y+2, −z+2. |
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Benzene-1,4-dioxydiacetic acid is an important biologically active compound that has been commonly used in herbicides and plant-growth agents. The two phenoxyacetate groups have versatile bonding modes to metal ions and easily forms complexes (Gao et al., 2005; Hong et al., 2006; Qiu et al., 2006; Qiu et al., 2007). Recently, we obtained the title nickel polymer (I), its crystal structure is reported here.
In the structure of (I) each NiII atom is coordinated by two O atoms from two benzene-1,4-dioxydiacetate ligands, two N atom from two 4,4'-bpy ligands, and displays a distorted octahedral geometry. The Ni atom lies on an inversion center and benzene-1,4-dioxydiacetate and 4,4'-bpy moieties lie other inversion centers. The benzene-1,4-dioxydiacetate ligands bridge nickel ions to form infinite zigzag chains, which are further interconnected by 4,4'-bpy ligands to form a grid-like layer parallel to the (0 - 1 1) plane (Fig. 2). Moreover, there are O—H···O hydrogen bonding interactions within the grid-like layer between the coordinated water molecules and the carboxylate O atoms (Table 1).