metal-organic compounds
catena-Poly[[[diaqua(di-2-pyridylamine-κ2N,N′)nickel(II)]-μ-fumarato-κ2O1:O4] tetrahydrate]
aDepartment of Inorganic Chemistry, Institute of Chemistry, P. J. Šafárik University, Moyzesova 11, 041 54 Košice, Slovakia, and bFachbereich Chemie der Philipps Universität, Hans-Meerwein Strasse, D-35032 Marburg, Germany
*Correspondence e-mail: juraj.cernak@upjs.sk
In the 4H2O4)(C10H9N3)(H2O)2]·4H2O}n, zigzag chains are built up from cis-[Ni(dpya)(H2O)2]2+ cations (dpya is di-2-pyridylamine) linked by bis-monodentate coordinated bridging fumarate ligands. The NiII atom is coordinated by one chelating dpya ligand, two aqua ligands in trans positions and two monodentate fumarate ligands in cis positions in the form of a deformed octahedron. The water molecules, O atoms of the fumarate carboxylate groups and the amine group of the dpya ligand are involved in an extended network of intra- and intermolecular O—H⋯O hydrogen bonds. Moreover, π–π interactions between the pyridine rings of the dpya ligand contribute to the stability of the structure. Two of the five uncoordinated water molecules are half-occupied.
of the title compound, {[Ni(CRelated literature
Several crystal structures of NiII fumarato (fum) complexes with bridging fumarato ligands have been reported in the literature, e.g. [Ni2(phen)4(fumarate)(H2O)2]fumarate·16H2O (phen = 1,10-phenantroline) (Ma et al., 2003) with a dinuclear structure, [Ni(py)3(fumarate)2]·py (py= pyridine (Mori et al., 2004) and [Ni(fumarate)(H2O)4] (Xie et al., 2003), both forming chain-like structures, or [Ni(phen)fum)] exhibiting a two-dimensional structure (Černák et al., 2009). For structurally characterized complexes of NiII containing the dpya ligand (dpya = 2,2′-dipyridylamine), see, for example: [Ni(dpya)(ox)]n (ox = oxalato) (Lu et al., 2001) or [Ni(dpya)2(dca)2] (dca = dicyanamidato) complexes (Huang et al., 2006).
Experimental
Crystal data
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Refinement
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Data collection: IPDS (Stoe & Cie, 1996); cell IPDS; data reduction: IPDS; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97.
Supporting information
https://doi.org/10.1107/S1600536810012225/hg2662sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810012225/hg2662Isup2.hkl
With the exception of dpya, which was of purum quality, the other reagents were of analytical grade and all were used without further purification. The title complex was prepared using the following procedure. An aqueous solution of Ni(CH3COO)2.4H2O(248 mg, 1 mmol in 30 cm3 H2O) and a solution of 171 mg (1 mmol) dpya ligand in 40 cm3of EtOH (96 %vv) were mixed firstly. To the formed azure hot (90 °C) solution solid fumaric acid (116 mg, 1 mmol) and aqueous solution of NaOH (2 cm3, 1 M) were added successively and the reaction mixture was stirred 60 minutes at 90 °C. The formed blue solution was left to evaporate slowly at room temperature. Within a week, in one of several reaction attempts, few blue plates of the title compound appeared. One crystal was picked off for X-ray structure analysis. After disturbing the mother liquor immediate jellification started which prevented isolation of further crystals.
All H atoms linked to aromatic carbon atoms were positioned geometrically, with C–H = 0.96Å and refined as riding with Uiso(H) = 1.2Ueq(C). The hydrogen atom H3N bonded to amine nitrogen atom N3 was refined with restrained distance N—H 0.89 Å and with Uiso(H) = 1.2Ueq(N). The hydrogen atoms from water molecules with full oxygen atom occupancies were located using the CALC-OH program within WinGX package (Farrugia, 1999) and refined with constrained geometric parameters (O—H, 0.85 Å and H···H, 1.334 Å); their thermal parameters were tied with parent oxygen atom(Uiso(H) = 1.5Ueq(O)).
As a continuation of our studies on syntheses, crystal structures and relationship structure vs. magnetic properties of low-dimensional magnetic materials [Černák et al., 2009] we have occasionally isolated a crystal of the title compound 1. Its
is polymeric and is composed of zig–zag chains and water molecules of crystallization (Fig. 1, 2, 3). The chains are formed by octahedrally coordinated NiII atoms linked by two bis(monodentate) fumarato ligands (Fig. 1, 2). Similar chain-like structure was observed in an another fumarato complex, [Ni(py)3(fumarate)2].py (py= pyridine) in which the NiII atoms are bridged alternatively by bis(monodentate) and bis(bidentate) bonded fumarato ligands [Mori et al., 2004].The heteroleptic coordination sphere of the NiII atom beside two fumarato ligands is completed by one bidentate chelate bonded dpya ligand and two aqua ligands placed in trans positions (Fig. 1). As can be seen from the values of the bond angles (Table 2), the octahedron around the NiII atom is somewhat deformed. The mean Ni–N bond lengths is 2.059 (3) Å, and the Ni–O bond lengths exhibit values from the range 2.048 (2) – 2.099 (2) Å. Similar values of Ni–N and Ni–O bond distances were observed in complexes [Ni(dpya)(ox)]n (Ni–N: 2.046 (2) Å) (Lu et al., 2001) and [Ni(fumarate)(H2O)4] (Ni–O: 2.064 (2) Å) (Xie et al., 2003).
The same type of bridging formed by bis(monodentato) fumarate ligand was already observed in dinuclear [Ni2(phen)4(fumarate)(H2O)2]fumarate.16H2O complex (phen = 1,10-phenantroline) (Ma et al., 2003). The observed geometric parameters associated with the fumarate ligand in 1 are similar to those found in the previously mentioned dinuclear complex (Ma et al., 2003) or in ionic.
The geometric parameters associated with dpya and aqua ligands are normal [Lu et al., 2001; Huang et al., 2006]. There are five general crystallographically distinct positions in the π–π interactions operate which further stabilize the structure (Fig. 3). The Cg1···Cg2i distance (symmetry code (i) -x, 0.5+y, 0.5-z, where Cg1 and Cg2 are centroids of the rings (N1/C1—C5) and (N2/C6—C10), respectively) between the aromatic rings is 3.723 (1) Å; these interactions links the {Ni(dpya)} units into layers lying in the bc plane.
occupied by not coordinated water molecules. Among these two positions (O8 and O9) are partially occupied with s.o.f. put to half as required by proximity of symmetry (-1) related positions of O8 and proximity of the O9 water oxygen to O8, respectively. The water molecules along with the not coordinated oxygen atoms from carboxylate groups are involved in hydrogen bonds of the O—H···O type; some of these HBs are intramolecular (Fig. 2, Table 3). In the hydrogen bonding system is involved also the dpyaligand through N—H···O type hydrogen bond (Fig. 2, Table 3). Between pairs of dpya ligandsSeveral crystal structures of NiII fumarato (fum) complexes with bridging fumarato ligands are reported in the literature, e.g. [Ni2(phen)4(fumarate)(H2O)2]fumarate.16H2O ( phen = 1,10-phenantroline) (Ma et al., 2003) with dinuclear structure, [Ni(py)3(fumarate)2].py (py= pyridine (Mori et al., 2004) and [Ni(fumarate)(H2O)4] (Xie et al., 2003), both forming chain-like structures, or [Ni(phen)fum)] exhibiting a two-dimensional structure (Černák et al., 2009). For structurally characterized complexes of NiII containing the dpya ligand (dpya = 2,2'-dipyidylamine), see, for example: [Ni(dpya)(ox)]n (ox = oxalato) (Lu et al., 2001) or [Ni(dpya)2(dca)2] (dca = dicyanamidato) complexes (Huang et al., 2006).
Data collection: IPDS (Stoe & Cie, 1996); cell
IPDS (Stoe & Cie, 1996); data reduction: IPDS (Stoe & Cie, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).Fig. 1. View of the crystal structure 1. The thermal ellipsoids are drawn at 30 % probability level. Symmetry codes: i: 1 - x, -0.5 + y, 0.5 - z, ii: 1 - x, 0.5 + y, 0.5 - z. | |
Fig. 2. Chain-like structure of 1 along with intramolecular and intermolecular hydrogen bonds (dashed lines). The bonds within the chain propagation are dark grey. The oxygen atoms with half ocupancy are drawn as half-transparent balls. Symmetry codes: i: 1 - x, 0.5 + y, 0.5 - z; ii: 1 - x, -0.5 + y, 0.5 - z; iii: x, 1.5 - y, -0.5 - z; iv: 1 - x, 1 - y, - z; v: 1 - x, 2 - y, - z; vi: - x, -0.5 + y, 0.5 - z. | |
Fig. 3. Scheme of π-π-interactions in 1. For the sake of clarity only the {Ni(dpya)} structural units are shown without hydrogen atoms. Symmetry codes: i: - x, 0.5 + y, 0.5 - z; ii: - x, -0.5 + y, 0.5 - z; iii: -x, 1 - y, 1 - z; iv: x, 1.5 - y, 0.5 + z. |
[Ni(C4H2O4)(C10H9N3)(H2O)2]·4H2O | F(000) = 936 |
Mr = 450.03 | Dx = 1.551 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 8000 reflections |
a = 12.1421 (12) Å | θ = 2.3–25.0° |
b = 12.4034 (8) Å | µ = 1.06 mm−1 |
c = 12.8701 (13) Å | T = 193 K |
β = 96.138 (12)° | Plates, blue |
V = 1927.2 (3) Å3 | 0.42 × 0.36 × 0.16 mm |
Z = 4 |
Stoe IPDS diffractometer | 3397 independent reflections |
Radiation source: fine-focus sealed tube | 2538 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.048 |
φ scans | θmax = 25.0°, θmin = 2.3° |
Absorption correction: gaussian (WinGX; Farrugia, 1999) | h = −14→14 |
Tmin = 0.750, Tmax = 0.836 | k = −14→14 |
13672 measured reflections | l = −15→15 |
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)] = 0.029 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.069 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.90 | w = 1/[σ2(Fo2) + (0.0432P)2] where P = (Fo2 + 2Fc2)/3 |
3397 reflections | (Δ/σ)max = 0.001 |
280 parameters | Δρmax = 0.42 e Å−3 |
16 restraints | Δρmin = −0.31 e Å−3 |
[Ni(C4H2O4)(C10H9N3)(H2O)2]·4H2O | V = 1927.2 (3) Å3 |
Mr = 450.03 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 12.1421 (12) Å | µ = 1.06 mm−1 |
b = 12.4034 (8) Å | T = 193 K |
c = 12.8701 (13) Å | 0.42 × 0.36 × 0.16 mm |
β = 96.138 (12)° |
Stoe IPDS diffractometer | 3397 independent reflections |
Absorption correction: gaussian (WinGX; Farrugia, 1999) | 2538 reflections with I > 2σ(I) |
Tmin = 0.750, Tmax = 0.836 | Rint = 0.048 |
13672 measured reflections |
R[F2 > 2σ(F2)] = 0.029 | 16 restraints |
wR(F2) = 0.069 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.90 | Δρmax = 0.42 e Å−3 |
3397 reflections | Δρmin = −0.31 e Å−3 |
280 parameters |
Experimental. Absorption correction: a grid of 8 x 8 x 8 = 512 sampling points was used |
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 > 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 | Occ. (<1) | |
Ni | 0.24621 (2) | 0.59939 (2) | 0.31901 (2) | 0.01368 (9) | |
N1 | 0.15403 (15) | 0.73037 (15) | 0.35699 (14) | 0.0191 (4) | |
N2 | 0.12272 (15) | 0.50121 (15) | 0.36286 (14) | 0.0179 (4) | |
N3 | −0.01512 (15) | 0.63520 (17) | 0.32761 (16) | 0.0237 (5) | |
H3N | −0.0882 (3) | 0.644 (2) | 0.317 (2) | 0.028* | |
C1 | 0.2063 (2) | 0.82458 (19) | 0.38251 (18) | 0.0237 (5) | |
H1 | 0.2833 | 0.8248 | 0.3912 | 0.028* | |
C2 | 0.1523 (2) | 0.9199 (2) | 0.3963 (2) | 0.0310 (6) | |
H2 | 0.1917 | 0.9827 | 0.4141 | 0.037* | |
C3 | 0.0372 (2) | 0.9198 (2) | 0.3831 (2) | 0.0336 (7) | |
H3 | −0.0020 | 0.9835 | 0.3898 | 0.040* | |
C4 | −0.0179 (2) | 0.8252 (2) | 0.35992 (19) | 0.0286 (6) | |
H4 | −0.0949 | 0.8236 | 0.3519 | 0.034* | |
C5 | 0.04309 (19) | 0.73020 (19) | 0.34832 (18) | 0.0204 (5) | |
C6 | 0.01564 (18) | 0.53059 (19) | 0.35449 (18) | 0.0197 (5) | |
C7 | −0.0681 (2) | 0.4572 (2) | 0.37210 (19) | 0.0278 (6) | |
H7 | −0.1419 | 0.4787 | 0.3649 | 0.033* | |
C8 | −0.0401 (2) | 0.3536 (2) | 0.4000 (2) | 0.0321 (6) | |
H8 | −0.0949 | 0.3038 | 0.4111 | 0.039* | |
C9 | 0.0702 (2) | 0.3232 (2) | 0.4115 (2) | 0.0298 (6) | |
H9 | 0.0909 | 0.2535 | 0.4318 | 0.036* | |
C10 | 0.14803 (19) | 0.3986 (2) | 0.39222 (18) | 0.0232 (5) | |
H10 | 0.2221 | 0.3782 | 0.3997 | 0.028* | |
C11 | 0.35852 (19) | 0.41929 (18) | 0.21127 (18) | 0.0211 (5) | |
C12 | 0.4552 (2) | 0.34435 (19) | 0.2153 (2) | 0.0237 (5) | |
H12 | 0.4647 | 0.3038 | 0.1561 | 0.028* | |
C13 | 0.52676 (19) | 0.33281 (19) | 0.29733 (19) | 0.0219 (5) | |
H13 | 0.5169 | 0.3725 | 0.3569 | 0.026* | |
C14 | 0.37611 (18) | 0.75874 (18) | 0.20000 (18) | 0.0194 (5) | |
O1 | 0.34712 (13) | 0.47257 (12) | 0.29159 (12) | 0.0215 (4) | |
O2 | 0.29572 (18) | 0.42549 (19) | 0.12676 (16) | 0.0551 (7) | |
O3 | 0.37265 (13) | 0.69567 (13) | 0.27580 (13) | 0.0232 (4) | |
O4 | 0.30434 (14) | 0.76425 (15) | 0.12189 (13) | 0.0321 (4) | |
O5 | 0.33762 (13) | 0.59538 (13) | 0.46659 (12) | 0.0219 (3) | |
H5A | 0.3240 | 0.6366 | 0.5164 | 0.033* | |
H5B | 0.3568 | 0.5360 | 0.4962 | 0.033* | |
O6 | 0.17160 (12) | 0.59825 (13) | 0.16421 (12) | 0.0175 (3) | |
H6A | 0.2057 | 0.6510 | 0.1403 | 0.026* | |
H6B | 0.2005 | 0.5428 | 0.1393 | 0.026* | |
O7 | 0.25446 (19) | 0.1566 (3) | 0.2196 (3) | 0.0818 (9) | |
H7A | 0.3002 | 0.1105 | 0.2475 | 0.123* | |
H7B | 0.2680 | 0.1597 | 0.1562 | 0.123* | |
O8 | 0.4461 (4) | 0.5742 (5) | 0.0058 (5) | 0.0810 (18) | 0.50 |
O9 | 0.5592 (5) | 0.5821 (4) | 0.1705 (5) | 0.0784 (17) | 0.50 |
O10 | 0.6567 (2) | 0.6997 (2) | 0.04168 (19) | 0.0643 (7) | |
H10B | 0.6851 | 0.6769 | −0.0117 | 0.096* | |
H10A | 0.6224 | 0.6455 | 0.0627 | 0.096* | |
O11 | 0.58881 (17) | 0.89674 (18) | −0.0632 (2) | 0.0576 (6) | |
H11A | 0.5219 | 0.8939 | −0.0903 | 0.086* | |
H11B | 0.5919 | 0.8526 | −0.0124 | 0.086* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni | 0.01153 (14) | 0.01349 (14) | 0.01623 (15) | 0.00042 (12) | 0.00244 (10) | 0.00048 (13) |
N1 | 0.0205 (10) | 0.0199 (10) | 0.0169 (10) | 0.0030 (8) | 0.0016 (8) | 0.0003 (8) |
N2 | 0.0179 (9) | 0.0190 (10) | 0.0168 (10) | −0.0008 (8) | 0.0028 (8) | 0.0003 (8) |
N3 | 0.0118 (9) | 0.0314 (11) | 0.0281 (11) | 0.0050 (8) | 0.0038 (8) | 0.0010 (9) |
C1 | 0.0292 (13) | 0.0187 (12) | 0.0225 (13) | 0.0014 (10) | −0.0008 (10) | −0.0014 (10) |
C2 | 0.0468 (16) | 0.0206 (13) | 0.0245 (13) | 0.0045 (11) | −0.0013 (12) | −0.0031 (11) |
C3 | 0.0504 (17) | 0.0292 (15) | 0.0216 (13) | 0.0210 (12) | 0.0059 (12) | 0.0001 (11) |
C4 | 0.0291 (13) | 0.0361 (15) | 0.0209 (13) | 0.0158 (12) | 0.0033 (11) | 0.0010 (12) |
C5 | 0.0200 (12) | 0.0263 (13) | 0.0152 (11) | 0.0073 (10) | 0.0034 (9) | 0.0029 (10) |
C6 | 0.0165 (11) | 0.0283 (13) | 0.0151 (11) | −0.0024 (10) | 0.0046 (9) | −0.0017 (10) |
C7 | 0.0182 (12) | 0.0417 (16) | 0.0241 (13) | −0.0099 (11) | 0.0052 (10) | −0.0056 (12) |
C8 | 0.0348 (15) | 0.0390 (15) | 0.0239 (14) | −0.0195 (13) | 0.0088 (11) | −0.0038 (12) |
C9 | 0.0435 (16) | 0.0223 (13) | 0.0244 (14) | −0.0089 (11) | 0.0079 (12) | 0.0034 (11) |
C10 | 0.0255 (12) | 0.0232 (12) | 0.0211 (12) | −0.0002 (11) | 0.0032 (10) | 0.0036 (11) |
C11 | 0.0189 (11) | 0.0212 (13) | 0.0230 (12) | 0.0044 (9) | 0.0004 (10) | −0.0053 (10) |
C12 | 0.0246 (13) | 0.0235 (13) | 0.0231 (13) | 0.0075 (10) | 0.0032 (11) | −0.0082 (10) |
C13 | 0.0211 (12) | 0.0238 (12) | 0.0212 (13) | 0.0062 (10) | 0.0038 (10) | −0.0070 (10) |
C14 | 0.0178 (11) | 0.0204 (12) | 0.0205 (13) | −0.0017 (9) | 0.0046 (10) | 0.0007 (10) |
O1 | 0.0214 (8) | 0.0229 (9) | 0.0204 (9) | 0.0079 (7) | 0.0028 (7) | −0.0021 (7) |
O2 | 0.0490 (12) | 0.0711 (16) | 0.0394 (12) | 0.0426 (11) | −0.0229 (10) | −0.0330 (11) |
O3 | 0.0168 (8) | 0.0257 (9) | 0.0263 (9) | −0.0048 (7) | −0.0010 (7) | 0.0096 (8) |
O4 | 0.0302 (10) | 0.0396 (11) | 0.0245 (10) | −0.0173 (8) | −0.0065 (8) | 0.0124 (8) |
O5 | 0.0287 (9) | 0.0184 (8) | 0.0177 (8) | 0.0061 (8) | −0.0018 (7) | −0.0021 (7) |
O6 | 0.0152 (7) | 0.0167 (7) | 0.0208 (8) | −0.0001 (7) | 0.0022 (6) | −0.0009 (7) |
O7 | 0.0263 (12) | 0.090 (2) | 0.127 (3) | −0.0084 (13) | −0.0006 (15) | 0.001 (2) |
O8 | 0.050 (3) | 0.098 (4) | 0.093 (4) | −0.020 (3) | 0.002 (3) | 0.052 (3) |
O9 | 0.079 (4) | 0.048 (3) | 0.115 (5) | 0.000 (3) | 0.043 (3) | 0.012 (3) |
O10 | 0.0457 (14) | 0.100 (2) | 0.0457 (14) | 0.0087 (14) | −0.0023 (10) | −0.0358 (15) |
O11 | 0.0310 (11) | 0.0421 (13) | 0.096 (2) | −0.0019 (10) | −0.0092 (11) | −0.0267 (13) |
Ni—O1 | 2.0475 (15) | C8—H8 | 0.9300 |
Ni—N2 | 2.0569 (18) | C9—C10 | 1.371 (3) |
Ni—N1 | 2.0611 (19) | C9—H9 | 0.9300 |
Ni—O3 | 2.0676 (15) | C10—H10 | 0.9300 |
Ni—O5 | 2.0955 (16) | C11—O1 | 1.247 (3) |
Ni—O6 | 2.0986 (16) | C11—O2 | 1.262 (3) |
N1—C5 | 1.340 (3) | C11—C12 | 1.493 (3) |
N1—C1 | 1.353 (3) | C12—C13 | 1.302 (3) |
N2—C6 | 1.343 (3) | C12—H12 | 0.9300 |
N2—C10 | 1.353 (3) | C13—C14i | 1.492 (3) |
N3—C6 | 1.384 (3) | C13—H13 | 0.9300 |
N3—C5 | 1.385 (3) | C14—O3 | 1.255 (3) |
N3—H3N | 0.8899 (10) | C14—O4 | 1.260 (3) |
C1—C2 | 1.372 (3) | C14—C13ii | 1.492 (3) |
C1—H1 | 0.9300 | O5—H5A | 0.8499 |
C2—C3 | 1.390 (4) | O5—H5B | 0.8499 |
C2—H2 | 0.9300 | O6—H6A | 0.8499 |
C3—C4 | 1.368 (4) | O6—H6B | 0.8499 |
C3—H3 | 0.9300 | O7—H7A | 0.8499 |
C4—C5 | 1.408 (3) | O7—H7B | 0.8500 |
C4—H4 | 0.9300 | O10—H10B | 0.8500 |
C6—C7 | 1.401 (3) | O10—H10A | 0.8499 |
C7—C8 | 1.367 (4) | O11—H11A | 0.8499 |
C7—H7 | 0.9300 | O11—H11B | 0.8500 |
C8—C9 | 1.384 (4) | ||
O1—Ni—N2 | 93.42 (7) | N2—C6—N3 | 120.5 (2) |
O1—Ni—N1 | 175.24 (7) | N2—C6—C7 | 121.6 (2) |
N2—Ni—N1 | 88.36 (8) | N3—C6—C7 | 117.9 (2) |
O1—Ni—O3 | 85.53 (7) | C8—C7—C6 | 119.2 (2) |
N2—Ni—O3 | 178.84 (7) | C8—C7—H7 | 120.4 |
N1—Ni—O3 | 92.65 (7) | C6—C7—H7 | 120.4 |
O1—Ni—O5 | 82.49 (6) | C7—C8—C9 | 119.7 (2) |
N2—Ni—O5 | 93.92 (7) | C7—C8—H8 | 120.2 |
N1—Ni—O5 | 92.99 (7) | C9—C8—H8 | 120.2 |
O3—Ni—O5 | 85.46 (6) | C10—C9—C8 | 118.2 (2) |
O1—Ni—O6 | 92.10 (6) | C10—C9—H9 | 120.9 |
N2—Ni—O6 | 90.18 (7) | C8—C9—H9 | 120.9 |
N1—Ni—O6 | 92.30 (7) | N2—C10—C9 | 123.5 (2) |
O3—Ni—O6 | 90.35 (6) | N2—C10—H10 | 118.3 |
O5—Ni—O6 | 173.40 (6) | C9—C10—H10 | 118.3 |
C5—N1—C1 | 117.6 (2) | O1—C11—O2 | 124.9 (2) |
C5—N1—Ni | 123.07 (16) | O1—C11—C12 | 117.2 (2) |
C1—N1—Ni | 119.05 (15) | O2—C11—C12 | 117.9 (2) |
C6—N2—C10 | 117.80 (19) | C13—C12—C11 | 123.4 (2) |
C6—N2—Ni | 123.03 (15) | C13—C12—H12 | 118.3 |
C10—N2—Ni | 118.87 (15) | C11—C12—H12 | 118.3 |
C6—N3—C5 | 129.1 (2) | C12—C13—C14i | 123.0 (2) |
C6—N3—H3N | 113.0 (18) | C12—C13—H13 | 118.5 |
C5—N3—H3N | 114.0 (18) | C14i—C13—H13 | 118.5 |
N1—C1—C2 | 123.8 (2) | O3—C14—O4 | 125.2 (2) |
N1—C1—H1 | 118.1 | O3—C14—C13ii | 117.3 (2) |
C2—C1—H1 | 118.1 | O4—C14—C13ii | 117.5 (2) |
C1—C2—C3 | 118.2 (2) | C11—O1—Ni | 132.19 (15) |
C1—C2—H2 | 120.9 | C14—O3—Ni | 131.06 (14) |
C3—C2—H2 | 120.9 | Ni—O5—H5A | 122.8 |
C4—C3—C2 | 119.2 (2) | Ni—O5—H5B | 121.3 |
C4—C3—H3 | 120.4 | H5A—O5—H5B | 104.5 |
C2—C3—H3 | 120.4 | Ni—O6—H6A | 99.3 |
C3—C4—C5 | 119.4 (2) | Ni—O6—H6B | 102.1 |
C3—C4—H4 | 120.3 | H6A—O6—H6B | 104.5 |
C5—C4—H4 | 120.3 | H7A—O7—H7B | 104.5 |
N1—C5—N3 | 120.3 (2) | H10B—O10—H10A | 104.5 |
N1—C5—C4 | 121.7 (2) | H11A—O11—H11B | 104.5 |
N3—C5—C4 | 118.0 (2) | ||
N2—Ni—N1—C5 | −30.95 (18) | C10—N2—C6—N3 | 178.2 (2) |
O3—Ni—N1—C5 | 149.62 (18) | Ni—N2—C6—N3 | −8.2 (3) |
O5—Ni—N1—C5 | −124.78 (18) | C10—N2—C6—C7 | −2.0 (3) |
O6—Ni—N1—C5 | 59.16 (18) | Ni—N2—C6—C7 | 171.57 (17) |
N2—Ni—N1—C1 | 155.52 (18) | C5—N3—C6—N2 | −30.8 (4) |
O3—Ni—N1—C1 | −23.91 (18) | C5—N3—C6—C7 | 149.4 (2) |
O5—Ni—N1—C1 | 61.69 (18) | N2—C6—C7—C8 | 1.0 (4) |
O6—Ni—N1—C1 | −114.37 (17) | N3—C6—C7—C8 | −179.2 (2) |
O1—Ni—N2—C6 | −154.26 (18) | C6—C7—C8—C9 | 0.7 (4) |
N1—Ni—N2—C6 | 30.16 (18) | C7—C8—C9—C10 | −1.3 (4) |
O5—Ni—N2—C6 | 123.05 (18) | C6—N2—C10—C9 | 1.4 (3) |
O6—Ni—N2—C6 | −62.14 (18) | Ni—N2—C10—C9 | −172.42 (19) |
O1—Ni—N2—C10 | 19.27 (17) | C8—C9—C10—N2 | 0.2 (4) |
N1—Ni—N2—C10 | −156.31 (17) | O1—C11—C12—C13 | −0.2 (4) |
O5—Ni—N2—C10 | −63.42 (17) | O2—C11—C12—C13 | 178.6 (3) |
O6—Ni—N2—C10 | 111.39 (17) | C11—C12—C13—C14i | −179.2 (2) |
C5—N1—C1—C2 | −2.3 (3) | O2—C11—O1—Ni | −9.5 (4) |
Ni—N1—C1—C2 | 171.57 (19) | C12—C11—O1—Ni | 169.25 (15) |
N1—C1—C2—C3 | −0.2 (4) | N2—Ni—O1—C11 | 91.7 (2) |
C1—C2—C3—C4 | 1.9 (4) | O3—Ni—O1—C11 | −88.8 (2) |
C2—C3—C4—C5 | −1.1 (4) | O5—Ni—O1—C11 | −174.8 (2) |
C1—N1—C5—N3 | −176.7 (2) | O6—Ni—O1—C11 | 1.4 (2) |
Ni—N1—C5—N3 | 9.7 (3) | O4—C14—O3—Ni | −12.0 (4) |
C1—N1—C5—C4 | 3.2 (3) | C13ii—C14—O3—Ni | 168.21 (15) |
Ni—N1—C5—C4 | −170.46 (17) | O1—Ni—O3—C14 | 115.7 (2) |
C6—N3—C5—N1 | 29.9 (4) | N1—Ni—O3—C14 | −68.7 (2) |
C6—N3—C5—C4 | −150.0 (2) | O5—Ni—O3—C14 | −161.5 (2) |
C3—C4—C5—N1 | −1.6 (4) | O6—Ni—O3—C14 | 23.6 (2) |
C3—C4—C5—N3 | 178.3 (2) |
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) −x+1, y+1/2, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O5—H5A···O4iii | 0.85 | 1.87 | 2.713 (2) | 175 |
O5—H5B···O11i | 0.85 | 2.01 | 2.859 (3) | 177 |
O6—H6B···O2 | 0.85 | 1.88 | 2.693 (2) | 161 |
O6—H6A···O4 | 0.85 | 1.88 | 2.706 (2) | 165 |
O7—H7B···O11iv | 0.85 | 2.32 | 2.988 (4) | 136 |
O7—H7A···O9i | 0.85 | 1.94 | 2.700 (7) | 148 |
O10—H10B···O2iv | 0.85 | 1.98 | 2.777 (3) | 155 |
O10—H10A···O8 | 0.85 | 2.36 | 2.987 (6) | 131 |
O10—H10A···O9 | 0.85 | 1.83 | 2.588 (6) | 147 |
O11—H11A···O5v | 0.85 | 2.43 | 3.116 (3) | 138 |
O11—H11B···O10 | 0.85 | 2.14 | 2.870 (4) | 144 |
N3—H3N···O7vi | 0.89 (1) | 2.03 (1) | 2.917 (3) | 175 (3) |
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (iii) x, −y+3/2, z+1/2; (iv) −x+1, −y+1, −z; (v) x, −y+3/2, z−1/2; (vi) −x, y+1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [Ni(C4H2O4)(C10H9N3)(H2O)2]·4H2O |
Mr | 450.03 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 193 |
a, b, c (Å) | 12.1421 (12), 12.4034 (8), 12.8701 (13) |
β (°) | 96.138 (12) |
V (Å3) | 1927.2 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 1.06 |
Crystal size (mm) | 0.42 × 0.36 × 0.16 |
Data collection | |
Diffractometer | Stoe IPDS |
Absorption correction | Gaussian (WinGX; Farrugia, 1999) |
Tmin, Tmax | 0.750, 0.836 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 13672, 3397, 2538 |
Rint | 0.048 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.029, 0.069, 0.90 |
No. of reflections | 3397 |
No. of parameters | 280 |
No. of restraints | 16 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.42, −0.31 |
Computer programs: IPDS (Stoe & Cie, 1996), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2006).
D—H···A | D—H | H···A | D···A | D—H···A |
O5—H5A···O4i | 0.85 | 1.87 | 2.713 (2) | 174.6 |
O5—H5B···O11ii | 0.85 | 2.01 | 2.859 (3) | 176.6 |
O6—H6B···O2 | 0.85 | 1.88 | 2.693 (2) | 160.5 |
O6—H6A···O4 | 0.85 | 1.88 | 2.706 (2) | 164.6 |
O7—H7B···O11iii | 0.85 | 2.32 | 2.988 (4) | 135.6 |
O7—H7A···O9ii | 0.85 | 1.94 | 2.700 (7) | 148.1 |
O10—H10B···O2iii | 0.85 | 1.98 | 2.777 (3) | 155.1 |
O10—H10A···O8 | 0.85 | 2.36 | 2.987 (6) | 131.0 |
O10—H10A···O9 | 0.85 | 1.83 | 2.588 (6) | 147.1 |
O11—H11A···O5iv | 0.85 | 2.43 | 3.116 (3) | 138.1 |
O11—H11B···O10 | 0.85 | 2.14 | 2.870 (4) | 143.6 |
N3—H3N···O7v | 0.8899 (10) | 2.029 (4) | 2.917 (3) | 175 (3) |
Symmetry codes: (i) x, −y+3/2, z+1/2; (ii) −x+1, y−1/2, −z+1/2; (iii) −x+1, −y+1, −z; (iv) x, −y+3/2, z−1/2; (v) −x, y+1/2, −z+1/2. |
Acknowledgements
This work was supported by the Slovak grant agency APVV under contract Nos. APVV-VVCE-0058–07 and APVV-0006–07, and by the grant agency VEGA (1/0089/09). Support from P. J. Šafarik University (VVGS 37/09–10) is acknowledged. AP thanks DAAD for the financial support during her stay at Philipps-Universität, Marburg. The authors thank Professor W. Massa (Philipps-Universität, Marburg) for his kind permission to use the diffractometer.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
As a continuation of our studies on syntheses, crystal structures and relationship structure vs. magnetic properties of low-dimensional magnetic materials [Černák et al., 2009] we have occasionally isolated a crystal of the title compound 1. Its crystal structure is polymeric and is composed of zig–zag chains and water molecules of crystallization (Fig. 1, 2, 3). The chains are formed by octahedrally coordinated NiII atoms linked by two bis(monodentate) fumarato ligands (Fig. 1, 2). Similar chain-like structure was observed in an another fumarato complex, [Ni(py)3(fumarate)2].py (py= pyridine) in which the NiII atoms are bridged alternatively by bis(monodentate) and bis(bidentate) bonded fumarato ligands [Mori et al., 2004].
The heteroleptic coordination sphere of the NiII atom beside two fumarato ligands is completed by one bidentate chelate bonded dpya ligand and two aqua ligands placed in trans positions (Fig. 1). As can be seen from the values of the bond angles (Table 2), the octahedron around the NiII atom is somewhat deformed. The mean Ni–N bond lengths is 2.059 (3) Å, and the Ni–O bond lengths exhibit values from the range 2.048 (2) – 2.099 (2) Å. Similar values of Ni–N and Ni–O bond distances were observed in complexes [Ni(dpya)(ox)]n (Ni–N: 2.046 (2) Å) (Lu et al., 2001) and [Ni(fumarate)(H2O)4] (Ni–O: 2.064 (2) Å) (Xie et al., 2003).
The same type of bridging formed by bis(monodentato) fumarate ligand was already observed in dinuclear [Ni2(phen)4(fumarate)(H2O)2]fumarate.16H2O complex (phen = 1,10-phenantroline) (Ma et al., 2003). The observed geometric parameters associated with the fumarate ligand in 1 are similar to those found in the previously mentioned dinuclear complex (Ma et al., 2003) or in ionic.
The geometric parameters associated with dpya and aqua ligands are normal [Lu et al., 2001; Huang et al., 2006]. There are five general crystallographically distinct positions in the unit cell occupied by not coordinated water molecules. Among these two positions (O8 and O9) are partially occupied with s.o.f. put to half as required by proximity of symmetry (-1) related positions of O8 and proximity of the O9 water oxygen to O8, respectively. The water molecules along with the not coordinated oxygen atoms from carboxylate groups are involved in hydrogen bonds of the O—H···O type; some of these HBs are intramolecular (Fig. 2, Table 3). In the hydrogen bonding system is involved also the dpyaligand through N—H···O type hydrogen bond (Fig. 2, Table 3). Between pairs of dpya ligands π–π interactions operate which further stabilize the structure (Fig. 3). The Cg1···Cg2i distance (symmetry code (i) -x, 0.5+y, 0.5-z, where Cg1 and Cg2 are centroids of the rings (N1/C1—C5) and (N2/C6—C10), respectively) between the aromatic rings is 3.723 (1) Å; these interactions links the {Ni(dpya)} units into layers lying in the bc plane.