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In the title compound, [Ni(C12H6O4)(C22H16N2O)2(H2O)2]n, the Ni2+ cation resides on a centre of inversion in a slightly distorted octa­hedral [N2O4] environment. The two carboxyl­ate groups of each naphthalene-2,6-di­carboxyl­ate (NDC2-) ligand, which reside on centres of inversion, link the NiII cations into a one-dimensional chain. Identical chains are linked by inter­molecular hydrogen bonds between coordinated water mol­ecules and the uncoordinated N atoms of 4-{4-[4-(pyridin-4-yl)phen­oxy]phen­yl}pyridine ligands to form (4,4)-topological sheets, and then the different sheets are inter­locked in an inclined fashion to give a three-dimensional polycatenation network. The stability of the structure is further enhanced by [pi]-[pi] stacking inter­actions between pyridine and benzene rings.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S010827011302012X/sf3203sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S010827011302012X/sf3203Isup2.hkl
Contains datablock I

CCDC reference: 965301

Introduction top

Recently, the design and synthesis of metal–organic coordination polymers have attracted muuch inter­est because of their inter­esting structural diversity and special properties, such as porosity, nonlinear optical activity, luminescence, magnetism and catalytic activity, as well as their intriguing variety of architectures and molecular topologies (Ni et al., 2005; Rowsell & Yaghi, 2005; Coronado et al., 2000; Guo et al., 2009). To construct novel coordination polymers, we usually choose carboxyl­ate-containing ligands which have varied coordination modes as the main connectors, and mixed ligands with N-donor groups as ancillary bridges (Deng et al., 2012; Dai et al., 2004; Sun et al., 2003). In the present case, we chose naphthalene-2,6-di­carb­oxy­lic acid (H2NDC) as our main ligand and 4-{4-[4-(pyridin-4-yl)phen­oxy]­phenyl}­pyridine (BPDPE) as the N-donor assistant ligand to synthesize a nickel complex. Compared with the linear bis­(pyridine) ligand, BPDPE is a V-shaped pyridine ligand, which can be regarded as a half-flexible ligand to construct more inter­esting structures (Hu et al., 2012). We report here the synthesis and structure of the title compound, [Ni(NDC)(BPDPE)2(H2O)2]n, (I).

Experimental top

Synthesis and crystallization top

All starting chemicals and solvents used in this synthesis were of reagent quality and purchased from commercial sources without further purification. A mixture of NiCl2.6H2O (48 mg, 0.2 mmol), H2NDC (22 mg, 0.1 mmol), BPDPE (32 mg, 0.1 mmol), DMF (7 ml) and water (7 ml) was placed in a Parr Teflon-lined stainless steel vessel (23 ml), heated to 393 K for 3 d, then cooled to room temperature slowly. Green diamond-like crystals of complex (I) (yield 34 mg, 70%) were collected at the bottom of the glass vessel.

Refinement top

Crystal data, data collection and structure refinement details are summarized in Table 1. H atoms bonded to C atoms were positioned geometrically and treated as riding, with C—H = 0.93 Å, and with Uiso(H) = 1.2Ueq(C). The aqua H atoms were placed so as to form a reasonable hydrogen-bond network, with O—H = 0.85 Å, and were refined as riding, with Uiso(H) = 1.2UUeq(O).

Results and discussion top

Compound (I) crystallizes in the monoclinic space group P21/c, and the asymmetric unit contains half of a central NiII cation, half of a doubly deprotonated H2NDC ligand, a BPDPE ligand and a coordinated water molecule. As shown in Fig. 1, the NiII centre is six-coordinated by two carboxyl­ate O atoms from two NDC2- ligands, two N atoms from two BPDPE ligands and two O atoms from two water molecules to form a slightly distorted o­cta­hedron. The NiII cation resides on a centre of inversion, as does the NDC2- ligand. The two carboxyl­ate groups of each NDC2- ligand coordinate with the NiII cation in a monodentate manner and only one N atom of each BPDPE ligand coordinates with the NiII cation, so a one-dimensional chain structure is formed extending along the c axis, with an Ni···Ni distance within the chain of about 13.653 Å. There are two types of chain which are related by an ac glide and these are arranged alternately, which may reduce repulsion for a greater stabilization of the structure (Fig. 2).

There are inter­molecular O4—H4C···N2i (see Table 2 for details and symmetry code) and intra­molecular O4—H4B···O2ii hydrogen bonds (Table 2) in complex (I). The inter­molecular hydrogen bonds are formed between identical chains, so the same types of chain extend into a (4,4)-topological layered network via these inter­molecular hydrogen bonds (Fig. 3). Because of the spacious nature of the network, it allows the crossed layers to inter­penetrate with each other to form inclined polycatenation networks, which accomplishes the transition from a two-dimensional to a three-dimensional structure for (I) (Fig. 4) (Batten & Robson, 1998). This demonstrates that the uncoordinated N atom and coordinated water molecules can be well used in the synthesis of unusual coordination frameworks (Hu et al., 2012). Additionally, there are weak ππ stacking inter­actions between the nearest C6–C10/N2 pyridine and C11–C16 benzene rings, with an inter­planar distance of 3.68 Å. The dihedral angle α defined by the stacked rings is 12.12° and the slippage angles are β = 20.64 and γ = 17.78° (Fig. 5). This moderate stacking inter­action further enhances the stability of complex (I).

Related literature top

For related literature, see: Batten & Robson (1998); Coronado et al. (2000); Dai et al. (2004); Deng et al. (2012); Guo et al. (2009); Hu et al. (2012); Ni et al. (2005); Rowsell & Yaghi (2005); Sun et al. (2003).

Computing details top

Data collection: APEX2 (Bruker, 2003); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT (Bruker, 2003); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
Fig. 1. The structure of (I), with displacement ellipsoids drawn at the 30% probability level. All H atoms have been omitted for clarity. [Symmetry codes: (i) -x + 3, -y + 1, -z + 2; (ii) x, y, z.]

Fig. 2. The two types of one-dimensional chain structure of (I), extending along the c axis.

Fig. 3. A view of the two-dimensional supramolecular layer stacked via intermolecular O—H···N hydrogen bonds (dashed lines). Different layers are shown in different colours and intramolecular hydrogen bonds have been omitted for clarity.

Fig. 4. (a) The three-dimensional network formed by the interlocking interaction in complex (I). (b) A space-filling model, showing the inclined interpenetration between the layers.

Fig. 5. The ππ stacking interactions in (I), shown as thin solid lines (light green in the electronic version of the journal). Dashed lines indicate intermolecular hydrogen bonds.
catena-Poly[[diaquabis(4-{4-[4-(pyridin-4-yl)phenoxy]phenyl}pyridine)nickel(II)]-µ2-naphthalene-2,6-dicarboxylato] top
Crystal data top
[Ni(C12H6O4)(C22H16N2O)2(H2O)2]F(000) = 996
Mr = 957.65Dx = 1.418 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2556 reflections
a = 11.4739 (6) Åθ = 3.0–28.6°
b = 15.9431 (7) ŵ = 0.50 mm1
c = 13.4291 (8) ÅT = 290 K
β = 114.048 (7)°Diamond-like, green
V = 2243.4 (2) Å30.21 × 0.19 × 0.15 mm
Z = 2
Data collection top
Bruker APEXII CCD area-detector
diffractometer
4407 independent reflections
Radiation source: fine-focus sealed tube3337 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
ϕ and ω scansθmax = 26.0°, θmin = 3.1°
Absorption correction: multi-scan
(SADABS; Bruker, 2003)
h = 1114
Tmin = 0.890, Tmax = 0.916k = 1912
9294 measured reflectionsl = 1616
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.124H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0526P)2 + 0.4401P]
where P = (Fo2 + 2Fc2)/3
4407 reflections(Δ/σ)max < 0.001
313 parametersΔρmax = 0.47 e Å3
1 restraintΔρmin = 0.36 e Å3
Crystal data top
[Ni(C12H6O4)(C22H16N2O)2(H2O)2]V = 2243.4 (2) Å3
Mr = 957.65Z = 2
Monoclinic, P21/cMo Kα radiation
a = 11.4739 (6) ŵ = 0.50 mm1
b = 15.9431 (7) ÅT = 290 K
c = 13.4291 (8) Å0.21 × 0.19 × 0.15 mm
β = 114.048 (7)°
Data collection top
Bruker APEXII CCD area-detector
diffractometer
4407 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2003)
3337 reflections with I > 2σ(I)
Tmin = 0.890, Tmax = 0.916Rint = 0.033
9294 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0471 restraint
wR(F2) = 0.124H-atom parameters constrained
S = 1.07Δρmax = 0.47 e Å3
4407 reflectionsΔρmin = 0.36 e Å3
313 parameters
Special details top

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) top
xyzUiso*/Ueq
C281.5548 (2)0.39910 (19)1.0747 (2)0.0480 (7)
H281.53100.34291.06780.058*
C10.8999 (2)0.63210 (17)0.6008 (2)0.0411 (7)
H10.98340.65090.62270.049*
C20.8213 (2)0.67478 (17)0.6381 (2)0.0431 (7)
H20.85160.72170.68220.052*
C30.6972 (2)0.64781 (17)0.6097 (2)0.0385 (6)
C40.6583 (2)0.58020 (18)0.5387 (2)0.0443 (7)
H40.57490.56060.51460.053*
C50.7424 (2)0.54190 (18)0.5035 (2)0.0425 (7)
H50.71300.49730.45500.051*
C60.0121 (4)1.1782 (2)0.4638 (3)0.0695 (10)
H60.02041.20300.40440.083*
C70.0923 (3)1.11316 (19)0.5138 (3)0.0617 (9)
H70.15421.09670.48970.074*
C80.0816 (2)1.07171 (17)0.6006 (2)0.0424 (7)
C90.0189 (3)1.0983 (2)0.6247 (3)0.0547 (8)
H90.03701.07060.67780.066*
C100.0921 (3)1.1658 (2)0.5700 (3)0.0655 (9)
H100.15801.18220.58920.079*
C110.1694 (3)1.00347 (17)0.6605 (2)0.0428 (7)
C120.1460 (3)0.95092 (19)0.7323 (3)0.0509 (8)
H120.07510.96110.74760.061*
C130.2241 (3)0.8842 (2)0.7818 (3)0.0534 (8)
H130.20660.85000.83010.064*
C140.3280 (3)0.8685 (2)0.7589 (3)0.0542 (8)
C150.3585 (3)0.9217 (2)0.6946 (3)0.0783 (12)
H150.43230.91280.68320.094*
C160.2804 (3)0.9890 (2)0.6458 (3)0.0659 (10)
H160.30271.02530.60220.079*
C170.4718 (3)0.7634 (2)0.7554 (3)0.0575 (9)
C180.4114 (3)0.7278 (3)0.6543 (3)0.0680 (10)
H180.32290.72920.61860.082*
C190.4837 (3)0.6898 (2)0.6058 (3)0.0584 (9)
H190.44330.66550.53730.070*
C200.6160 (2)0.68767 (17)0.6584 (2)0.0419 (7)
C210.6722 (3)0.7247 (2)0.7604 (3)0.0536 (8)
H210.76070.72440.79690.064*
C220.6007 (3)0.7619 (2)0.8091 (3)0.0589 (9)
H220.64030.78570.87800.071*
C231.1790 (2)0.46317 (19)0.7315 (2)0.0367 (6)
C241.3388 (3)0.5745 (2)0.8383 (2)0.0490 (7)
H241.29180.61300.78510.059*
C251.2988 (2)0.49020 (17)0.8275 (2)0.0370 (6)
C261.3672 (2)0.43308 (19)0.9036 (2)0.0404 (7)
H261.34020.37750.89640.048*
C271.4817 (2)0.45770 (17)0.9958 (2)0.0358 (6)
N10.86374 (18)0.56559 (13)0.53535 (17)0.0336 (5)
N20.0763 (3)1.20860 (17)0.4932 (3)0.0668 (8)
Ni11.00000.50000.50000.02874 (15)
O11.13149 (16)0.51694 (11)0.65671 (14)0.0400 (5)
O21.13494 (17)0.39159 (13)0.73173 (16)0.0546 (6)
O30.4003 (2)0.79838 (16)0.8081 (2)0.0760 (7)
O41.06571 (15)0.61064 (11)0.45375 (14)0.0367 (4)
H4B1.00460.63330.40070.055*
H4C1.09280.64430.50750.055*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C280.0459 (16)0.0455 (17)0.0403 (16)0.0010 (13)0.0049 (14)0.0079 (14)
C10.0352 (13)0.0425 (16)0.0482 (17)0.0030 (12)0.0198 (13)0.0075 (14)
C20.0447 (15)0.0416 (16)0.0481 (17)0.0005 (13)0.0240 (13)0.0116 (14)
C30.0376 (14)0.0380 (15)0.0436 (16)0.0077 (12)0.0204 (12)0.0066 (13)
C40.0309 (13)0.0478 (17)0.0555 (18)0.0000 (12)0.0191 (13)0.0042 (15)
C50.0364 (14)0.0403 (16)0.0489 (17)0.0012 (12)0.0154 (13)0.0092 (14)
C60.093 (3)0.043 (2)0.079 (3)0.0029 (18)0.043 (2)0.0121 (19)
C70.074 (2)0.0441 (18)0.080 (2)0.0038 (17)0.044 (2)0.0067 (17)
C80.0486 (15)0.0336 (15)0.0476 (16)0.0018 (13)0.0223 (14)0.0058 (13)
C90.0561 (18)0.0548 (19)0.060 (2)0.0116 (15)0.0304 (16)0.0089 (17)
C100.059 (2)0.065 (2)0.074 (2)0.0168 (17)0.0296 (18)0.002 (2)
C110.0452 (15)0.0447 (17)0.0460 (16)0.0004 (13)0.0262 (14)0.0047 (14)
C120.0531 (17)0.0533 (19)0.061 (2)0.0113 (15)0.0385 (16)0.0069 (16)
C130.0626 (18)0.0569 (19)0.0592 (19)0.0153 (16)0.0436 (16)0.0139 (16)
C140.0595 (18)0.062 (2)0.0543 (19)0.0247 (16)0.0367 (16)0.0131 (16)
C150.069 (2)0.096 (3)0.100 (3)0.037 (2)0.065 (2)0.042 (2)
C160.069 (2)0.069 (2)0.083 (3)0.0189 (18)0.055 (2)0.032 (2)
C170.068 (2)0.063 (2)0.059 (2)0.0332 (17)0.0448 (18)0.0241 (18)
C180.0458 (17)0.104 (3)0.060 (2)0.0281 (18)0.0269 (16)0.019 (2)
C190.0460 (16)0.083 (2)0.0492 (18)0.0143 (16)0.0223 (15)0.0039 (17)
C200.0420 (14)0.0430 (16)0.0468 (16)0.0104 (12)0.0243 (13)0.0091 (14)
C210.0517 (17)0.059 (2)0.0564 (19)0.0122 (15)0.0281 (15)0.0023 (16)
C220.067 (2)0.065 (2)0.0545 (19)0.0170 (17)0.0347 (17)0.0015 (17)
C230.0268 (12)0.0522 (17)0.0283 (14)0.0042 (12)0.0083 (11)0.0057 (13)
C240.0413 (15)0.0576 (19)0.0366 (16)0.0002 (14)0.0040 (13)0.0029 (15)
C250.0290 (12)0.0524 (18)0.0273 (13)0.0067 (12)0.0090 (11)0.0004 (13)
C260.0345 (14)0.0527 (18)0.0322 (14)0.0019 (13)0.0119 (12)0.0013 (13)
C270.0335 (13)0.0438 (15)0.0317 (14)0.0045 (12)0.0148 (12)0.0026 (13)
N10.0334 (11)0.0330 (12)0.0353 (12)0.0023 (9)0.0150 (9)0.0028 (10)
N20.083 (2)0.0403 (15)0.079 (2)0.0101 (15)0.0359 (17)0.0057 (15)
Ni10.0261 (2)0.0321 (3)0.0248 (2)0.00333 (18)0.00703 (18)0.0026 (2)
O10.0354 (9)0.0456 (11)0.0282 (10)0.0038 (8)0.0019 (8)0.0036 (9)
O20.0451 (11)0.0585 (14)0.0413 (12)0.0046 (10)0.0017 (9)0.0076 (11)
O30.0946 (16)0.0898 (18)0.0713 (16)0.0552 (14)0.0623 (14)0.0368 (14)
O40.0338 (9)0.0397 (10)0.0320 (10)0.0017 (8)0.0088 (8)0.0001 (8)
Geometric parameters (Å, º) top
C28—C24i1.368 (4)C15—C161.381 (4)
C28—C271.405 (4)C15—H150.9300
C28—H280.9300C16—H160.9300
C1—N11.331 (3)C17—C221.357 (4)
C1—C21.375 (4)C17—C181.370 (5)
C1—H10.9300C17—O31.400 (3)
C2—C31.385 (4)C18—C191.385 (4)
C2—H20.9300C18—H180.9300
C3—C41.387 (4)C19—C201.390 (4)
C3—C201.481 (4)C19—H190.9300
C4—C51.378 (4)C20—C211.386 (4)
C4—H40.9300C21—C221.374 (4)
C5—N11.334 (3)C21—H210.9300
C5—H50.9300C22—H220.9300
C6—N21.321 (4)C23—O21.249 (3)
C6—C71.367 (4)C23—O11.263 (3)
C6—H60.9300C23—C251.514 (4)
C7—C81.388 (4)C24—C28i1.368 (4)
C7—H70.9300C24—C251.408 (4)
C8—C91.386 (4)C24—H240.9300
C8—C111.478 (4)C25—C261.355 (4)
C9—C101.378 (4)C26—C271.445 (3)
C9—H90.9300C26—H260.9300
C10—N21.311 (4)C27—C27i1.403 (5)
C10—H100.9300N1—Ni12.0900 (19)
C11—C121.384 (4)Ni1—O12.0470 (17)
C11—C161.385 (4)Ni1—O1ii2.0470 (17)
C12—C131.376 (4)Ni1—N1ii2.0900 (19)
C12—H120.9300Ni1—O4ii2.1089 (17)
C13—C141.369 (4)Ni1—O42.1089 (17)
C13—H130.9300O4—H4B0.8500
C14—C151.354 (4)O4—H4C0.8501
C14—O31.389 (4)
C24i—C28—C27119.3 (3)C17—C18—C19119.3 (3)
C24i—C28—H28120.3C17—C18—H18120.4
C27—C28—H28120.3C19—C18—H18120.4
N1—C1—C2124.1 (2)C18—C19—C20120.8 (3)
N1—C1—H1118.0C18—C19—H19119.6
C2—C1—H1118.0C20—C19—H19119.6
C1—C2—C3120.0 (3)C21—C20—C19117.6 (3)
C1—C2—H2120.0C21—C20—C3119.7 (2)
C3—C2—H2120.0C19—C20—C3122.6 (3)
C2—C3—C4115.9 (2)C22—C21—C20121.8 (3)
C2—C3—C20120.4 (3)C22—C21—H21119.1
C4—C3—C20123.6 (2)C20—C21—H21119.1
C5—C4—C3120.4 (2)C17—C22—C21119.2 (3)
C5—C4—H4119.8C17—C22—H22120.4
C3—C4—H4119.8C21—C22—H22120.4
N1—C5—C4123.4 (3)O2—C23—O1125.3 (2)
N1—C5—H5118.3O2—C23—C25119.0 (2)
C4—C5—H5118.3O1—C23—C25115.6 (3)
N2—C6—C7125.3 (4)C28i—C24—C25121.5 (3)
N2—C6—H6117.4C28i—C24—H24119.3
C7—C6—H6117.4C25—C24—H24119.3
C6—C7—C8120.0 (3)C26—C25—C24120.0 (2)
C6—C7—H7120.0C26—C25—C23119.8 (3)
C8—C7—H7120.0C24—C25—C23120.3 (2)
C9—C8—C7114.7 (3)C25—C26—C27120.6 (3)
C9—C8—C11123.1 (3)C25—C26—H26119.7
C7—C8—C11122.2 (3)C27—C26—H26119.7
C10—C9—C8119.9 (3)C27i—C27—C28120.8 (3)
C10—C9—H9120.0C27i—C27—C26117.9 (3)
C8—C9—H9120.0C28—C27—C26121.3 (3)
N2—C10—C9125.2 (3)C1—N1—C5116.2 (2)
N2—C10—H10117.4C1—N1—Ni1119.22 (16)
C9—C10—H10117.4C5—N1—Ni1124.43 (18)
C12—C11—C16116.7 (3)C10—N2—C6114.4 (3)
C12—C11—C8122.8 (2)O1—Ni1—O1ii180.0
C16—C11—C8120.5 (3)O1—Ni1—N190.38 (8)
C13—C12—C11122.1 (3)O1ii—Ni1—N189.62 (8)
C13—C12—H12119.0O1—Ni1—N1ii89.62 (8)
C11—C12—H12119.0O1ii—Ni1—N1ii90.38 (8)
C14—C13—C12119.2 (3)N1—Ni1—N1ii180.00 (6)
C14—C13—H13120.4O1—Ni1—O4ii90.56 (7)
C12—C13—H13120.4O1ii—Ni1—O4ii89.44 (7)
C15—C14—C13120.3 (3)N1—Ni1—O4ii87.78 (7)
C15—C14—O3123.2 (3)N1ii—Ni1—O4ii92.22 (7)
C13—C14—O3116.5 (3)O1—Ni1—O489.44 (7)
C14—C15—C16120.2 (3)O1ii—Ni1—O490.56 (7)
C14—C15—H15119.9N1—Ni1—O492.22 (7)
C16—C15—H15119.9N1ii—Ni1—O487.78 (7)
C15—C16—C11121.2 (3)O4ii—Ni1—O4180.0
C15—C16—H16119.4C23—O1—Ni1128.79 (18)
C11—C16—H16119.4C14—O3—C17116.1 (2)
C22—C17—C18121.4 (3)Ni1—O4—H4B109.3
C22—C17—O3118.4 (3)Ni1—O4—H4C109.2
C18—C17—O3120.2 (3)H4B—O4—H4C109.5
N1—C1—C2—C31.6 (5)O3—C17—C22—C21177.4 (3)
C1—C2—C3—C43.5 (4)C20—C21—C22—C170.8 (5)
C1—C2—C3—C20173.6 (3)C28i—C24—C25—C260.9 (4)
C2—C3—C4—C52.3 (4)C28i—C24—C25—C23178.8 (3)
C20—C3—C4—C5174.6 (3)O2—C23—C25—C2610.2 (4)
C3—C4—C5—N10.9 (5)O1—C23—C25—C26170.2 (2)
N2—C6—C7—C82.2 (6)O2—C23—C25—C24169.5 (3)
C6—C7—C8—C93.9 (5)O1—C23—C25—C2410.2 (4)
C6—C7—C8—C11177.3 (3)C24—C25—C26—C270.4 (4)
C7—C8—C9—C105.3 (4)C23—C25—C26—C27180.0 (2)
C11—C8—C9—C10176.0 (3)C24i—C28—C27—C27i1.3 (5)
C8—C9—C10—N20.8 (5)C24i—C28—C27—C26178.8 (3)
C9—C8—C11—C1211.6 (4)C25—C26—C27—C27i0.8 (4)
C7—C8—C11—C12167.1 (3)C25—C26—C27—C28179.1 (3)
C9—C8—C11—C16169.0 (3)C2—C1—N1—C51.7 (4)
C7—C8—C11—C1612.4 (5)C2—C1—N1—Ni1173.3 (2)
C16—C11—C12—C134.0 (5)C4—C5—N1—C12.9 (4)
C8—C11—C12—C13175.5 (3)C4—C5—N1—Ni1171.8 (2)
C11—C12—C13—C140.5 (5)C9—C10—N2—C65.1 (5)
C12—C13—C14—C154.7 (5)C7—C6—N2—C106.7 (5)
C12—C13—C14—O3177.6 (3)C1—N1—Ni1—O138.0 (2)
C13—C14—C15—C164.2 (6)C5—N1—Ni1—O1136.6 (2)
O3—C14—C15—C16178.3 (4)C1—N1—Ni1—O1ii142.0 (2)
C14—C15—C16—C110.5 (6)C5—N1—Ni1—O1ii43.4 (2)
C12—C11—C16—C154.5 (5)C1—N1—Ni1—O4ii128.5 (2)
C8—C11—C16—C15175.0 (3)C5—N1—Ni1—O4ii46.0 (2)
C22—C17—C18—C190.2 (5)C1—N1—Ni1—O451.5 (2)
O3—C17—C18—C19176.8 (3)C5—N1—Ni1—O4134.0 (2)
C17—C18—C19—C200.2 (5)O2—C23—O1—Ni116.5 (4)
C18—C19—C20—C210.0 (5)C25—C23—O1—Ni1163.91 (16)
C18—C19—C20—C3180.0 (3)N1—Ni1—O1—C23110.7 (2)
C2—C3—C20—C2126.9 (4)N1ii—Ni1—O1—C2369.3 (2)
C4—C3—C20—C21149.9 (3)O4ii—Ni1—O1—C2322.9 (2)
C2—C3—C20—C19153.1 (3)O4—Ni1—O1—C23157.1 (2)
C4—C3—C20—C1930.1 (4)C15—C14—O3—C1726.7 (5)
C19—C20—C21—C220.5 (5)C13—C14—O3—C17155.7 (3)
C3—C20—C21—C22179.5 (3)C22—C17—O3—C14117.8 (3)
C18—C17—C22—C210.7 (5)C18—C17—O3—C1465.4 (4)
Symmetry codes: (i) x+3, y+1, z+2; (ii) x+2, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O4—H4C···N2iii0.852.352.959 (3)129
O4—H4B···O2ii0.851.892.614 (2)143
Symmetry codes: (ii) x+2, y+1, z+1; (iii) x+1, y+2, z+1.

Experimental details

Crystal data
Chemical formula[Ni(C12H6O4)(C22H16N2O)2(H2O)2]
Mr957.65
Crystal system, space groupMonoclinic, P21/c
Temperature (K)290
a, b, c (Å)11.4739 (6), 15.9431 (7), 13.4291 (8)
β (°) 114.048 (7)
V3)2243.4 (2)
Z2
Radiation typeMo Kα
µ (mm1)0.50
Crystal size (mm)0.21 × 0.19 × 0.15
Data collection
DiffractometerBruker APEXII CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2003)
Tmin, Tmax0.890, 0.916
No. of measured, independent and
observed [I > 2σ(I)] reflections
9294, 4407, 3337
Rint0.033
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.124, 1.07
No. of reflections4407
No. of parameters313
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.47, 0.36

Computer programs: APEX2 (Bruker, 2003), SAINT (Bruker, 2003), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O4—H4C···N2i0.852.352.959 (3)128.7
O4—H4B···O2ii0.851.892.614 (2)142.5
Symmetry codes: (i) x+1, y+2, z+1; (ii) x+2, y+1, z+1.
 

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