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In the title compound, [Ni2(C12H8O12)(C12H8N2)2]n, the 3,6-dicarboxy­cyclo­hexane-1,2,4,5-tetra­carboxyl­ate (H2chhc4−) anion has crystallographically imposed C2 symmetry and bridges the six-coordinate Ni atoms to generate polymeric _\infty^{\,\,\,1}[Ni2(H2chhc)2/2(C12H8N2)2] chains extending in the [010] direction. The coordination polymer chains are linked into a three-dimensional framework by O—H...O and C—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270106032495/gd3041sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270106032495/gd3041Isup2.hkl
Contains datablock I

CCDC reference: 625668

Comment top

In recent years, metal-organic coordination polymers have been attracting more and more attention owing to their potential application in many fields (Moulton & Zaworotko, 2001; MacGillivray et al., 1998). It is well known that the aromatic carboxylic acids, such as terephthalic acid (Chen et al., 2003), benzene-1,3,5-tricarboxylic acid (Chui et al., 1999), benzene-1,2,4,5- tetracarboxylic acid (Murugavel et al., 2002) and mellitic acid (Ranganathan et al., 2001), exhibit a variety of bridging modes and coordination fashions and have been widely used to construct coordination polymers with specific network topologies and interesting properties. Because of their greater conformational flexibility, the aliphatic carboxylic acids have also aroused much attention in the field of synthesis of coordination polymers (Zheng et al., 2004; Zheng & Kong, 2002). Comparably few naphthenic polycarboxylic acids have been explored as ligands for the construction of coordination polymers (Bi et al., 2003; Myunghyun et al., 2003; Kil & Myunghyun, 2001). In the present contribution, we report a new nickel coordination polymer, [Ni2(C12H8N2)2(H2chhc)], (I), resulting from self-assembly of Ni2+ ions, phenanthroline (phen) and a tetra-anion derived from 1,2,3,4,5,6-cyclohexanehexacarboxylic acid (H6chhc).

The asymmetric unit of the title compound consists of one Ni2+ cation, one phen ligand and one-half of a H2chhc4− anion lying across a twofold rotation axis. The Ni atoms are each in a distorted octahedral environment defined by four O atoms of two carboxylate groups from different H2chhc4− anions and two N atoms of one phen ligand. The Ni—N bond distances are 2.050 (2) Å and 2.056 (2) Å, respectively, and the Ni—O bond distances vary from 2.084 (2) Å to 2.118 (2) Å. Obviously, such bonding values fall in the normal region (Zheng et al., 2002). The H2chhc4− anions display a stable chair conformation with the two opposite carboxyl groups and four carboxylate groups orientating equatorially, similar to those reported in the literature (Bi et al., 2003; Myunghyun et al., 2003; Kil & Myunghyun, 2001). Each carboxylate group of the H2chhc4− anion chelates one Ni atom; as a result, the H2chhc4− anions are each coordinated to four [Ni(phen)]2+ units, leading to polymeric chains formulated as 1[Ni2(C12H8N2)2/2] running along the [010] direction with the phen ligands exo-orientated, as shown in Fig. 1. On the basis of the interchain C—H···O hydrogen bonds (Table 1) these chains are assembled into layers parallel to (101) (Fig. 2). The layers are further connected to form a three-dimensional framework via strong interlayer O—H···O hydrogen bonds and weak interchain C—H···O hydrogen bonds. The H2chhc4− anions exhibit the normal C—O bond distances (Kil & Myunghyun, 2001).

Experimental top

The Ni(OH)2.xH2O precipitate deposited from dropwise addition of 1 M NaOH (3.0 ml) to a stirred aqueous solution of NiCl2·6H2O (0.24 g, 1.0 mmol, in 7.0 ml H2O), followed by separation by centrifugation and washing with distilled water several times until no detectable Cl anions remained in the supernatant. Subsequently, the precipitate was added to a stirred aqueous solution of H6chhc (0.17 g, 0.50 mmol) and 1,10-phenanthroline monohydrate (0.20 g, 1.0 mmol) in water (20.0 ml). The resulting mixture was further stirred for ca 30 minutes and then filtered. The green filtrate was allowed to stand at room temperature. Slow evaporation for several days afforded green plate-like crystals (yield ca 20% based on the initial NiCl2·6H2O input).

Refinement top

Compound (I) is monoclinic; space group C2/c was assumed and comfirmed by the analysis. H atoms attached to C atoms were placed in calculated positions and refined using a riding model [C—H = 0.93 or 0.98 Å, and Uiso(H) = 1.2Ueq(C)], while the H atom on atom O3 was observed in a difference Fourier map and was refined freely [O—H = 0.86 (4) Å].

Computing details top

Data collection: XSCANS (Siemens, 1996); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A fragment of the one-dimensional 1[Ni2(phen)2(H2chhc)2/2] polymeric chain. Displacement ellipsoids are drawn at the 45% probability level. H atoms have been omitted.
[Figure 2] Fig. 2. The two-dimensional supramolecular layer in (I) parallel to (101). Hydrogen bonds are indicated by dashed lines.
[Figure 3] Fig. 3. The packing of (I). Hydrogen bonds are indicated by dashed lines.
catena-Poly-[bis[(1,10-phenanthroline)nickel(II)]-µ- 3,6-dicarboxycyclohexane-1,2,4,5-tetracarboxylato] top
Crystal data top
[Ni2(C12H8O12)(C12H8N2)2]F(000) = 1680
Mr = 411.01Dx = 1.692 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 25 reflections
a = 22.018 (4) Åθ = 10–25°
b = 8.9600 (18) ŵ = 1.24 mm1
c = 16.371 (3) ÅT = 298 K
β = 92.49 (3)°Plate, green
V = 3226.6 (11) Å30.31 × 0.22 × 0.11 mm
Z = 8
Data collection top
Bruker P4
diffractometer
2959 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.030
Graphite monochromatorθmax = 27.5°, θmin = 1.9°
ω/2θ scansh = 128
Absorption correction: ψ scan
(North et al., 1968)
k = 111
Tmin = 0.727, Tmax = 0.872l = 2121
4519 measured reflections3 standard reflections every 97 reflections
3715 independent reflections intensity decay: none
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.087 w = 1/[σ2(Fo2) + (0.0381P)2 + 3.2579P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.001
3715 reflectionsΔρmax = 0.34 e Å3
250 parametersΔρmin = 0.29 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.38
Crystal data top
[Ni2(C12H8O12)(C12H8N2)2]V = 3226.6 (11) Å3
Mr = 411.01Z = 8
Monoclinic, C2/cMo Kα radiation
a = 22.018 (4) ŵ = 1.24 mm1
b = 8.9600 (18) ÅT = 298 K
c = 16.371 (3) Å0.31 × 0.22 × 0.11 mm
β = 92.49 (3)°
Data collection top
Bruker P4
diffractometer
2959 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.030
Tmin = 0.727, Tmax = 0.8723 standard reflections every 97 reflections
4519 measured reflections intensity decay: none
3715 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0360 restraints
wR(F2) = 0.087H atoms treated by a mixture of independent and constrained refinement
S = 1.01Δρmax = 0.34 e Å3
3715 reflectionsΔρmin = 0.29 e Å3
250 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
Ni0.902824 (12)0.35453 (3)0.857256 (16)0.01903 (10)
N10.81335 (9)0.2954 (2)0.83859 (12)0.0295 (4)
N20.86862 (9)0.4467 (2)0.96070 (11)0.0255 (4)
O10.94713 (8)0.15587 (18)0.89271 (9)0.0281 (4)
O20.93194 (8)0.21155 (19)0.76394 (9)0.0279 (4)
O31.01924 (8)0.1440 (2)0.95146 (10)0.0364 (4)
O40.91851 (9)0.1705 (2)0.95658 (11)0.0421 (5)
O50.90510 (7)0.44072 (18)0.79280 (10)0.0256 (3)
O60.98354 (7)0.52381 (17)0.86585 (9)0.0246 (3)
C10.78741 (13)0.2137 (4)0.77850 (17)0.0433 (7)
H10.81200.16700.74140.052*
C20.72423 (15)0.1962 (5)0.7695 (2)0.0590 (10)
H20.70730.13880.72710.071*
C30.68809 (13)0.2636 (5)0.8231 (2)0.0597 (10)
H30.64610.25240.81730.072*
C40.71318 (12)0.3502 (4)0.88740 (19)0.0470 (7)
C50.67951 (13)0.4271 (5)0.9478 (2)0.0634 (10)
H50.63730.42210.94480.076*
C60.70726 (15)0.5060 (5)1.0085 (2)0.0628 (10)
H60.68390.55561.04600.075*
C70.77247 (13)0.5151 (4)1.01667 (18)0.0438 (7)
C80.80477 (16)0.5896 (4)1.08044 (19)0.0540 (8)
H80.78380.63941.12030.065*
C90.86665 (15)0.5892 (4)1.08413 (17)0.0473 (7)
H90.88820.63601.12700.057*
C100.89725 (12)0.5168 (3)1.02188 (15)0.0329 (6)
H100.93950.51831.02390.039*
C110.80676 (10)0.4441 (3)0.95836 (14)0.0294 (5)
C120.77736 (10)0.3608 (3)0.89305 (15)0.0319 (5)
C130.95634 (10)0.1295 (2)0.81794 (13)0.0220 (4)
C140.99478 (10)0.0044 (2)0.79603 (13)0.0204 (4)
H141.03440.00460.82530.024*
C150.96382 (9)0.1480 (2)0.82531 (13)0.0199 (4)
H150.92170.14930.80320.024*
C160.96322 (11)0.1532 (3)0.91831 (14)0.0250 (5)
C170.99619 (9)0.2900 (2)0.79650 (12)0.0191 (4)
H171.03650.29540.82410.023*
C180.95958 (9)0.4275 (2)0.81973 (12)0.0197 (4)
H3A1.0186 (17)0.148 (4)1.004 (2)0.071 (12)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni0.01956 (14)0.01605 (15)0.02151 (15)0.00066 (12)0.00102 (10)0.00012 (12)
N10.0278 (10)0.0308 (11)0.0296 (10)0.0075 (9)0.0013 (8)0.0036 (9)
N20.0251 (9)0.0258 (10)0.0258 (9)0.0004 (8)0.0028 (7)0.0001 (8)
O10.0426 (9)0.0212 (8)0.0207 (7)0.0064 (7)0.0032 (7)0.0005 (7)
O20.0374 (9)0.0242 (8)0.0222 (8)0.0071 (7)0.0018 (7)0.0009 (7)
O30.0387 (10)0.0494 (12)0.0209 (8)0.0039 (9)0.0014 (7)0.0004 (9)
O40.0444 (11)0.0453 (12)0.0381 (10)0.0014 (9)0.0201 (8)0.0016 (9)
O50.0230 (8)0.0216 (8)0.0318 (8)0.0000 (7)0.0042 (6)0.0054 (7)
O60.0240 (8)0.0190 (8)0.0305 (8)0.0014 (6)0.0031 (6)0.0064 (7)
C10.0442 (15)0.0444 (17)0.0406 (14)0.0171 (14)0.0072 (12)0.0021 (13)
C20.0505 (19)0.074 (2)0.0510 (18)0.0301 (18)0.0175 (15)0.0028 (18)
C30.0263 (14)0.084 (3)0.068 (2)0.0197 (16)0.0137 (14)0.018 (2)
C40.0237 (12)0.062 (2)0.0551 (17)0.0061 (14)0.0014 (12)0.0182 (16)
C50.0231 (13)0.089 (3)0.079 (2)0.0087 (17)0.0141 (15)0.017 (2)
C60.0384 (17)0.083 (3)0.069 (2)0.0192 (18)0.0263 (16)0.004 (2)
C70.0395 (15)0.0490 (18)0.0444 (15)0.0088 (13)0.0177 (12)0.0030 (14)
C80.065 (2)0.056 (2)0.0430 (16)0.0114 (17)0.0211 (15)0.0141 (16)
C90.065 (2)0.0473 (17)0.0300 (13)0.0022 (16)0.0042 (13)0.0126 (13)
C100.0336 (13)0.0355 (14)0.0293 (12)0.0011 (11)0.0019 (10)0.0018 (11)
C110.0245 (11)0.0321 (14)0.0317 (12)0.0033 (10)0.0036 (9)0.0053 (11)
C120.0218 (11)0.0368 (14)0.0370 (13)0.0031 (11)0.0004 (9)0.0073 (12)
C130.0293 (11)0.0137 (10)0.0234 (10)0.0027 (9)0.0043 (9)0.0005 (9)
C140.0239 (11)0.0163 (10)0.0210 (10)0.0005 (9)0.0026 (8)0.0009 (8)
C150.0209 (10)0.0161 (10)0.0227 (10)0.0009 (9)0.0018 (8)0.0005 (9)
C160.0326 (12)0.0155 (10)0.0273 (11)0.0017 (10)0.0052 (9)0.0010 (9)
C170.0211 (10)0.0150 (10)0.0213 (10)0.0003 (8)0.0004 (8)0.0006 (9)
C180.0217 (10)0.0174 (10)0.0202 (10)0.0003 (9)0.0035 (8)0.0022 (9)
Geometric parameters (Å, º) top
Ni—N12.050 (2)C4—C121.415 (3)
Ni—N22.0561 (19)C4—C51.437 (5)
Ni—O6i2.0843 (16)C5—C61.346 (5)
Ni—O12.0994 (17)C5—H50.9300
Ni—O22.1146 (16)C6—C71.438 (4)
Ni—O5i2.1181 (16)C6—H60.9300
Ni—C18i2.412 (2)C7—C111.396 (4)
Ni—C132.436 (2)C7—C81.406 (5)
N1—C11.334 (3)C8—C91.361 (5)
N1—C121.352 (3)C8—H80.9300
N2—C101.319 (3)C9—C101.405 (4)
N2—C111.361 (3)C9—H90.9300
O1—C131.272 (3)C10—H100.9300
O2—C131.253 (3)C11—C121.435 (4)
O3—C161.328 (3)C13—C141.520 (3)
O3—H3A0.86 (4)C14—C14ii1.534 (4)
O4—C161.200 (3)C14—C151.542 (3)
O5—C181.265 (3)C14—H140.9800
O6—C181.248 (3)C15—C161.524 (3)
C1—C21.401 (4)C15—C171.542 (3)
C1—H10.9300C15—H150.9800
C2—C31.352 (5)C17—C181.530 (3)
C2—H20.9300C17—C17ii1.539 (4)
C3—C41.401 (5)C17—H170.9800
C3—H30.9300C18—Niiii2.412 (2)
N1—Ni—N280.95 (8)C8—C7—C6124.5 (3)
N1—Ni—O6i162.99 (8)C9—C8—C7120.3 (3)
N2—Ni—O6i94.36 (7)C9—C8—H8119.8
N1—Ni—O1104.71 (8)C7—C8—H8119.8
N2—Ni—O1107.17 (7)C8—C9—C10118.7 (3)
O6i—Ni—O192.30 (7)C8—C9—H9120.7
N1—Ni—O293.17 (8)C10—C9—H9120.7
N2—Ni—O2166.35 (7)N2—C10—C9122.8 (3)
O6i—Ni—O294.66 (7)N2—C10—H10118.6
O1—Ni—O262.24 (6)C9—C10—H10118.6
N1—Ni—O5i101.13 (7)N2—C11—C7122.9 (2)
N2—Ni—O5i94.59 (7)N2—C11—C12116.6 (2)
O6i—Ni—O5i62.75 (6)C7—C11—C12120.4 (2)
O1—Ni—O5i148.35 (6)N1—C12—C4122.7 (3)
O2—Ni—O5i98.65 (6)N1—C12—C11117.3 (2)
N1—Ni—C13102.66 (8)C4—C12—C11120.0 (2)
C1—N1—C12118.7 (2)O2—C13—O1119.2 (2)
C1—N1—Ni129.01 (19)O2—C13—C14121.52 (19)
C12—N1—Ni112.12 (16)O1—C13—C14119.19 (19)
C10—N2—C11118.3 (2)O2—C13—Ni60.20 (11)
C10—N2—Ni129.54 (17)O1—C13—Ni59.50 (11)
C11—N2—Ni111.83 (16)C14—C13—Ni175.05 (16)
C13—O1—Ni89.04 (13)C13—C14—C14ii109.91 (16)
C13—O2—Ni88.86 (13)C13—C14—C15109.07 (17)
C16—O3—H3A110 (2)C14ii—C14—C15113.12 (14)
C18—O5—Niiii87.13 (13)C13—C14—H14108.2
C18—O6—Niiii89.08 (13)C14ii—C14—H14108.2
N1—C1—C2122.0 (3)C15—C14—H14108.2
N1—C1—H1119.0C16—C15—C14111.08 (18)
C2—C1—H1119.0C16—C15—C17107.71 (17)
C3—C2—C1119.5 (3)C14—C15—C17112.13 (16)
C3—C2—H2120.3C16—C15—H15108.6
C1—C2—H2120.3C14—C15—H15108.6
C2—C3—C4120.7 (3)C17—C15—H15108.6
C2—C3—H3119.7O4—C16—O3124.3 (2)
C4—C3—H3119.7O4—C16—C15124.7 (2)
C3—C4—C12116.5 (3)O3—C16—C15110.98 (19)
C3—C4—C5125.7 (3)C18—C17—C17ii109.10 (14)
C12—C4—C5117.8 (3)C18—C17—C15109.46 (16)
C6—C5—C4122.0 (3)C17ii—C17—C15111.98 (14)
C6—C5—H5119.0C18—C17—H17108.7
C4—C5—H5119.0C17ii—C17—H17108.7
C5—C6—C7121.1 (3)C15—C17—H17108.7
C5—C6—H6119.4O6—C18—O5121.0 (2)
C7—C6—H6119.4O6—C18—C17119.60 (19)
C11—C7—C8116.9 (3)O5—C18—C17119.37 (19)
C11—C7—C6118.6 (3)
Symmetry codes: (i) x, y+1, z; (ii) x+2, y, z+3/2; (iii) x, y1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C6—H6···O4iv0.932.483.210 (4)136
O3—H3A···O1v0.86 (4)1.82 (3)2.628 (2)155 (4)
C10—H10···O6v0.932.423.139 (3)134
Symmetry codes: (iv) x+3/2, y+1/2, z+2; (v) x+2, y, z+2.

Experimental details

Crystal data
Chemical formula[Ni2(C12H8O12)(C12H8N2)2]
Mr411.01
Crystal system, space groupMonoclinic, C2/c
Temperature (K)298
a, b, c (Å)22.018 (4), 8.9600 (18), 16.371 (3)
β (°) 92.49 (3)
V3)3226.6 (11)
Z8
Radiation typeMo Kα
µ (mm1)1.24
Crystal size (mm)0.31 × 0.22 × 0.11
Data collection
DiffractometerBruker P4
diffractometer
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.727, 0.872
No. of measured, independent and
observed [I > 2σ(I)] reflections
4519, 3715, 2959
Rint0.030
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.036, 0.087, 1.01
No. of reflections3715
No. of parameters250
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.34, 0.29

Computer programs: XSCANS (Siemens, 1996), XSCANS, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997), SHELXTL.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C6—H6···O4i0.932.483.210 (4)136
O3—H3A···O1ii0.86 (4)1.82 (3)2.628 (2)155 (4)
C10—H10···O6ii0.932.423.139 (3)134
Symmetry codes: (i) x+3/2, y+1/2, z+2; (ii) x+2, y, z+2.
 

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