The title compound, [Ni(μ-C4H2O4)(C7H6N2)2(H2O)2]n, is a one-dimensional polymeric complex bridged by fumarate dianions. The Ni atom lies on one inversion centre and the fumarate on another. The molecular chains are linked by hydrogen bonding. π–π stacking between parallel benzimidazole rings exists in the crystal structure.
Supporting information
CCDC reference: 245155
Key indicators
- Single-crystal X-ray study
- T = 295 K
- Mean (C-C) = 0.004 Å
- R factor = 0.034
- wR factor = 0.084
- Data-to-parameter ratio = 11.6
checkCIF/PLATON results
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Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
Crystal data top
[Ni(C4H2O4)(C7H6N2)2(H2O)2] | Z = 1 |
Mr = 445.07 | F(000) = 230 |
Triclinic, P1 | Dx = 1.641 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71069 Å |
a = 7.065 (1) Å | Cell parameters from 2668 reflections |
b = 8.4842 (10) Å | θ = 3.0–26.0° |
c = 8.6617 (9) Å | µ = 1.12 mm−1 |
α = 98.471 (7)° | T = 295 K |
β = 112.685 (4)° | Prism, green |
γ = 103.098 (4)° | 0.27 × 0.14 × 0.10 mm |
V = 450.37 (10) Å3 | |
Data collection top
Rigaku R-AXIS RAPID diffractometer | 1616 independent reflections |
Radiation source: fine-focus sealed tube | 1511 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.038 |
Detector resolution: 10.00 pixels mm-1 | θmax = 25.2°, θmin = 2.6° |
ω scans | h = −8→7 |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | k = −10→10 |
Tmin = 0.74, Tmax = 0.89 | l = −10→10 |
3114 measured reflections | |
Refinement top
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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.084 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0476P)2 + 0.3701P] where P = (Fo2 + 2Fc2)/3 |
1616 reflections | (Δ/σ)max = 0.001 |
139 parameters | Δρmax = 0.27 e Å−3 |
0 restraints | Δρmin = −0.28 e Å−3 |
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 | x | y | z | Uiso*/Ueq | |
Ni | 0.5000 | 0.5000 | 0.5000 | 0.01881 (15) | |
O1 | 0.2747 (3) | 0.26834 (19) | 0.4323 (2) | 0.0241 (4) | |
O2 | 0.1056 (3) | 0.3179 (2) | 0.5970 (2) | 0.0270 (4) | |
O3 | 0.3007 (3) | 0.6170 (2) | 0.5673 (2) | 0.0287 (4) | |
N1 | 0.7654 (4) | 0.5579 (3) | 1.0396 (3) | 0.0305 (5) | |
H1 | 0.8118 | 0.6199 | 1.1427 | 0.037* | |
N3 | 0.6318 (3) | 0.4840 (2) | 0.7531 (2) | 0.0248 (4) | |
C2 | 0.6916 (4) | 0.6049 (3) | 0.8925 (3) | 0.0290 (5) | |
H2 | 0.6834 | 0.7123 | 0.8889 | 0.035* | |
C4 | 0.6353 (4) | 0.1839 (3) | 0.7276 (3) | 0.0316 (6) | |
H4 | 0.5788 | 0.1519 | 0.6074 | 0.038* | |
C5 | 0.6882 (5) | 0.0718 (4) | 0.8249 (4) | 0.0404 (7) | |
H5 | 0.6671 | −0.0376 | 0.7694 | 0.049* | |
C6 | 0.7730 (6) | 0.1205 (4) | 1.0056 (4) | 0.0478 (8) | |
H6 | 0.8065 | 0.0423 | 1.0678 | 0.057* | |
C7 | 0.8080 (5) | 0.2797 (4) | 1.0934 (4) | 0.0411 (7) | |
H7 | 0.8660 | 0.3115 | 1.2137 | 0.049* | |
C8 | 0.7536 (4) | 0.3922 (3) | 0.9957 (3) | 0.0276 (5) | |
C9 | 0.6692 (4) | 0.3454 (3) | 0.8153 (3) | 0.0230 (5) | |
C11 | 0.1524 (4) | 0.2216 (3) | 0.5016 (3) | 0.0220 (5) | |
C12 | 0.0593 (4) | 0.0364 (3) | 0.4650 (3) | 0.0266 (5) | |
H12 | 0.0871 | −0.0319 | 0.3874 | 0.032* | |
H3A | 0.205 (7) | 0.653 (6) | 0.500 (6) | 0.080* | |
H3B | 0.216 (7) | 0.534 (6) | 0.581 (6) | 0.080* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Ni | 0.0220 (2) | 0.0152 (2) | 0.0197 (2) | 0.00365 (16) | 0.01040 (17) | 0.00524 (16) |
O1 | 0.0284 (9) | 0.0193 (8) | 0.0249 (8) | 0.0023 (7) | 0.0148 (7) | 0.0057 (6) |
O2 | 0.0326 (9) | 0.0212 (8) | 0.0309 (9) | 0.0066 (7) | 0.0186 (8) | 0.0061 (7) |
O3 | 0.0313 (9) | 0.0258 (9) | 0.0344 (10) | 0.0098 (7) | 0.0185 (8) | 0.0102 (8) |
N1 | 0.0382 (12) | 0.0326 (12) | 0.0184 (10) | 0.0113 (9) | 0.0117 (9) | 0.0016 (8) |
N3 | 0.0298 (11) | 0.0200 (10) | 0.0235 (10) | 0.0054 (8) | 0.0115 (9) | 0.0058 (8) |
C2 | 0.0341 (13) | 0.0237 (12) | 0.0273 (12) | 0.0073 (10) | 0.0126 (11) | 0.0055 (10) |
C4 | 0.0413 (15) | 0.0279 (13) | 0.0276 (13) | 0.0133 (11) | 0.0155 (12) | 0.0078 (11) |
C5 | 0.0583 (18) | 0.0312 (14) | 0.0402 (15) | 0.0213 (13) | 0.0241 (14) | 0.0141 (12) |
C6 | 0.075 (2) | 0.0460 (17) | 0.0444 (17) | 0.0369 (16) | 0.0320 (16) | 0.0284 (14) |
C7 | 0.0569 (18) | 0.0530 (18) | 0.0246 (13) | 0.0306 (15) | 0.0189 (13) | 0.0175 (13) |
C8 | 0.0312 (12) | 0.0311 (13) | 0.0246 (12) | 0.0129 (10) | 0.0142 (10) | 0.0083 (10) |
C9 | 0.0245 (12) | 0.0251 (12) | 0.0228 (11) | 0.0085 (9) | 0.0120 (9) | 0.0100 (9) |
C11 | 0.0227 (11) | 0.0200 (11) | 0.0196 (11) | 0.0038 (9) | 0.0070 (9) | 0.0053 (9) |
C12 | 0.0311 (13) | 0.0201 (12) | 0.0311 (13) | 0.0045 (10) | 0.0185 (11) | 0.0053 (10) |
Geometric parameters (Å, º) top
Ni—O1 | 2.0646 (15) | C4—C5 | 1.382 (4) |
Ni—O3 | 2.0984 (18) | C4—C9 | 1.384 (4) |
Ni—N3 | 2.0647 (19) | C4—H4 | 0.9300 |
O1—C11 | 1.257 (3) | C5—C6 | 1.398 (4) |
O2—C11 | 1.263 (3) | C5—H5 | 0.9300 |
O3—H3A | 0.85 (5) | C6—C7 | 1.366 (4) |
O3—H3B | 0.87 (5) | C6—H6 | 0.9300 |
N1—C2 | 1.336 (3) | C7—C8 | 1.388 (4) |
N1—C8 | 1.376 (3) | C7—H7 | 0.9300 |
N1—H1 | 0.8600 | C8—C9 | 1.395 (3) |
N3—C2 | 1.316 (3) | C11—C12 | 1.492 (3) |
N3—C9 | 1.401 (3) | C12—C12i | 1.310 (5) |
C2—H2 | 0.9300 | C12—H12 | 0.9300 |
| | | |
O1—Ni—N3 | 89.40 (7) | C4—C5—H5 | 119.6 |
O1—Ni—O3 | 90.36 (7) | C6—C5—H5 | 119.6 |
N3—Ni—O3 | 86.66 (8) | C7—C6—C5 | 121.8 (3) |
C11—O1—Ni | 127.73 (15) | C7—C6—H6 | 119.1 |
Ni—O3—H3A | 126 (3) | C5—C6—H6 | 119.1 |
Ni—O3—H3B | 101 (3) | C6—C7—C8 | 117.3 (3) |
H3A—O3—H3B | 99 (4) | C6—C7—H7 | 121.3 |
C2—N1—C8 | 107.4 (2) | C8—C7—H7 | 121.3 |
C2—N1—H1 | 126.3 | N1—C8—C7 | 132.8 (2) |
C8—N1—H1 | 126.3 | N1—C8—C9 | 105.8 (2) |
C2—N3—C9 | 104.98 (19) | C7—C8—C9 | 121.4 (2) |
C2—N3—Ni | 126.05 (17) | C4—C9—C8 | 120.8 (2) |
C9—N3—Ni | 128.93 (16) | C4—C9—N3 | 130.6 (2) |
N3—C2—N1 | 113.2 (2) | C8—C9—N3 | 108.6 (2) |
N3—C2—H2 | 123.4 | O1—C11—O2 | 125.2 (2) |
N1—C2—H2 | 123.4 | O1—C11—C12 | 115.3 (2) |
C5—C4—C9 | 117.7 (2) | O2—C11—C12 | 119.4 (2) |
C5—C4—H4 | 121.1 | C12i—C12—C11 | 124.3 (3) |
C9—C4—H4 | 121.1 | C12i—C12—H12 | 117.8 |
C4—C5—C6 | 120.9 (3) | C11—C12—H12 | 117.8 |
Symmetry code: (i) −x, −y, −z+1. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O2ii | 0.86 | 2.05 | 2.868 (3) | 159 |
O3—H3A···O2iii | 0.86 (5) | 2.11 (5) | 2.893 (3) | 151 (5) |
O3—H3B···O2 | 0.87 (5) | 1.87 (5) | 2.699 (3) | 159 (5) |
Symmetry codes: (ii) −x+1, −y+1, −z+2; (iii) −x, −y+1, −z+1. |