Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803017586/lh6099sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536803017586/lh6099Isup2.hkl |
CCDC reference: 222809
Key indicators
- Single-crystal X-ray study
- T = 150 K
- Mean (C-C) = 0.008 Å
- R factor = 0.045
- wR factor = 0.113
- Data-to-parameter ratio = 12.2
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ..... 0.99 PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang.. 8
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion
An ethanol solution (5 ml) of benzimidazole (0.24 g, 2 mmol) was mixed with an aqueous solution (5 ml) of CoCl2·6H2O (0.24 g, 1 mmol) at room temperature. After refluxing the solution for 30 min, an aqueous solution (5 ml) containing fumaric acid (0.12 g, 1 mmol) and NaOH (0.08 g, 2 mmol) was added. The mixture was refluxed for 1 h and filtered. The pink single crystals were obtained after 2 d.
H atoms of the water molecule were located in a difference Fourier map and were included in structure-factor calculations with fixed positional and displacement parameters of Uiso = 0.05 Å2. Other H atoms were placed in calculated positions with C—H distances of 0.93 Å and N—H distances of 0.86 Å, and were included in final cycles of refinement in the riding mode with Uiso(H) = 1.2Ueq of the carrier atom.
Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; 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) and XP (Siemens, 1994); software used to prepare material for publication: WinGX (Farrugia, 1999).
[Co(C4H2O4)(C7H6N2)2(H2O)2] | Z = 1 |
Mr = 445.29 | F(000) = 229 |
Triclinic, P1 | Dx = 1.625 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.0668 (10) Å | Cell parameters from 1988 reflections |
b = 8.5150 (12) Å | θ = 2.0–23.0° |
c = 8.7929 (13) Å | µ = 0.99 mm−1 |
α = 99.358 (11)° | T = 150 K |
β = 113.322 (13)° | Prism, pink |
γ = 102.787 (12)° | 0.32 × 0.30 × 0.22 mm |
V = 454.95 (13) Å3 |
Bruker SMART CCD diffractometer | 1623 independent reflections |
Radiation source: fine-focus sealed tube | 996 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.053 |
ω and ϕ scans | θmax = 25.2°, θmin = 2.6° |
Absorption correction: empirical (using intensity measurements) (SADABS; Bruker, 1999) | h = −8→4 |
Tmin = 0.722, Tmax = 0.802 | k = −9→10 |
2497 measured reflections | l = −10→10 |
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)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.113 | H-atom parameters constrained |
S = 0.91 | w = 1/[σ2(Fo2) + (0.0269P)2 + 0.2058P] where P = (Fo2 + 2Fc2)/3 |
1623 reflections | (Δ/σ)max < 0.001 |
133 parameters | Δρmax = 0.51 e Å−3 |
0 restraints | Δρmin = −0.50 e Å−3 |
[Co(C4H2O4)(C7H6N2)2(H2O)2] | γ = 102.787 (12)° |
Mr = 445.29 | V = 454.95 (13) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.0668 (10) Å | Mo Kα radiation |
b = 8.5150 (12) Å | µ = 0.99 mm−1 |
c = 8.7929 (13) Å | T = 150 K |
α = 99.358 (11)° | 0.32 × 0.30 × 0.22 mm |
β = 113.322 (13)° |
Bruker SMART CCD diffractometer | 1623 independent reflections |
Absorption correction: empirical (using intensity measurements) (SADABS; Bruker, 1999) | 996 reflections with I > 2σ(I) |
Tmin = 0.722, Tmax = 0.802 | Rint = 0.053 |
2497 measured reflections |
R[F2 > 2σ(F2)] = 0.045 | 0 restraints |
wR(F2) = 0.113 | H-atom parameters constrained |
S = 0.91 | Δρmax = 0.51 e Å−3 |
1623 reflections | Δρmin = −0.50 e Å−3 |
133 parameters |
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 | ||
Co | 0.5000 | 0.5000 | 0.5000 | 0.0168 (3) | |
O1 | 0.2738 (5) | 0.2672 (4) | 0.4332 (4) | 0.0183 (9) | |
O2 | 0.1069 (5) | 0.3189 (4) | 0.5978 (4) | 0.0173 (8) | |
O3 | 0.2983 (5) | 0.6180 (4) | 0.5682 (4) | 0.0194 (9) | |
N1 | 0.7701 (6) | 0.5607 (5) | 1.0466 (5) | 0.0190 (10) | |
H1 | 0.8158 | 0.6230 | 1.1493 | 0.023* | |
N3 | 0.6309 (6) | 0.4838 (5) | 0.7561 (5) | 0.0179 (10) | |
C2 | 0.6941 (8) | 0.6059 (6) | 0.8993 (6) | 0.0201 (13) | |
H2 | 0.6862 | 0.7132 | 0.8974 | 0.024* | |
C4 | 0.6366 (8) | 0.1839 (6) | 0.7264 (6) | 0.0204 (13) | |
H4 | 0.5786 | 0.1505 | 0.6068 | 0.025* | |
C5 | 0.6938 (9) | 0.0747 (7) | 0.8255 (7) | 0.0269 (14) | |
H5 | 0.6712 | −0.0352 | 0.7697 | 0.032* | |
C6 | 0.7858 (8) | 0.1247 (7) | 1.0094 (6) | 0.0277 (14) | |
H6 | 0.8256 | 0.0485 | 1.0706 | 0.033* | |
C7 | 0.8158 (8) | 0.2843 (7) | 1.0963 (7) | 0.0247 (13) | |
H7 | 0.8717 | 0.3170 | 1.2158 | 0.030* | |
C8 | 0.7606 (7) | 0.3943 (6) | 1.0008 (6) | 0.0176 (12) | |
C9 | 0.6715 (8) | 0.3471 (6) | 0.8175 (6) | 0.0161 (12) | |
C11 | 0.1553 (8) | 0.2211 (6) | 0.5030 (6) | 0.0169 (12) | |
C12 | 0.0596 (8) | 0.0350 (6) | 0.4656 (6) | 0.0207 (13) | |
H12 | 0.0862 | −0.0350 | 0.3889 | 0.025* | |
H31 | 0.2250 | 0.5256 | 0.6003 | 0.050* | |
H32 | 0.1829 | 0.6475 | 0.5039 | 0.050* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co | 0.0184 (6) | 0.0157 (6) | 0.0172 (6) | 0.0054 (5) | 0.0089 (5) | 0.0045 (5) |
O1 | 0.022 (2) | 0.017 (2) | 0.0192 (19) | 0.0031 (16) | 0.0141 (17) | 0.0045 (16) |
O2 | 0.024 (2) | 0.012 (2) | 0.022 (2) | 0.0062 (16) | 0.0152 (17) | 0.0050 (16) |
O3 | 0.017 (2) | 0.021 (2) | 0.025 (2) | 0.0078 (16) | 0.0107 (17) | 0.0097 (17) |
N1 | 0.025 (3) | 0.018 (3) | 0.011 (2) | 0.007 (2) | 0.007 (2) | 0.001 (2) |
N3 | 0.022 (2) | 0.016 (3) | 0.021 (2) | 0.007 (2) | 0.014 (2) | 0.007 (2) |
C2 | 0.029 (3) | 0.012 (3) | 0.020 (3) | 0.006 (2) | 0.013 (3) | 0.004 (2) |
C4 | 0.028 (3) | 0.018 (3) | 0.018 (3) | 0.006 (2) | 0.012 (3) | 0.006 (2) |
C5 | 0.042 (4) | 0.017 (3) | 0.032 (3) | 0.013 (3) | 0.024 (3) | 0.010 (3) |
C6 | 0.035 (4) | 0.032 (4) | 0.022 (3) | 0.020 (3) | 0.011 (3) | 0.016 (3) |
C7 | 0.025 (3) | 0.032 (4) | 0.017 (3) | 0.014 (3) | 0.007 (3) | 0.008 (3) |
C8 | 0.014 (3) | 0.020 (3) | 0.016 (3) | 0.003 (2) | 0.007 (2) | −0.001 (3) |
C9 | 0.019 (3) | 0.018 (3) | 0.018 (3) | 0.006 (2) | 0.012 (2) | 0.010 (2) |
C11 | 0.018 (3) | 0.019 (3) | 0.014 (3) | 0.007 (2) | 0.006 (2) | 0.007 (2) |
C12 | 0.029 (3) | 0.015 (3) | 0.026 (3) | 0.008 (2) | 0.021 (3) | 0.003 (2) |
Co—O1 | 2.075 (3) | C4—C5 | 1.392 (7) |
Co—N3 | 2.110 (4) | C4—C9 | 1.402 (7) |
Co—O3 | 2.125 (3) | C4—H4 | 0.93 |
O1—C11 | 1.253 (5) | C5—C6 | 1.428 (7) |
O2—C11 | 1.278 (5) | C5—H5 | 0.93 |
O3—H31 | 0.987 | C6—C7 | 1.372 (7) |
O3—H32 | 0.905 | C6—H6 | 0.93 |
N1—C2 | 1.348 (6) | C7—C8 | 1.375 (7) |
N1—C8 | 1.387 (6) | C7—H7 | 0.93 |
N1—H1 | 0.86 | C8—C9 | 1.425 (6) |
N3—C2 | 1.338 (6) | C11—C12 | 1.502 (7) |
N3—C9 | 1.399 (6) | C12—C12i | 1.315 (8) |
C2—H2 | 0.93 | C12—H12 | 0.93 |
O1—Co—N3 | 87.60 (13) | C4—C5—H5 | 118.7 |
O1—Co—O3 | 89.97 (12) | C6—C5—H5 | 118.7 |
N3—Co—O3 | 85.64 (14) | C7—C6—C5 | 120.5 (5) |
C11—O1—Co | 128.1 (3) | C7—C6—H6 | 119.8 |
Co—O3—H31 | 98.1 | C5—C6—H6 | 119.8 |
Co—O3—H32 | 131.6 | C6—C7—C8 | 117.8 (5) |
H31—O3—H32 | 100.1 | C6—C7—H7 | 121.1 |
C2—N1—C8 | 106.9 (4) | C8—C7—H7 | 121.1 |
C2—N1—H1 | 126.5 | C7—C8—N1 | 132.4 (5) |
C8—N1—H1 | 126.5 | C7—C8—C9 | 122.4 (5) |
C2—N3—C9 | 103.7 (4) | N1—C8—C9 | 105.1 (4) |
C2—N3—Co | 126.9 (3) | N3—C9—C4 | 129.7 (5) |
C9—N3—Co | 129.4 (3) | N3—C9—C8 | 109.7 (4) |
N3—C2—N1 | 114.5 (5) | C4—C9—C8 | 120.6 (5) |
N3—C2—H2 | 122.8 | O1—C11—O2 | 125.3 (5) |
N1—C2—H2 | 122.8 | O1—C11—C12 | 116.0 (4) |
C5—C4—C9 | 116.0 (5) | O2—C11—C12 | 118.6 (4) |
C5—C4—H4 | 122.0 | C12i—C12—C11 | 124.1 (6) |
C9—C4—H4 | 122.0 | C12i—C12—H12 | 117.9 |
C4—C5—C6 | 122.7 (5) | C11—C12—H12 | 117.9 |
Symmetry code: (i) −x, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H31···O2 | 0.99 | 1.77 | 2.712 (5) | 159 |
O3—H32···O2ii | 0.91 | 1.99 | 2.871 (5) | 163 |
N1—H1···O2iii | 0.86 | 2.01 | 2.827 (5) | 158 |
Symmetry codes: (ii) −x, −y+1, −z+1; (iii) −x+1, −y+1, −z+2. |
Experimental details
Crystal data | |
Chemical formula | [Co(C4H2O4)(C7H6N2)2(H2O)2] |
Mr | 445.29 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 150 |
a, b, c (Å) | 7.0668 (10), 8.5150 (12), 8.7929 (13) |
α, β, γ (°) | 99.358 (11), 113.322 (13), 102.787 (12) |
V (Å3) | 454.95 (13) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 0.99 |
Crystal size (mm) | 0.32 × 0.30 × 0.22 |
Data collection | |
Diffractometer | Bruker SMART CCD diffractometer |
Absorption correction | Empirical (using intensity measurements) (SADABS; Bruker, 1999) |
Tmin, Tmax | 0.722, 0.802 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2497, 1623, 996 |
Rint | 0.053 |
(sin θ/λ)max (Å−1) | 0.599 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.045, 0.113, 0.91 |
No. of reflections | 1623 |
No. of parameters | 133 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.51, −0.50 |
Computer programs: SMART (Bruker, 1999), SAINT (Bruker, 1999), SAINT, SIR92 (Altomare et al., 1993), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997) and XP (Siemens, 1994), WinGX (Farrugia, 1999).
Co—O1 | 2.075 (3) | O2—C11 | 1.278 (5) |
Co—N3 | 2.110 (4) | C11—C12 | 1.502 (7) |
Co—O3 | 2.125 (3) | C12—C12i | 1.315 (8) |
O1—C11 | 1.253 (5) | ||
O1—Co—N3 | 87.60 (13) | N3—Co—O3 | 85.64 (14) |
O1—Co—O3 | 89.97 (12) |
Symmetry code: (i) −x, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H31···O2 | 0.99 | 1.77 | 2.712 (5) | 159 |
O3—H32···O2ii | 0.91 | 1.99 | 2.871 (5) | 163 |
N1—H1···O2iii | 0.86 | 2.01 | 2.827 (5) | 158 |
Symmetry codes: (ii) −x, −y+1, −z+1; (iii) −x+1, −y+1, −z+2. |
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The aromatic π–π-stacking interaction has shown to be correlated with the electron transfer in some biological system (Deisenhofer & Michel, 1989). As part of investigation on the π–π-stacking interaction in metal complexes (Chen, 2003), the title polymeric CoII complex, (I), with the benzimidazole ligand has recently been prepared in the laboratory.
The coordination environment around the CoII atom in (I) is illustrated in Fig. 1. The CoII atom is located at an inversion center and possesses an octahedral coordinate geometry formed by benzimidazole molecules, water molecules and fumarate dianions with the normal geometry parameters (Table 1). The carboxyl group of the fumarate dianion coordinates in a monodentate manner to the CoII atom. The uncoordinated carboxyl O atom (O2) is hydrogen bonded to the neighboring benzimidazole and coordinated water molecules (Fig. 1).
Each fumarate dianion bridges two CoII atoms through both terminal carboxyl groups to form polymeric complex chains as shown in Fig. 2. Adjacent polymeric chains link each other by hydrogen bonds (Table 2). The overlapped arrangement of benzimidazole rings is observed between the adjacent complex molecules related by an inversion center (Fig. 3). The shorter separation of 3.35 (2) Å between neighboring parallel benzimidazole rings suggests the existence of the π–π stacking.