supplementary materials
Diaquabis(2-oxidopyridinium-3-carboxylato-
2O2,O3)cobalt(II)
Diluted sodium hydroxide H2O solution was added in drops into 30 ml H2O solution containing Co(ClO4)2·6H2O (0.1830 g, 0.500 mmol) and 2-hydroxyl-3-carboxylpyridine (0.1390 g, 1.13 mmol) until the pH value reached 4, and the solution was stirred for another a few minutes. The red single crystals were obtained after the mixed solution had been allowed to stand at room temperature for one week.
H atoms of water molecule were located in a difference Fourier map and included in the refinements as riding in their as-found positions, with O—H = 0.886–0.889 Å, Uiso(H) = 1.5Ueq(O); the rest of the H atoms were placed in calculated positions with C—H = 0.93 Å, Uiso(H) = 1.2Ueq(C); N—H = 0.86 Å, Uiso(H) = 1.2Ueq(N).
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS (Bruker, 2001); program(s) used to refine structure: SHELXTL (Bruker, 2001); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Diaquabis(2-oxidopyridinium-3-carboxylate)cobalt(II)
top
Crystal data top
| [Co(C6H4NO3)2(H2O)2] | F000 = 378 |
| Mr = 371.17 | Dx = 1.811 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 1158 reflections |
| a = 7.4216 (19) Å | θ = 2.8–26.7º |
| b = 12.330 (3) Å | µ = 1.31 mm−1 |
| c = 7.550 (2) Å | T = 298 (2) K |
| β = 99.921 (4)º | Prism, red |
| V = 680.6 (3) Å3 | 0.26 × 0.20 × 0.05 mm |
| Z = 2 | |
Data collection top
Bruker SMART APEX CCD diffractometer | 1331 independent reflections |
| Radiation source: fine-focus sealed tube | 1151 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.035 |
| T = 298(2) K | θmax = 26.0º |
| φ and ω scans | θmin = 2.8º |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −8→9 |
| Tmin = 0.727, Tmax = 0.937 | k = −15→8 |
| 3627 measured reflections | l = −9→8 |
Refinement top
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.034 | H-atom parameters constrained |
| wR(F2) = 0.083 | w = 1/[σ2(Fo2) + (0.0376P)2 + 0.5342P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.02 | (Δ/σ)max < 0.001 |
| 1331 reflections | Δρmax = 0.39 e Å−3 |
| 106 parameters | Δρmin = −0.29 e Å−3 |
| Primary atom site location: structure-invariant direct methods | Extinction correction: none |
Crystal data top
| [Co(C6H4NO3)2(H2O)2] | V = 680.6 (3) Å3 |
| Mr = 371.17 | Z = 2 |
| Monoclinic, P21/c | Mo Kα |
| a = 7.4216 (19) Å | µ = 1.31 mm−1 |
| b = 12.330 (3) Å | T = 298 (2) K |
| c = 7.550 (2) Å | 0.26 × 0.20 × 0.05 mm |
| β = 99.921 (4)º | |
Data collection top
Bruker SMART APEX CCD diffractometer | 1331 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1151 reflections with I > 2σ(I) |
| Tmin = 0.727, Tmax = 0.937 | Rint = 0.035 |
| 3627 measured reflections | |
Refinement top
| R[F2 > 2σ(F2)] = 0.034 | 106 parameters |
| wR(F2) = 0.083 | H-atom parameters constrained |
| S = 1.02 | Δρmax = 0.39 e Å−3 |
| 1331 reflections | Δρmin = −0.29 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 | |
| O1 | −0.0608 (2) | 0.84059 (13) | −0.0153 (2) | 0.0183 (4) | |
| C6 | 0.0373 (3) | 0.7569 (2) | 0.0071 (3) | 0.0153 (5) | |
| Co1 | 0.0000 | 1.0000 | 0.0000 | 0.01392 (16) | |
| O3 | 0.2707 (2) | 0.95557 (14) | −0.0135 (2) | 0.0185 (4) | |
| N1 | 0.5220 (3) | 0.86194 (17) | 0.1087 (3) | 0.0195 (5) | |
| H1 | 0.5827 | 0.9211 | 0.1047 | 0.023* | |
| O2 | −0.0295 (2) | 0.66277 (14) | −0.0126 (2) | 0.0194 (4) | |
| C1 | 0.2408 (3) | 0.7664 (2) | 0.0610 (3) | 0.0158 (5) | |
| C5 | 0.3400 (4) | 0.6753 (2) | 0.1223 (3) | 0.0198 (6) | |
| H4 | 0.2783 | 0.6098 | 0.1246 | 0.024* | |
| O4 | 0.0769 (3) | 0.99441 (13) | 0.2817 (2) | 0.0239 (4) | |
| H6 | 0.0545 | 1.0547 | 0.3380 | 0.036* | |
| H5 | 0.0372 | 0.9411 | 0.3444 | 0.036* | |
| C2 | 0.3378 (3) | 0.8659 (2) | 0.0496 (3) | 0.0157 (5) | |
| C3 | 0.6169 (4) | 0.7728 (2) | 0.1729 (3) | 0.0235 (6) | |
| H2 | 0.7427 | 0.7769 | 0.2115 | 0.028* | |
| C4 | 0.5282 (4) | 0.6769 (2) | 0.1809 (4) | 0.0245 (6) | |
| H3 | 0.5913 | 0.6145 | 0.2241 | 0.029* | |
Atomic displacement parameters (Å2) top| | U11 | U22 | U33 | U12 | U13 | U23 |
| O1 | 0.0140 (9) | 0.0112 (9) | 0.0291 (10) | 0.0005 (7) | 0.0023 (7) | −0.0004 (7) |
| C6 | 0.0171 (13) | 0.0169 (14) | 0.0124 (11) | 0.0000 (9) | 0.0041 (10) | 0.0001 (10) |
| Co1 | 0.0123 (3) | 0.0098 (3) | 0.0198 (3) | 0.00027 (18) | 0.00311 (18) | 0.00043 (19) |
| O3 | 0.0146 (9) | 0.0132 (9) | 0.0285 (10) | 0.0006 (7) | 0.0055 (7) | 0.0025 (8) |
| N1 | 0.0135 (11) | 0.0200 (12) | 0.0251 (12) | −0.0025 (8) | 0.0031 (9) | 0.0012 (9) |
| O2 | 0.0194 (10) | 0.0111 (10) | 0.0269 (10) | −0.0022 (7) | 0.0020 (8) | −0.0005 (7) |
| C1 | 0.0171 (13) | 0.0153 (13) | 0.0152 (11) | −0.0011 (10) | 0.0036 (10) | 0.0005 (10) |
| C5 | 0.0203 (14) | 0.0191 (14) | 0.0209 (13) | −0.0001 (10) | 0.0056 (11) | 0.0030 (10) |
| O4 | 0.0371 (12) | 0.0128 (9) | 0.0223 (9) | −0.0003 (8) | 0.0064 (8) | 0.0011 (7) |
| C2 | 0.0138 (13) | 0.0191 (14) | 0.0148 (12) | −0.0004 (10) | 0.0041 (10) | −0.0015 (10) |
| C3 | 0.0152 (13) | 0.0317 (16) | 0.0230 (13) | 0.0024 (11) | 0.0013 (11) | 0.0075 (12) |
| C4 | 0.0207 (15) | 0.0230 (15) | 0.0294 (14) | 0.0081 (11) | 0.0033 (11) | 0.0101 (11) |
Geometric parameters (Å, °) top
| O1—C6 | 1.257 (3) | N1—C2 | 1.364 (3) |
| O1—Co1 | 2.0155 (17) | N1—H1 | 0.8600 |
| C6—O2 | 1.261 (3) | C1—C5 | 1.379 (3) |
| C6—C1 | 1.500 (3) | C1—C2 | 1.432 (3) |
| Co1—O1i | 2.0155 (17) | C5—C4 | 1.390 (4) |
| Co1—O3i | 2.1016 (17) | C5—H4 | 0.9300 |
| Co1—O3 | 2.1016 (17) | O4—H6 | 0.8862 |
| Co1—O4i | 2.1065 (19) | O4—H5 | 0.8893 |
| Co1—O4 | 2.1065 (19) | C3—C4 | 1.359 (4) |
| O3—C2 | 1.271 (3) | C3—H2 | 0.9300 |
| N1—C3 | 1.350 (3) | C4—H3 | 0.9300 |
| | | |
| C6—O1—Co1 | 132.40 (16) | C3—N1—H1 | 117.3 |
| O1—C6—O2 | 122.2 (2) | C2—N1—H1 | 117.3 |
| O1—C6—C1 | 120.3 (2) | C5—C1—C2 | 118.3 (2) |
| O2—C6—C1 | 117.5 (2) | C5—C1—C6 | 118.8 (2) |
| O1i—Co1—O1 | 180.0 | C2—C1—C6 | 122.9 (2) |
| O1i—Co1—O3i | 87.10 (7) | C1—C5—C4 | 123.0 (2) |
| O1—Co1—O3i | 92.90 (7) | C1—C5—H4 | 118.5 |
| O1i—Co1—O3 | 92.90 (7) | C4—C5—H4 | 118.5 |
| O1—Co1—O3 | 87.10 (7) | Co1—O4—H6 | 114.6 |
| O3i—Co1—O3 | 180.0 | Co1—O4—H5 | 120.3 |
| O1i—Co1—O4i | 92.57 (7) | H6—O4—H5 | 105.0 |
| O1—Co1—O4i | 87.43 (7) | O3—C2—N1 | 117.4 (2) |
| O3i—Co1—O4i | 86.87 (7) | O3—C2—C1 | 126.8 (2) |
| O3—Co1—O4i | 93.13 (7) | N1—C2—C1 | 115.8 (2) |
| O1i—Co1—O4 | 87.43 (7) | N1—C3—C4 | 119.8 (2) |
| O1—Co1—O4 | 92.57 (7) | N1—C3—H2 | 120.1 |
| O3i—Co1—O4 | 93.13 (7) | C4—C3—H2 | 120.1 |
| O3—Co1—O4 | 86.87 (7) | C3—C4—C5 | 117.8 (2) |
| O4i—Co1—O4 | 180.00 (9) | C3—C4—H3 | 121.1 |
| C2—O3—Co1 | 121.63 (15) | C5—C4—H3 | 121.1 |
| C3—N1—C2 | 125.3 (2) | | |
| | | |
| Co1—O1—C6—O2 | −178.61 (15) | O2—C6—C1—C2 | 165.8 (2) |
| Co1—O1—C6—C1 | 2.1 (3) | C2—C1—C5—C4 | 3.0 (4) |
| C6—O1—Co1—O1i | 9(13) | C6—C1—C5—C4 | −177.8 (2) |
| C6—O1—Co1—O3i | −164.1 (2) | Co1—O3—C2—N1 | −151.59 (17) |
| C6—O1—Co1—O3 | 15.9 (2) | Co1—O3—C2—C1 | 30.4 (3) |
| C6—O1—Co1—O4i | 109.2 (2) | C3—N1—C2—O3 | −177.3 (2) |
| C6—O1—Co1—O4 | −70.8 (2) | C3—N1—C2—C1 | 1.0 (4) |
| O1i—Co1—O3—C2 | 149.27 (18) | C5—C1—C2—O3 | 175.4 (2) |
| O1—Co1—O3—C2 | −30.73 (18) | C6—C1—C2—O3 | −3.8 (4) |
| O3i—Co1—O3—C2 | −15 (93) | C5—C1—C2—N1 | −2.6 (3) |
| O4i—Co1—O3—C2 | −117.99 (18) | C6—C1—C2—N1 | 178.2 (2) |
| O4—Co1—O3—C2 | 62.01 (18) | C2—N1—C3—C4 | 0.5 (4) |
| O1—C6—C1—C5 | 166.0 (2) | N1—C3—C4—C5 | −0.3 (4) |
| O2—C6—C1—C5 | −13.3 (3) | C1—C5—C4—C3 | −1.4 (4) |
| O1—C6—C1—C2 | −14.8 (3) | | |
| Symmetry codes: (i) −x, −y+2, −z. |
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H5···O2ii | 0.89 | 1.80 | 2.686 (2) | 175 |
| O4—H6···O2iii | 0.89 | 1.91 | 2.772 (2) | 165 |
| N1—H1···O3iv | 0.86 | 2.06 | 2.886 (3) | 162 |
| C3—H2···O1v | 0.93 | 2.56 | 3.100 (3) | 118 |
| C3—H2···O2vi | 0.93 | 2.56 | 3.318 (3) | 139 |
| Symmetry codes: (ii) x, −y+3/2, z+1/2; (iii) −x, y+1/2, −z+1/2; (iv) −x+1, −y+2, −z; (v) x+1, y, z; (vi) x+1, −y+3/2, z+1/2. |
Table 1
Selected geometric parameters (Å) top| O1—Co1 | 2.0155 (17) | Co1—O4 | 2.1065 (19) |
| Co1—O3 | 2.1016 (17) | | |
Table 2
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H5···O2i | 0.89 | 1.80 | 2.686 (2) | 175 |
| O4—H6···O2ii | 0.89 | 1.91 | 2.772 (2) | 165 |
| N1—H1···O3iii | 0.86 | 2.06 | 2.886 (3) | 162 |
| C3—H2···O1iv | 0.93 | 2.56 | 3.100 (3) | 118 |
| C3—H2···O2v | 0.93 | 2.56 | 3.318 (3) | 139 |
| Symmetry codes: (i) x, −y+3/2, z+1/2; (ii) −x, y+1/2, −z+1/2; (iii) −x+1, −y+2, −z; (iv) x+1, y, z; (v) x+1, −y+3/2, z+1/2. |
Bruker (1997). SMART (Version 5.6) and SAINT (Version 5.06a), Bruker AXS Inc., Madison, Wisconsin, USA.
Bruker (2001). SHELXS and SHELXTL (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.
Sakai, K. I., Imakubo, T., Ichikawa, M. & Taniguchi, Y. (2006). Dalton Trans. 881–883.
Sheldrick, G. M. (1996). SADABS. (Version 2.10). University of Göttingen, Germany.
Metal complexes containing N-heterocyclic ligands play a pivotal role in the area of modern coordination chemistry, and it has been reported that complex containing 3-hydroxypicolinamide ligand displays strong fluorescent emission (Sakai et al., 2006). The interest in this area led us to synthesize the title complex, and here we report its crystal structure, (I).
Fig. 1 shows the molecular structure of (I), the CoII atom lies in an inversion centre and assumes a little distored octahedral geometry (Table 1). There is a weak π-π stacking interaction between adjacent pyridyl rings of the neighboring complexes; the relevant distances are Cg1···Cg1i = 3.8067 (17) Å and Cg1···Cg1iperp = 3.533 Å [symmetry codes: (i) X, 3/2-Y, −1/2+Z; Cg1 is the centroid of pyridyl ring; Cg1···Cg1perp is the perpendicular distance from ring Cg1 to ring Cg1i]. Table 2 and Fig. 2 show the information of O—H···O, N—H···O and C—H···O hydrogen bonds, and it is the hydrogen bonds that led to the connection of adjacent mononuclear complexes and to the formation of a super-molecular three-dimensional polymer.