metal-organic compounds
catena-Poly[[lead(II)-μ-(2-oxidobenzaldehyde isonicotinoylhydrazonato)] methanol monosolvate]
aDepartment of Chemistry, Faculty of Science, Tabriz Branch, Islamic Azad University, PO Box 1655, Tabriz, Iran, bDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia, cChemistry Department, Faculty of Science, King Abdulaziz University, PO Box 80203 Jeddah, Saudi Arabia, and dDepartment of Inorganic Chemistry, Faculty of Chemistry, University of Tabriz, PO Box 5166616471, Tabriz, Iran
*Correspondence e-mail: shahverdizadeh@iaut.ac.ir, edward.tiekink@gmail.com
The Pb atom in the polymeric title compound, {[Pb(C13H9N3O2)]·CH3OH}n, is five-coordinated within an N2O2 donor set and a lone pair of electrons, as the N-isonicotinamidosalicylaldiminate ligand coordinates the PbII atom via the O,N,O′-donors and simultaneously bridges a neighbouring Pb atom via the pyridine N atom; the coordination geometry is based on a trigonal bipyramid with the O atoms in axial positions. The resulting supramolecular chain is a 31 helix along the c axis. These chains are linked via intermolecular Pb⋯O,N interactions, as well as O—H⋯O hydrogen bonds.
Related literature
For crystal engineering studies of metal complexes containing isonicotinylhydrazonate ligands, see: Yuan et al. (2007); Vrdoljak et al. (2010, 2011). For specialized crystallization techniques, see: Harrowfield et al. (1996).
Experimental
Crystal data
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Refinement
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Data collection: CrysAlis PRO (Agilent, 2010); cell CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536811043078/su2329sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811043078/su2329Isup2.hkl
A methanol solution (25 ml) of salicylaldehyde (10 mmol) was added drop wise to a methanol solution (15 ml) of 4-pyridinecarboxylic acid hydrazide (10 mmol) and the mixture was stirred for 3 h. The white precipitate was removed by filtration and recrystallized from methanol solution. Then a mixture of the ligand (0.5 mmol) and lead(II) acetate (0.5 mmol) in methanol (35 ml) was stirred at rt for 45 min to give a yellow precipitate which was filtered off and dried. Crystals were obtained by using the branched tube method (Harrowfield et al., 1996). Thus, the complex (0.3 mmol) was placed in the arm to be heated. Methanol was added to fill both arms, and then the arm to be heated was placed in a water bath at 333 K. After 3 days, yellow crystals were deposited in the cooler arm. They were filtered off, washed with water and air dried. Yield: 68%; M.pt. 560 K.
C-bound H atoms were placed in calculated positions and were included in the
in the riding model approximation: O—H = 0.84 Å, C—H = 0.95 and 0.98 Å, for CH and CH3 H atoms, respectively, with Uiso(H) = k × Ueq(O,C), where k = 1.5 for OH and CH3H atoms, and k = 1.2 for all other H atoms.Data collection: CrysAlis PRO (Agilent, 2010); cell
CrysAlis PRO (Agilent, 2010); data reduction: CrysAlis PRO (Agilent, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).[Pb(C13H9N3O2)]·CH4O | Dx = 2.229 Mg m−3 |
Mr = 478.46 | Mo Kα radiation, λ = 0.71073 Å |
Hexagonal, R3 | Cell parameters from 12065 reflections |
Hall symbol: -R 3 | θ = 2.4–29.3° |
a = 28.6702 (5) Å | µ = 11.84 mm−1 |
c = 9.0146 (2) Å | T = 100 K |
V = 6417.1 (3) Å3 | Prism, colourless |
Z = 18 | 0.20 × 0.15 × 0.10 mm |
F(000) = 4032 |
Agilent SuperNova Dual diffractometer with an Atlas detector | 2958 independent reflections |
Radiation source: SuperNova (Cu) X-ray Source | 2816 reflections with I > 2σ(I) |
Mirror monochromator | Rint = 0.026 |
Detector resolution: 10.4041 pixels mm-1 | θmax = 26.5°, θmin = 2.4° |
ω scans | h = −35→35 |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −35→35 |
Tmin = 0.349, Tmax = 1.000 | l = −11→11 |
17626 measured reflections |
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)] = 0.015 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.032 | H-atom parameters constrained |
S = 1.11 | w = 1/[σ2(Fo2) + (0.0114P)2 + 19.9099P] where P = (Fo2 + 2Fc2)/3 |
2958 reflections | (Δ/σ)max = 0.005 |
193 parameters | Δρmax = 0.95 e Å−3 |
0 restraints | Δρmin = −0.60 e Å−3 |
[Pb(C13H9N3O2)]·CH4O | Z = 18 |
Mr = 478.46 | Mo Kα radiation |
Hexagonal, R3 | µ = 11.84 mm−1 |
a = 28.6702 (5) Å | T = 100 K |
c = 9.0146 (2) Å | 0.20 × 0.15 × 0.10 mm |
V = 6417.1 (3) Å3 |
Agilent SuperNova Dual diffractometer with an Atlas detector | 2958 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | 2816 reflections with I > 2σ(I) |
Tmin = 0.349, Tmax = 1.000 | Rint = 0.026 |
17626 measured reflections |
R[F2 > 2σ(F2)] = 0.015 | 0 restraints |
wR(F2) = 0.032 | H-atom parameters constrained |
S = 1.11 | w = 1/[σ2(Fo2) + (0.0114P)2 + 19.9099P] where P = (Fo2 + 2Fc2)/3 |
2958 reflections | Δρmax = 0.95 e Å−3 |
193 parameters | Δρmin = −0.60 e Å−3 |
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 | ||
Pb | 0.172066 (4) | 0.851864 (4) | 1.061072 (10) | 0.01156 (4) | |
O1 | 0.09837 (8) | 0.86813 (8) | 1.0476 (2) | 0.0186 (4) | |
O2 | 0.25307 (7) | 0.88497 (8) | 1.19856 (19) | 0.0147 (4) | |
O3 | 0.08109 (8) | 0.83045 (11) | 0.7716 (2) | 0.0318 (6) | |
H3o | 0.0854 | 0.8444 | 0.8561 | 0.051 (12)* | |
N1 | 0.17051 (9) | 0.89277 (9) | 1.2955 (2) | 0.0119 (4) | |
N2 | 0.21170 (9) | 0.90223 (9) | 1.3966 (2) | 0.0118 (5) | |
N3 | 0.39001 (9) | 0.94432 (9) | 1.6044 (2) | 0.0152 (5) | |
C1 | 0.07467 (11) | 0.88735 (11) | 1.1315 (3) | 0.0144 (6) | |
C2 | 0.03012 (11) | 0.89079 (11) | 1.0785 (3) | 0.0189 (6) | |
H2 | 0.0177 | 0.8792 | 0.9803 | 0.023* | |
C3 | 0.00415 (12) | 0.91040 (12) | 1.1650 (3) | 0.0227 (6) | |
H3 | −0.0252 | 0.9129 | 1.1248 | 0.027* | |
C4 | 0.02038 (12) | 0.92671 (13) | 1.3109 (3) | 0.0242 (7) | |
H4 | 0.0025 | 0.9403 | 1.3702 | 0.029* | |
C5 | 0.06267 (12) | 0.92271 (12) | 1.3669 (3) | 0.0207 (6) | |
H5 | 0.0733 | 0.9330 | 1.4669 | 0.025* | |
C6 | 0.09089 (11) | 0.90384 (11) | 1.2809 (3) | 0.0145 (6) | |
C7 | 0.13591 (11) | 0.90432 (11) | 1.3515 (3) | 0.0141 (5) | |
H7 | 0.1411 | 0.9145 | 1.4531 | 0.017* | |
C8 | 0.25097 (10) | 0.89833 (10) | 1.3328 (3) | 0.0119 (5) | |
C9 | 0.38059 (11) | 0.91341 (11) | 1.4841 (3) | 0.0146 (5) | |
H9 | 0.4057 | 0.9022 | 1.4592 | 0.017* | |
C10 | 0.33565 (10) | 0.89697 (10) | 1.3940 (3) | 0.0130 (5) | |
H10 | 0.3306 | 0.8756 | 1.3084 | 0.016* | |
C11 | 0.29821 (10) | 0.91231 (10) | 1.4312 (3) | 0.0116 (5) | |
C12 | 0.30750 (11) | 0.94353 (11) | 1.5581 (3) | 0.0170 (6) | |
H12 | 0.2822 | 0.9539 | 1.5884 | 0.020* | |
C13 | 0.35383 (12) | 0.95919 (12) | 1.6392 (3) | 0.0197 (6) | |
H13 | 0.3604 | 0.9815 | 1.7235 | 0.024* | |
C14 | 0.02725 (13) | 0.81018 (16) | 0.7254 (4) | 0.0360 (9) | |
H14A | 0.0034 | 0.7974 | 0.8120 | 0.054* | |
H14B | 0.0171 | 0.7802 | 0.6562 | 0.054* | |
H14C | 0.0239 | 0.8388 | 0.6759 | 0.054* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Pb | 0.01132 (6) | 0.01153 (6) | 0.00909 (5) | 0.00365 (4) | −0.00016 (3) | 0.00041 (4) |
O1 | 0.0158 (10) | 0.0239 (11) | 0.0158 (9) | 0.0096 (9) | −0.0023 (8) | −0.0010 (8) |
O2 | 0.0146 (10) | 0.0187 (10) | 0.0091 (9) | 0.0071 (8) | −0.0009 (7) | 0.0003 (7) |
O3 | 0.0130 (11) | 0.0577 (16) | 0.0209 (11) | 0.0150 (11) | −0.0056 (9) | −0.0155 (11) |
N1 | 0.0111 (11) | 0.0087 (11) | 0.0128 (10) | 0.0027 (9) | −0.0013 (9) | 0.0011 (9) |
N2 | 0.0111 (11) | 0.0123 (11) | 0.0116 (10) | 0.0055 (9) | −0.0026 (9) | −0.0009 (9) |
N3 | 0.0129 (12) | 0.0180 (12) | 0.0151 (11) | 0.0081 (10) | −0.0039 (9) | −0.0016 (9) |
C1 | 0.0109 (13) | 0.0098 (13) | 0.0179 (13) | 0.0018 (11) | 0.0025 (11) | 0.0044 (11) |
C2 | 0.0162 (15) | 0.0184 (15) | 0.0186 (14) | 0.0061 (12) | −0.0030 (11) | 0.0027 (12) |
C3 | 0.0137 (15) | 0.0267 (17) | 0.0297 (16) | 0.0117 (13) | −0.0030 (12) | 0.0052 (13) |
C4 | 0.0209 (16) | 0.0286 (17) | 0.0282 (16) | 0.0162 (14) | 0.0019 (13) | −0.0006 (13) |
C5 | 0.0188 (15) | 0.0235 (16) | 0.0198 (14) | 0.0106 (13) | 0.0000 (12) | −0.0007 (12) |
C6 | 0.0116 (13) | 0.0110 (13) | 0.0180 (13) | 0.0035 (11) | 0.0003 (11) | 0.0029 (11) |
C7 | 0.0160 (14) | 0.0129 (13) | 0.0113 (12) | 0.0057 (12) | 0.0009 (11) | −0.0011 (10) |
C8 | 0.0129 (13) | 0.0069 (12) | 0.0137 (12) | 0.0033 (11) | 0.0006 (10) | 0.0022 (10) |
C9 | 0.0130 (14) | 0.0148 (14) | 0.0169 (13) | 0.0077 (12) | 0.0015 (11) | 0.0020 (11) |
C10 | 0.0129 (13) | 0.0112 (13) | 0.0124 (12) | 0.0040 (11) | 0.0009 (10) | −0.0001 (10) |
C11 | 0.0111 (13) | 0.0087 (12) | 0.0132 (12) | 0.0035 (11) | 0.0002 (10) | 0.0010 (10) |
C12 | 0.0146 (14) | 0.0212 (15) | 0.0183 (14) | 0.0113 (12) | −0.0012 (11) | −0.0049 (11) |
C13 | 0.0197 (15) | 0.0262 (16) | 0.0175 (14) | 0.0147 (13) | −0.0043 (12) | −0.0086 (12) |
C14 | 0.0178 (16) | 0.061 (3) | 0.0259 (17) | 0.0175 (17) | −0.0050 (13) | −0.0137 (16) |
Pb—O1 | 2.3837 (19) | C3—H3 | 0.9500 |
Pb—O2 | 2.3721 (18) | C4—C5 | 1.370 (4) |
Pb—N1 | 2.428 (2) | C4—H4 | 0.9500 |
Pb—N3i | 2.530 (2) | C5—C6 | 1.410 (4) |
O1—C1 | 1.308 (3) | C5—H5 | 0.9500 |
O2—C8 | 1.280 (3) | C6—C7 | 1.433 (4) |
O3—C14 | 1.413 (4) | C7—H7 | 0.9500 |
O3—H3o | 0.8400 | C8—C11 | 1.497 (4) |
N1—C7 | 1.295 (3) | C9—C10 | 1.391 (4) |
N1—N2 | 1.406 (3) | C9—H9 | 0.9500 |
N2—C8 | 1.318 (3) | C10—C11 | 1.389 (4) |
N3—C9 | 1.340 (3) | C10—H10 | 0.9500 |
N3—C13 | 1.341 (4) | C11—C12 | 1.393 (4) |
N3—Pbii | 2.530 (2) | C12—C13 | 1.380 (4) |
C1—C2 | 1.412 (4) | C12—H12 | 0.9500 |
C1—C6 | 1.426 (4) | C13—H13 | 0.9500 |
C2—C3 | 1.377 (4) | C14—H14A | 0.9800 |
C2—H2 | 0.9500 | C14—H14B | 0.9800 |
C3—C4 | 1.395 (4) | C14—H14C | 0.9800 |
O2—Pb—O1 | 137.27 (6) | C5—C6—C1 | 119.5 (3) |
O2—Pb—N1 | 66.59 (7) | C5—C6—C7 | 116.0 (2) |
O1—Pb—N1 | 73.59 (7) | C1—C6—C7 | 124.5 (2) |
O2—Pb—N3i | 83.72 (7) | N1—C7—C6 | 128.7 (2) |
O1—Pb—N3i | 82.01 (7) | N1—C7—H7 | 115.6 |
N1—Pb—N3i | 90.94 (7) | C6—C7—H7 | 115.6 |
C1—O1—Pb | 138.69 (17) | O2—C8—N2 | 127.5 (2) |
C8—O2—Pb | 115.50 (16) | O2—C8—C11 | 118.0 (2) |
C14—O3—H3o | 109.5 | N2—C8—C11 | 114.6 (2) |
C7—N1—N2 | 112.0 (2) | N3—C9—C10 | 122.9 (3) |
C7—N1—Pb | 131.62 (18) | N3—C9—H9 | 118.6 |
N2—N1—Pb | 116.13 (15) | C10—C9—H9 | 118.6 |
C8—N2—N1 | 111.8 (2) | C11—C10—C9 | 118.9 (2) |
C9—N3—C13 | 117.9 (2) | C11—C10—H10 | 120.6 |
C9—N3—Pbii | 119.49 (17) | C9—C10—H10 | 120.6 |
C13—N3—Pbii | 121.59 (18) | C10—C11—C12 | 118.2 (2) |
O1—C1—C2 | 120.8 (2) | C10—C11—C8 | 120.7 (2) |
O1—C1—C6 | 122.2 (2) | C12—C11—C8 | 121.0 (2) |
C2—C1—C6 | 116.9 (2) | C13—C12—C11 | 119.2 (3) |
C3—C2—C1 | 122.0 (3) | C13—C12—H12 | 120.4 |
C3—C2—H2 | 119.0 | C11—C12—H12 | 120.4 |
C1—C2—H2 | 119.0 | N3—C13—C12 | 123.0 (3) |
C2—C3—C4 | 120.8 (3) | N3—C13—H13 | 118.5 |
C2—C3—H3 | 119.6 | C12—C13—H13 | 118.5 |
C4—C3—H3 | 119.6 | O3—C14—H14A | 109.5 |
C5—C4—C3 | 118.7 (3) | O3—C14—H14B | 109.5 |
C5—C4—H4 | 120.6 | H14A—C14—H14B | 109.5 |
C3—C4—H4 | 120.6 | O3—C14—H14C | 109.5 |
C4—C5—C6 | 122.1 (3) | H14A—C14—H14C | 109.5 |
C4—C5—H5 | 119.0 | H14B—C14—H14C | 109.5 |
C6—C5—H5 | 119.0 | ||
O2—Pb—O1—C1 | −23.4 (3) | O1—C1—C6—C7 | 3.9 (4) |
N1—Pb—O1—C1 | −1.6 (3) | C2—C1—C6—C7 | −178.4 (3) |
N3i—Pb—O1—C1 | −95.0 (3) | N2—N1—C7—C6 | 175.1 (3) |
O1—Pb—O2—C8 | 34.3 (2) | Pb—N1—C7—C6 | −10.7 (4) |
N1—Pb—O2—C8 | 11.55 (17) | C5—C6—C7—N1 | −174.9 (3) |
N3i—Pb—O2—C8 | 105.32 (18) | C1—C6—C7—N1 | 3.1 (5) |
O2—Pb—N1—C7 | 172.3 (3) | Pb—O2—C8—N2 | −9.3 (3) |
O1—Pb—N1—C7 | 8.1 (2) | Pb—O2—C8—C11 | 171.80 (17) |
N3i—Pb—N1—C7 | 89.5 (2) | N1—N2—C8—O2 | −3.6 (4) |
O2—Pb—N1—N2 | −13.71 (15) | N1—N2—C8—C11 | 175.3 (2) |
O1—Pb—N1—N2 | −177.83 (18) | C13—N3—C9—C10 | 0.9 (4) |
N3i—Pb—N1—N2 | −96.45 (17) | Pbii—N3—C9—C10 | −167.6 (2) |
C7—N1—N2—C8 | −170.4 (2) | N3—C9—C10—C11 | −1.2 (4) |
Pb—N1—N2—C8 | 14.4 (3) | C9—C10—C11—C12 | −0.1 (4) |
Pb—O1—C1—C2 | 179.32 (19) | C9—C10—C11—C8 | 176.4 (2) |
Pb—O1—C1—C6 | −3.1 (4) | O2—C8—C11—C10 | −17.9 (4) |
O1—C1—C2—C3 | 179.4 (3) | N2—C8—C11—C10 | 163.1 (2) |
C6—C1—C2—C3 | 1.7 (4) | O2—C8—C11—C12 | 158.5 (2) |
C1—C2—C3—C4 | −1.4 (5) | N2—C8—C11—C12 | −20.5 (4) |
C2—C3—C4—C5 | −0.2 (5) | C10—C11—C12—C13 | 1.7 (4) |
C3—C4—C5—C6 | 1.5 (5) | C8—C11—C12—C13 | −174.8 (3) |
C4—C5—C6—C1 | −1.2 (4) | C9—N3—C13—C12 | 0.9 (4) |
C4—C5—C6—C7 | 177.0 (3) | Pbii—N3—C13—C12 | 169.1 (2) |
O1—C1—C6—C5 | −178.1 (3) | C11—C12—C13—N3 | −2.2 (5) |
C2—C1—C6—C5 | −0.4 (4) |
Symmetry codes: (i) −x+y−1/3, −x+4/3, z−2/3; (ii) −y+4/3, x−y+5/3, z+2/3. |
Experimental details
Crystal data | |
Chemical formula | [Pb(C13H9N3O2)]·CH4O |
Mr | 478.46 |
Crystal system, space group | Hexagonal, R3 |
Temperature (K) | 100 |
a, c (Å) | 28.6702 (5), 9.0146 (2) |
V (Å3) | 6417.1 (3) |
Z | 18 |
Radiation type | Mo Kα |
µ (mm−1) | 11.84 |
Crystal size (mm) | 0.20 × 0.15 × 0.10 |
Data collection | |
Diffractometer | Agilent SuperNova Dual diffractometer with an Atlas detector |
Absorption correction | Multi-scan (CrysAlis PRO; Agilent, 2010) |
Tmin, Tmax | 0.349, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 17626, 2958, 2816 |
Rint | 0.026 |
(sin θ/λ)max (Å−1) | 0.628 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.015, 0.032, 1.11 |
No. of reflections | 2958 |
No. of parameters | 193 |
H-atom treatment | H-atom parameters constrained |
w = 1/[σ2(Fo2) + (0.0114P)2 + 19.9099P] where P = (Fo2 + 2Fc2)/3 | |
Δρmax, Δρmin (e Å−3) | 0.95, −0.60 |
Computer programs: CrysAlis PRO (Agilent, 2010), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2010).
Acknowledgements
The authors thank Islamic Azad University and the University of Malaya for support.
References
Agilent (2010). CrysAlis PRO. Agilent Technologies, Yarnton, Oxfordshire, England. Google Scholar
Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany. Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Harrowfield, J. M., Miyamae, H., Skelton, B. W., Soudi, A. A. & White, A. H. (1996). Aust. J. Chem. 49, 1165–1169. CSD CrossRef Web of Science Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Vrdoljak, V., Prugovečki, B., Matković-Čalogović, D. R., Dreos, R., Siega, P. & Tavagnacco, C. (2010). Cryst. Growth Des. 10, 1373–1382. Web of Science CrossRef CAS Google Scholar
Vrdoljak, V., Prugovečki, B., Matković-Calogović, D. & Pisk, P. (2011). CrystEngComm, 13, 4382–4390. Web of Science CSD CrossRef CAS Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
Yuan, Y.-Z., Zhou, J., Liu, X., Liu, L.-H. & Yu, K.-B. (2007). Inorg. Chem. Commun. 10, 475–478. Web of Science CSD CrossRef CAS Google Scholar
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2-Oxide-3-benzaldehyde isonicotinylhydrazonato ligands related to that in the title complex, (I), are attracting interest in the context of crystal engineering endeavours (Vrdoljak et al., 2010, 2011). Thus far, the only lead(II) complex reported with this class of ligand is a binuclear complex where the pyridine-N atom does not participate in coordination (Yuan et al., 2007).
The asymmetric unit of compound (I) comprises a PbII atom, a N-isonicotinamidosalicylaldiminato ligand and a methanol molecule of solvation, Fig. 1. The PbII atom is coordinated by the O,N,O atoms of the ligand and the pyridine-N atom bridges to a symmetry related PbII atom. The resultant N2O2 donor set plus the lone pair of electrons is based on a trigonal bipyramid with the O atoms in axial positions [O1—Pb—O2 = 137.27 (6)°] and the N atoms [N1—Pb—N3i = 90.94 (7)°] and lone pair in equatorial positions; symmetry operation: (i) 1/3 - x + y, 4/3 - x, -2/3 + z.
The µ2-bridging mode of the tetradentate N-isonicotinamidosalicylaldiminato ligand leads to a 31 helical chain along the c axis, Fig. 2. The considerable distortions from the ideal geometry arises from the acute chelate angles (O2—Pb—N1 = 66.59 (7)° and O1—Pb—N1 = 73.59 (7)°) as well as the close approach of other donor atoms. Examples of the latter are a methanol-O3 atom [2.959 (3) Å; symmetry operation: 1/3 - x, 5/3 - y, 5/3 - z] and a hydrazine-N2 atom [2.881 (2) Å; symmetry operation: 1/3 - x, 5/3 - y, 8/3 - z]. These interactions along with hydrogen bonding contacts between the methanol molecule of solvation and atom O1 lead to linear chains along the c axis (Fig. 3 and Table 1), i.e. providing links between the 31 chains mediated by Pb···N interactions, Fig. 4.