Literature DB >> 21201073

Poly[bis-(μ(3)-acetato-κO,O':O:O')bis-(μ(2)-acetato-κO,O':O)(μ(2)-2,5-dimethyl-benzene-1,4-diol-κO:O')dilead(II)].

Krzysztof Lyczko, Joanna Bak.   

Abstract

The title compound, [Pb(2)(C(2)H(3)O(2))(4)(C(8)H(10)O(2))](n), has a polymeric structure, with acetatolead(II) chains and 2,5-dimethyl-benzene-1,4-diol mol-ecules forming bridges between two Pb(II) ions from neighbouring chains. Each Pb(II) centre is surrounded by eight O atoms; four belong to bidentate acetate ions, three to neighbouring bridging acetate groups and one to the 2,5-dimethyl-benzene-1,4-diol mol-ecule. The Pb(II) ions are chelated symmetrically and asymmetrically by acetate ligands. The coordination environment of the Pb(II) ion can be described as a hemidirected Pb(II)O(6) core with the empty space around the metal ion filled by the stereochemically active 6s(2) electron pair and two longer Pb-O contacts. The Pb-O distances are in the range of 2.355 (3)-2.994 (3) Å. Additionally, the crystal structure is stabilized by O-H⋯O hydrogen bonds.

Entities:  

Year:  2008        PMID: 21201073      PMCID: PMC2959230          DOI: 10.1107/S1600536808030535

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

Other crystal structures containing polymeric lead(II) acetate were reported by: Rajaram & Rao (1982 ▶); Bryant et al. (1984 ▶); Harrowfield et al. (1996 ▶). Van der Waals radii of lead(II) and oxygen were presented by Bondi (1964 ▶). The synthesis of the title compound was carried out similarly to the method used for obtaining the bis­(2,4-penta­nedionato)lead(II) complex described by Lyczko et al. (2006 ▶). Hemi- and holodirected geometries of lead(II) complexes and the role of the 6s 2 lone electron pair of the lead(II) ion were discussed by Shimoni-Livny et al. (1998 ▶).

Experimental

Crystal data

[Pb2(C2H3O2)4(C8H10O2)] M = 788.72 Triclinic, a = 7.4905 (11) Å b = 7.5526 (10) Å c = 10.2522 (15) Å α = 93.043 (11)° β = 100.787 (12)° γ = 116.377 (14)° V = 504.28 (12) Å3 Z = 1 Mo Kα radiation μ = 16.72 mm−1 T = 100 (2) K 0.35 × 0.26 × 0.14 mm

Data collection

Kuma KM-4 four-circle CCD diffractometer Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2005 ▶) T min = 0.040, T max = 0.227 9065 measured reflections 2432 independent reflections 2317 reflections with I > 2σ(I) R int = 0.041

Refinement

R[F 2 > 2σ(F 2)] = 0.017 wR(F 2) = 0.043 S = 1.07 2432 reflections 132 parameters H-atom parameters constrained Δρmax = 1.30 e Å−3 Δρmin = −1.67 e Å−3 Data collection: CrysAlis CCD (Oxford Diffraction, 2005 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2005 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808030535/nc2114sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808030535/nc2114Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Pb2(C2H3O2)4(C8H10O2)]Z = 1
Mr = 788.72F(000) = 362
Triclinic, P1Dx = 2.597 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.4905 (11) ÅCell parameters from 9065 reflections
b = 7.5526 (10) Åθ = 3.0–28.7°
c = 10.2522 (15) ŵ = 16.72 mm1
α = 93.043 (11)°T = 100 K
β = 100.787 (12)°Prismatic, colourless
γ = 116.377 (14)°0.35 × 0.26 × 0.14 mm
V = 504.28 (12) Å3
Kuma KM-4 four-circle CCD diffractometer2432 independent reflections
Radiation source: fine-focus sealed tube2317 reflections with I > 2σ(I)
graphiteRint = 0.041
Detector resolution: 8.6479 pixels mm-1θmax = 28.7°, θmin = 3.1°
ω scansh = −9→9
Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2005)k = −10→10
Tmin = 0.040, Tmax = 0.227l = −13→13
9065 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.017H-atom parameters constrained
wR(F2) = 0.043w = 1/[σ2(Fo2) + (0.0223P)2 + 0.6288P] where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
2432 reflectionsΔρmax = 1.30 e Å3
132 parametersΔρmin = −1.67 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0077 (5)
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.
xyzUiso*/Ueq
Pb10.205617 (17)0.362095 (17)0.046792 (11)0.00910 (6)
O10.4490 (4)0.6463 (4)−0.0457 (2)0.0121 (5)
O20.1324 (4)0.6005 (4)−0.0858 (3)0.0154 (5)
O30.1663 (4)0.2264 (4)−0.1751 (2)0.0148 (5)
O4−0.1191 (4)0.0447 (4)−0.1145 (3)0.0214 (6)
C10.3154 (5)0.6990 (5)−0.0954 (3)0.0111 (6)
C20.3723 (6)0.8784 (6)−0.1662 (4)0.0155 (7)
H2A0.51800.9365−0.16680.023*
H2B0.34660.9780−0.11920.023*
H2C0.28960.8380−0.25890.023*
C3−0.0132 (5)0.0788 (6)−0.1992 (4)0.0135 (7)
C4−0.0903 (6)−0.0587 (6)−0.3316 (4)0.0212 (8)
H4A−0.0509−0.1658−0.32160.032*
H4B−0.03010.0174−0.40020.032*
H4C−0.2400−0.1172−0.35880.032*
C50.5070 (5)0.5941 (5)0.3871 (3)0.0124 (7)
O50.5039 (4)0.6836 (4)0.2743 (3)0.0166 (5)
H50.62160.73560.25910.025*
C60.3672 (5)0.5861 (6)0.4637 (4)0.0129 (7)
C70.3647 (5)0.4909 (5)0.5766 (3)0.0133 (7)
H70.27200.48410.63030.016*
C80.2300 (6)0.6797 (7)0.4230 (4)0.0207 (8)
H8A0.15260.67320.49140.031*
H8B0.13440.60740.33660.031*
H8C0.31330.81990.41450.031*
U11U22U33U12U13U23
Pb10.00762 (8)0.00740 (8)0.01117 (8)0.00219 (6)0.00281 (5)0.00244 (5)
O10.0087 (12)0.0098 (12)0.0179 (12)0.0040 (10)0.0032 (9)0.0049 (10)
O20.0082 (12)0.0150 (13)0.0246 (14)0.0054 (11)0.0062 (10)0.0077 (11)
O30.0130 (12)0.0112 (12)0.0157 (12)0.0012 (11)0.0048 (9)0.0017 (10)
O40.0123 (13)0.0247 (16)0.0203 (14)0.0021 (12)0.0053 (10)0.0018 (12)
C10.0119 (16)0.0087 (16)0.0123 (16)0.0048 (14)0.0025 (12)0.0006 (13)
C20.0098 (17)0.0120 (18)0.0240 (19)0.0034 (15)0.0051 (14)0.0091 (15)
C30.0107 (17)0.0115 (17)0.0151 (16)0.0037 (15)−0.0002 (13)0.0028 (14)
C40.023 (2)0.0139 (19)0.0179 (18)0.0035 (17)0.0004 (15)−0.0014 (15)
C50.0120 (16)0.0105 (17)0.0090 (15)0.0010 (14)0.0011 (12)0.0005 (13)
O50.0146 (13)0.0202 (14)0.0150 (12)0.0062 (12)0.0061 (10)0.0089 (11)
C60.0110 (17)0.0105 (16)0.0145 (16)0.0036 (14)0.0013 (12)−0.0007 (13)
C70.0109 (16)0.0128 (17)0.0133 (16)0.0029 (14)0.0038 (12)0.0001 (14)
C80.0190 (19)0.025 (2)0.0224 (19)0.0138 (18)0.0055 (15)0.0065 (16)
Pb1—O32.355 (3)C2—H2C0.9800
Pb1—O12.493 (3)C3—C41.509 (5)
Pb1—O22.499 (3)C4—H4A0.9800
Pb1—O1i2.618 (2)C4—H4B0.9800
Pb1—O42.700 (3)C4—H4C0.9800
Pb1—O2ii2.767 (3)C5—O51.372 (4)
Pb1—O52.993 (3)C5—C7iv1.384 (5)
Pb1—O4iii2.994 (3)C5—C61.405 (5)
O1—C11.267 (4)O5—H50.8400
O1—Pb1i2.618 (2)C6—C71.393 (5)
O2—C11.263 (4)C6—C81.499 (5)
O3—C31.275 (4)C7—C5iv1.384 (5)
O4—C31.245 (4)C7—H70.9500
C1—C21.500 (5)C8—H8A0.9800
C2—H2A0.9800C8—H8B0.9800
C2—H2B0.9800C8—H8C0.9800
O3—Pb1—O175.58 (9)O4—C3—O3121.2 (3)
O3—Pb1—O277.94 (9)O4—C3—C4120.8 (3)
O1—Pb1—O252.08 (8)O3—C3—C4118.0 (3)
O3—Pb1—O1i75.04 (8)C3—C4—H4A109.5
O1—Pb1—O1i66.16 (9)C3—C4—H4B109.5
O2—Pb1—O1i116.77 (8)H4A—C4—H4B109.5
O3—Pb1—O450.93 (8)C3—C4—H4C109.5
O1—Pb1—O4121.84 (8)H4A—C4—H4C109.5
O2—Pb1—O491.50 (9)H4B—C4—H4C109.5
O1i—Pb1—O4111.98 (8)O5—C5—C7iv122.7 (3)
C1—O1—Pb194.0 (2)O5—C5—C6116.7 (3)
C1—O1—Pb1i149.3 (2)C7iv—C5—C6120.6 (3)
Pb1—O1—Pb1i113.84 (9)C5—O5—H5109.5
C1—O2—Pb193.8 (2)C7—C6—C5117.4 (3)
C3—O3—Pb1101.7 (2)C7—C6—C8122.9 (3)
C3—O4—Pb186.2 (2)C5—C6—C8119.8 (3)
O2—C1—O1120.1 (3)C5iv—C7—C6122.0 (3)
O2—C1—C2119.4 (3)C5iv—C7—H7119.0
O1—C1—C2120.6 (3)C6—C7—H7119.0
C1—C2—H2A109.5C6—C8—H8A109.5
C1—C2—H2B109.5C6—C8—H8B109.5
H2A—C2—H2B109.5H8A—C8—H8B109.5
C1—C2—H2C109.5C6—C8—H8C109.5
H2A—C2—H2C109.5H8A—C8—H8C109.5
H2B—C2—H2C109.5H8B—C8—H8C109.5
O3—Pb1—O1—C186.8 (2)O2—Pb1—O4—C374.2 (2)
O2—Pb1—O1—C11.04 (19)O1i—Pb1—O4—C3−45.6 (2)
O1i—Pb1—O1—C1166.6 (3)Pb1—O2—C1—O11.9 (3)
O4—Pb1—O1—C164.6 (2)Pb1—O2—C1—C2−178.1 (3)
O3—Pb1—O1—Pb1i−79.76 (11)Pb1—O1—C1—O2−1.9 (3)
O2—Pb1—O1—Pb1i−165.57 (16)Pb1i—O1—C1—O2153.6 (3)
O1i—Pb1—O1—Pb1i0.0Pb1—O1—C1—C2178.1 (3)
O4—Pb1—O1—Pb1i−101.97 (11)Pb1i—O1—C1—C2−26.4 (6)
O3—Pb1—O2—C1−82.0 (2)Pb1—O4—C3—O3−1.8 (3)
O1—Pb1—O2—C1−1.05 (19)Pb1—O4—C3—C4175.7 (3)
O1i—Pb1—O2—C1−15.8 (2)Pb1—O3—C3—O42.1 (4)
O4—Pb1—O2—C1−131.5 (2)Pb1—O3—C3—C4−175.4 (3)
O1—Pb1—O3—C3−156.6 (2)O5—C5—C6—C7178.3 (3)
O2—Pb1—O3—C3−103.1 (2)C7iv—C5—C6—C70.3 (6)
O1i—Pb1—O3—C3134.7 (2)O5—C5—C6—C8−2.3 (5)
O4—Pb1—O3—C3−1.1 (2)C7iv—C5—C6—C8179.8 (4)
O3—Pb1—O4—C31.1 (2)C5—C6—C7—C5iv−0.3 (6)
O1—Pb1—O4—C329.2 (2)C8—C6—C7—C5iv−179.8 (4)
D—H···AD—HH···AD···AD—H···A
O5—H5···O3i0.841.872.668 (4)159.
Table 1

Selected bond lengths (Å)

Pb1—O32.355 (3)
Pb1—O12.493 (3)
Pb1—O22.499 (3)
Pb1—O1i2.618 (2)
Pb1—O42.700 (3)
Pb1—O2ii2.767 (3)
Pb1—O52.993 (3)
Pb1—O4iii2.994 (3)

Symmetry codes: (i) ; (ii) ; (iii) .

Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O5—H5⋯O3i0.841.872.668 (4)159

Symmetry code: (i) .

  2 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Crystal structure of lead(II) acetylacetonate and the structure of the acetylacetone solvated lead(II) ion in solution studied by large-angle X-ray scattering.

Authors:  Krzysztof Lyczko; Jerzy Narbutt; Beata Paluchowska; Jan K Maurin; Ingmar Persson
Journal:  Dalton Trans       Date:  2006-06-13       Impact factor: 4.390

  2 in total
  1 in total

1.  Crystal structures of three lead(II) acetate-bridged di-amino-benzene coordination polymers.

Authors:  David K Geiger; Dylan E Parsons; Patricia L Zick
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2014-11-21
  1 in total

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