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In the title compound, [Pb2(C12H6O4)2(C12H8N2)]n or [Pb2(1,4-NDC)2(L)]n, where 1,4-NDC is naphthalene-1,4-dicarboxyl­ate and L is 1,10-phenanthroline, the 1,4-NDC ligands link the PbII atoms into a layer structure. One Pb atom is ligated by L and also bonded to four 1,4-NDC O atoms and the other Pb atom bonds only to six 1,4-NDC O atoms. The lone pairs of the Pb atoms appear to be stereochemically active. Aromatic π–π stacking between L and 1,4-NDC ligands in adjacent layers helps to establish the packing [minimum centroid–centroid separation = 3.505 (3) Å].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807050702/hb2579sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807050702/hb2579Isup2.hkl
Contains datablock I

CCDC reference: 667184

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.008 Å
  • R factor = 0.024
  • wR factor = 0.046
  • Data-to-parameter ratio = 15.7

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 2.86 Ratio PLAT220_ALERT_2_C Large Non-Solvent O Ueq(max)/Ueq(min) ... 3.42 Ratio PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for O1 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C12
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.47 From the CIF: _reflns_number_total 6786 Count of symmetry unique reflns 3554 Completeness (_total/calc) 190.94% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 3232 Fraction of Friedel pairs measured 0.909 Are heavy atom types Z>Si present yes PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K PLAT791_ALERT_1_G Confirm the Absolute Configuration of C12 = . R PLAT794_ALERT_5_G Check Predicted Bond Valency for Pb1 (2) 2.04 PLAT794_ALERT_5_G Check Predicted Bond Valency for Pb2 (2) 2.02 PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 7 ALERT level G = General alerts; check 3 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 4 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 2 ALERT type 5 Informative message, check

Comment top

Lead(II), with its large radius, flexible coordination environment, and variable stereochemical activity, provides unique opportunities for formation of unusual coordination polymer network topologies with interesting properties (Fan & Zhu, 2006; 2007). Herein, we present a new Pb(II) coordination polymer, namely the title compound, (I), [Pb2(1,4-NDC)2(L)], where L= 1,10-phenanthroline and 1,4-NDC =naphthalene-1,4-dicarboxylate.

Selected bond lengthes and angles are listed in Table 1. In compound (I) there exist two 1,4-NDC dianions, one L ligand and two crystallographically independent Pb(II) atoms (Fig. 1). Pb1 is six-coordinated by six carboxylate O atoms from four 1,4-NDC ligands, and its lone pair of electrons appears to be stereochemically active. Atom Pb2 is also six-coordinated, by two N atoms from one chelating L ligand, and four carboxylate O atoms from three 1,4-NDC ligands, while the lone pair of electrons completes its environment. The 1,4-NDC dianions link neighboring Pb(II) atoms to generate a layer structure and the L ligands are located on both sides of the layers (Fig. 2). Moreover, the neighboring layers interact through π-π forces between L and 1,4-NDC ligands, forming a three-dimensional supramolecular structure.

Related literature top

For studies on related lead(II) carboxylates, see Fan & Zhu (2006) and (2007).

Experimental top

A mixture of Pb(NO3)2 (1 mmol), 1,4-H2NDC (1 mmol) and L (1 mmol) were dissolved in 15 ml distilled water, followed by addition of triethylamine until the pH value of the system was adjusted to about 6. The resulting solution was sealed in a 23-ml Teflon-lined stainless steel autoclave and heated at 453 K for 7 days under autogenous pressure. Afterwards, the reaction system was slowly cooled to room temperature. Colourless slabs and plates of (I) were collected.

Refinement top

All the H atoms were generated geometrically (C—H = 0.93 Å) and refined as riding with Uiso(H)= 1.2Ueq(C).

Structure description top

Lead(II), with its large radius, flexible coordination environment, and variable stereochemical activity, provides unique opportunities for formation of unusual coordination polymer network topologies with interesting properties (Fan & Zhu, 2006; 2007). Herein, we present a new Pb(II) coordination polymer, namely the title compound, (I), [Pb2(1,4-NDC)2(L)], where L= 1,10-phenanthroline and 1,4-NDC =naphthalene-1,4-dicarboxylate.

Selected bond lengthes and angles are listed in Table 1. In compound (I) there exist two 1,4-NDC dianions, one L ligand and two crystallographically independent Pb(II) atoms (Fig. 1). Pb1 is six-coordinated by six carboxylate O atoms from four 1,4-NDC ligands, and its lone pair of electrons appears to be stereochemically active. Atom Pb2 is also six-coordinated, by two N atoms from one chelating L ligand, and four carboxylate O atoms from three 1,4-NDC ligands, while the lone pair of electrons completes its environment. The 1,4-NDC dianions link neighboring Pb(II) atoms to generate a layer structure and the L ligands are located on both sides of the layers (Fig. 2). Moreover, the neighboring layers interact through π-π forces between L and 1,4-NDC ligands, forming a three-dimensional supramolecular structure.

For studies on related lead(II) carboxylates, see Fan & Zhu (2006) and (2007).

Computing details top

Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO (Rigaku, 1998); data reduction: PROCESS-AUTO (Rigaku, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL-Plus (Sheldrick, 1990); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of (I) expanded to show the lead coordination spheres, with displacement ellipsoids for the non-hydrogen atoms drawn at the 30% probability level. H atoms omitted for clarity. Symmetry codes: (i) 1 - x, y - 1/2, 1 - z; (ii) 1 - x, y + 1/2, 2 - z; (iii) 1 - x, y - 1/2, 1 - z.
[Figure 2] Fig. 2. : The extended layer structure of (I). The hydrogen atoms are omitted for clarity.
(1E,4E)-1,5-Bis(2-chlorophenyl)penta-1,4-dien-3-one top
Crystal data top
[Pb2(C12H6O4)2(C12H8N2)]F(000) = 956
Mr = 1022.92Dx = 2.276 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 14193 reflections
a = 7.063 (3) Åθ = 3.0–27.5°
b = 14.602 (5) ŵ = 11.33 mm1
c = 14.526 (5) ÅT = 293 K
β = 94.922 (5)°Slab, colourless
V = 1492.6 (10) Å30.29 × 0.15 × 0.09 mm
Z = 2
Data collection top
Rigaku R-AXIS RAPID
diffractometer
6786 independent reflections
Radiation source: rotating anode6429 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.036
Detector resolution: 10.0 pixels mm-1θmax = 27.5°, θmin = 3.1°
ω scansh = 97
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
k = 1818
Tmin = 0.141, Tmax = 0.368l = 1818
14649 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.024H-atom parameters constrained
wR(F2) = 0.046 w = 1/[σ2(Fo2)]
where P = (Fo2 + 2Fc2)/3
S = 0.91(Δ/σ)max = 0.001
6786 reflectionsΔρmax = 0.60 e Å3
433 parametersΔρmin = 1.06 e Å3
1 restraintAbsolute structure: Flack (1983), 3232 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.011 (5)
Crystal data top
[Pb2(C12H6O4)2(C12H8N2)]V = 1492.6 (10) Å3
Mr = 1022.92Z = 2
Monoclinic, P21Mo Kα radiation
a = 7.063 (3) ŵ = 11.33 mm1
b = 14.602 (5) ÅT = 293 K
c = 14.526 (5) Å0.29 × 0.15 × 0.09 mm
β = 94.922 (5)°
Data collection top
Rigaku R-AXIS RAPID
diffractometer
6786 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
6429 reflections with I > 2σ(I)
Tmin = 0.141, Tmax = 0.368Rint = 0.036
14649 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.024H-atom parameters constrained
wR(F2) = 0.046Δρmax = 0.60 e Å3
S = 0.91Δρmin = 1.06 e Å3
6786 reflectionsAbsolute structure: Flack (1983), 3232 Friedel pairs
433 parametersAbsolute structure parameter: 0.011 (5)
1 restraint
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
xyzUiso*/Ueq
C10.8600 (7)0.3121 (4)0.8347 (4)0.0310 (11)
C20.8383 (7)0.3959 (3)0.8940 (4)0.0262 (11)
C30.6962 (7)0.3962 (4)0.9510 (4)0.0375 (12)
H30.61890.34480.95240.045*
C40.6608 (8)0.4704 (4)1.0076 (4)0.0396 (13)
H40.55890.46861.04410.048*
C50.7767 (7)0.5462 (3)1.0094 (4)0.0339 (12)
C60.9682 (7)0.4729 (3)0.8950 (3)0.0254 (10)
C71.1281 (7)0.4789 (3)0.8432 (4)0.0349 (11)
H71.14880.43350.80040.042*
C81.2530 (8)0.5502 (3)0.8549 (5)0.0453 (15)
H81.35930.55140.82130.054*
C91.2242 (8)0.6206 (4)0.9159 (4)0.0447 (14)
H91.31190.66810.92380.054*
C101.0669 (8)0.6206 (3)0.9645 (4)0.0435 (13)
H101.04600.66951.00330.052*
C130.3703 (7)0.1061 (3)0.6647 (4)0.0242 (10)
C140.3748 (6)0.0248 (3)0.6024 (3)0.0212 (9)
C150.4044 (6)0.0375 (3)0.5120 (4)0.0289 (10)
H160.42430.09620.49000.035*
C160.4051 (7)0.0378 (3)0.4518 (4)0.0305 (11)
H170.43090.02850.39080.037*
C170.3689 (6)0.1242 (3)0.4810 (4)0.0273 (10)
C200.3402 (6)0.1398 (3)0.5757 (3)0.0242 (10)
C240.3427 (6)0.0644 (3)0.6368 (4)0.0251 (10)
C230.3107 (7)0.0790 (3)0.7304 (4)0.0320 (11)
H230.31090.02910.77020.038*
C190.3103 (7)0.2291 (3)0.6133 (4)0.0351 (12)
H130.31000.28020.57510.042*
C210.2826 (8)0.2399 (4)0.7039 (4)0.0438 (13)
H210.26520.29850.72680.053*
C310.7904 (8)0.2644 (4)0.6450 (6)0.056 (2)
H310.77160.32600.65780.067*
C320.8171 (8)0.2400 (4)0.5597 (5)0.0478 (15)
H320.81740.28460.51400.057*
C270.8455 (7)0.1461 (4)0.5359 (5)0.0411 (14)
C260.8780 (7)0.1184 (4)0.4484 (4)0.0460 (14)
H260.88080.16180.40170.055*
C280.8420 (6)0.0786 (3)0.6056 (4)0.0327 (12)
C290.8154 (7)0.1041 (3)0.6991 (4)0.0313 (11)
C350.7991 (8)0.0630 (4)0.8511 (4)0.0467 (14)
H350.80080.01780.89630.056*
C360.8966 (7)0.0346 (4)0.4998 (4)0.0423 (13)
H360.91390.09620.48640.051*
C180.3599 (8)0.1990 (3)0.4078 (4)0.0370 (12)
C300.7893 (8)0.1983 (4)0.7199 (5)0.0459 (16)
C120.7355 (8)0.6235 (3)1.0724 (4)0.0381 (12)
C220.2796 (8)0.1646 (4)0.7639 (4)0.0425 (13)
H220.25680.17290.82550.051*
C340.7771 (10)0.1539 (5)0.8771 (5)0.0610 (19)
H340.76730.16890.93880.073*
C110.9371 (7)0.5482 (3)0.9567 (4)0.0280 (11)
C250.9060 (8)0.0290 (5)0.4290 (5)0.0552 (17)
H250.93090.01050.37000.066*
C330.7700 (10)0.2208 (4)0.8114 (6)0.0587 (19)
H330.75220.28150.82790.070*
N10.8641 (5)0.0117 (3)0.5859 (3)0.0305 (9)
N20.8177 (6)0.0382 (3)0.7636 (3)0.0348 (10)
O10.9883 (6)0.3066 (3)0.7806 (4)0.0512 (12)
O20.7379 (5)0.2472 (2)0.8418 (3)0.0323 (8)
O30.5033 (4)0.1186 (2)0.7271 (3)0.0312 (8)
O40.2304 (4)0.1607 (2)0.6549 (2)0.0297 (8)
O50.4507 (6)0.1824 (3)0.3387 (3)0.0577 (12)
O60.2628 (6)0.2688 (2)0.4181 (3)0.0498 (11)
O70.8192 (7)0.6248 (3)1.1507 (3)0.0593 (12)
O80.6205 (9)0.6829 (4)1.0446 (4)0.102 (2)
Pb10.38951 (3)0.256319 (9)0.794522 (12)0.02560 (5)
Pb20.86603 (2)0.137997 (11)0.714247 (12)0.02589 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.028 (2)0.036 (3)0.028 (3)0.005 (2)0.002 (2)0.008 (2)
C20.028 (2)0.026 (2)0.025 (3)0.0022 (19)0.002 (2)0.008 (2)
C30.044 (3)0.041 (3)0.028 (3)0.013 (2)0.007 (2)0.011 (2)
C40.040 (3)0.051 (3)0.030 (3)0.004 (2)0.014 (2)0.011 (3)
C50.043 (3)0.039 (3)0.019 (3)0.003 (2)0.003 (2)0.010 (2)
C60.030 (2)0.024 (2)0.022 (3)0.0012 (18)0.001 (2)0.0037 (19)
C70.044 (3)0.028 (2)0.035 (3)0.002 (2)0.014 (2)0.003 (2)
C80.046 (3)0.035 (3)0.057 (4)0.003 (2)0.013 (3)0.005 (3)
C90.050 (3)0.038 (3)0.045 (4)0.017 (2)0.000 (3)0.000 (3)
C100.059 (3)0.034 (3)0.036 (3)0.007 (2)0.003 (3)0.008 (2)
C130.030 (2)0.020 (2)0.024 (3)0.0000 (18)0.011 (2)0.0026 (19)
C140.0170 (19)0.022 (2)0.025 (2)0.0028 (16)0.0033 (18)0.0021 (19)
C150.029 (2)0.028 (2)0.029 (3)0.0007 (19)0.002 (2)0.002 (2)
C160.032 (2)0.035 (2)0.025 (3)0.002 (2)0.005 (2)0.005 (2)
C170.023 (2)0.026 (2)0.032 (3)0.0041 (18)0.004 (2)0.009 (2)
C200.023 (2)0.026 (2)0.023 (2)0.0007 (17)0.0015 (19)0.0041 (19)
C240.022 (2)0.026 (2)0.028 (3)0.0006 (18)0.002 (2)0.001 (2)
C230.037 (3)0.032 (2)0.028 (3)0.003 (2)0.011 (2)0.008 (2)
C190.040 (3)0.021 (2)0.044 (3)0.0028 (19)0.002 (2)0.008 (2)
C210.055 (3)0.029 (2)0.047 (3)0.008 (3)0.004 (3)0.008 (3)
C310.046 (3)0.026 (3)0.093 (6)0.000 (2)0.012 (4)0.015 (3)
C320.040 (3)0.033 (3)0.069 (5)0.001 (2)0.006 (3)0.023 (3)
C270.019 (2)0.041 (3)0.063 (4)0.001 (2)0.001 (3)0.020 (3)
C260.033 (3)0.063 (4)0.042 (4)0.004 (3)0.007 (3)0.029 (3)
C280.022 (2)0.033 (2)0.043 (3)0.0004 (19)0.000 (2)0.008 (2)
C290.027 (2)0.022 (2)0.044 (3)0.0011 (18)0.004 (2)0.004 (2)
C350.051 (3)0.055 (3)0.033 (3)0.001 (3)0.001 (3)0.001 (3)
C360.035 (3)0.054 (3)0.038 (3)0.005 (2)0.008 (2)0.006 (3)
C180.047 (3)0.034 (3)0.030 (3)0.012 (2)0.001 (3)0.008 (2)
C300.036 (3)0.031 (3)0.068 (5)0.003 (2)0.010 (3)0.001 (3)
C120.045 (3)0.033 (3)0.037 (3)0.001 (2)0.006 (2)0.012 (2)
C220.057 (3)0.041 (3)0.030 (3)0.003 (3)0.008 (3)0.005 (3)
C340.062 (4)0.069 (4)0.049 (4)0.010 (3)0.011 (3)0.023 (4)
C110.036 (3)0.024 (2)0.023 (3)0.003 (2)0.002 (2)0.008 (2)
C250.039 (3)0.090 (5)0.038 (4)0.011 (3)0.013 (3)0.015 (4)
C330.065 (4)0.039 (3)0.069 (5)0.005 (3)0.012 (4)0.017 (3)
N10.0249 (19)0.028 (2)0.038 (3)0.0016 (16)0.0030 (19)0.0051 (19)
N20.036 (2)0.033 (2)0.035 (3)0.0005 (17)0.003 (2)0.002 (2)
O10.052 (2)0.039 (2)0.066 (3)0.0082 (19)0.027 (2)0.028 (2)
O20.0352 (17)0.0233 (16)0.038 (2)0.0018 (14)0.0003 (15)0.0073 (16)
O30.0340 (17)0.0242 (16)0.034 (2)0.0008 (13)0.0019 (15)0.0047 (15)
O40.0290 (17)0.0328 (18)0.0279 (19)0.0069 (13)0.0045 (15)0.0033 (15)
O50.081 (3)0.050 (2)0.046 (3)0.002 (2)0.027 (3)0.022 (2)
O60.069 (3)0.034 (2)0.046 (3)0.0107 (19)0.000 (2)0.0143 (18)
O70.090 (3)0.052 (3)0.034 (2)0.015 (2)0.007 (2)0.014 (2)
O80.121 (5)0.100 (4)0.076 (4)0.071 (4)0.050 (4)0.056 (3)
Pb10.03473 (10)0.02015 (8)0.02271 (9)0.00014 (7)0.00705 (7)0.00040 (8)
Pb20.02927 (9)0.02153 (8)0.02683 (10)0.00054 (7)0.00221 (7)0.00271 (8)
Geometric parameters (Å, º) top
C1—O11.252 (7)C31—C321.319 (10)
C1—O21.291 (6)C31—C301.454 (9)
C1—C21.512 (7)C31—H310.9300
C2—C31.355 (7)C32—C271.432 (8)
C2—C61.450 (7)C32—H320.9300
C3—C41.396 (7)C27—C261.372 (9)
C3—H30.9300C27—C281.413 (7)
C4—C51.375 (7)C26—C251.354 (9)
C4—H40.9300C26—H260.9300
C5—C111.420 (7)C28—N11.362 (6)
C5—C121.498 (7)C28—C291.436 (8)
C6—C71.412 (7)C29—N21.341 (7)
C6—C111.447 (6)C29—C301.425 (7)
C7—C81.365 (7)C35—N21.339 (8)
C7—H70.9300C35—C341.392 (8)
C8—C91.383 (8)C35—H350.9300
C8—H80.9300C36—N11.333 (7)
C9—C101.366 (9)C36—C251.391 (9)
C9—H90.9300C36—H360.9300
C10—C111.397 (7)C18—O61.245 (6)
C10—H100.9300C18—O51.261 (7)
C13—O31.261 (6)C30—C331.386 (10)
C13—O41.268 (6)C12—O81.232 (7)
C13—C141.495 (6)C12—O71.236 (7)
C14—C151.359 (7)C22—H220.9300
C14—C241.420 (6)C34—C331.364 (10)
C15—C161.406 (7)C34—H340.9300
C15—H160.9300C25—H250.9300
C16—C171.362 (7)C33—H330.9300
C16—H170.9300Pb2—N12.622 (4)
C17—C201.426 (7)Pb2—N22.701 (4)
C17—C181.522 (7)Pb2—O12.756 (4)
C20—C241.413 (6)Pb2—O22.661 (4)
C20—C191.436 (6)Pb2—O32.600 (4)
C24—C231.415 (7)Pb2—O6i2.464 (4)
C23—C221.366 (7)Pb1—O22.501 (4)
C23—H230.9300Pb1—O32.405 (3)
C19—C211.356 (8)Pb1—O42.633 (3)
C19—H130.9300Pb1—O5i2.488 (4)
C21—C221.404 (8)Pb1—O7ii2.588 (4)
C21—H210.9300Pb1—O8ii2.577 (5)
O1—C1—O2121.8 (5)N2—C35—C34122.5 (6)
O1—C1—C2121.6 (4)N2—C35—H35118.7
O2—C1—C2116.6 (4)C34—C35—H35118.7
C3—C2—C6119.5 (4)N1—C36—C25123.3 (6)
C3—C2—C1117.9 (4)N1—C36—H36118.4
C6—C2—C1122.6 (4)C25—C36—H36118.4
C2—C3—C4122.8 (5)O6—C18—O5125.2 (5)
C2—C3—H3118.6O6—C18—C17119.6 (5)
C4—C3—H3118.6O5—C18—C17115.2 (5)
C5—C4—C3120.0 (5)C33—C30—C29117.2 (6)
C5—C4—H4120.0C33—C30—C31124.6 (6)
C3—C4—H4120.0C29—C30—C31118.2 (6)
C4—C5—C11120.5 (5)O8—C12—O7122.7 (5)
C4—C5—C12118.1 (5)O8—C12—C5119.2 (5)
C11—C5—C12121.2 (4)O7—C12—C5118.1 (5)
C7—C6—C11117.0 (4)C23—C22—C21118.9 (5)
C7—C6—C2125.2 (4)C23—C22—H22120.5
C11—C6—C2117.8 (4)C21—C22—H22120.5
C8—C7—C6121.2 (5)C33—C34—C35119.4 (7)
C8—C7—H7119.4C33—C34—H34120.3
C6—C7—H7119.4C35—C34—H34120.3
C7—C8—C9121.2 (6)C10—C11—C5121.4 (5)
C7—C8—H8119.4C10—C11—C6119.4 (5)
C9—C8—H8119.4C5—C11—C6119.2 (4)
C10—C9—C8120.0 (5)C26—C25—C36118.2 (6)
C10—C9—H9120.0C26—C25—H25120.9
C8—C9—H9120.0C36—C25—H25120.9
C9—C10—C11121.1 (5)C34—C33—C30120.1 (6)
C9—C10—H10119.5C34—C33—H33120.0
C11—C10—H10119.5C30—C33—H33120.0
O3—C13—O4121.0 (4)C36—N1—C28118.2 (5)
O3—C13—C14119.8 (4)C36—N1—Pb2120.0 (3)
O4—C13—C14119.2 (4)C28—N1—Pb2121.7 (4)
C15—C14—C24120.5 (5)C35—N2—C29118.3 (5)
C15—C14—C13119.3 (4)C35—N2—Pb2122.3 (4)
C24—C14—C13120.2 (4)C29—N2—Pb2119.4 (4)
C14—C15—C16120.2 (4)C1—O1—Pb293.1 (3)
C14—C15—H16119.9C1—O2—Pb1125.9 (3)
C16—C15—H16119.9C1—O2—Pb296.6 (3)
C17—C16—C15121.3 (5)Pb1—O2—Pb2103.08 (12)
C17—C16—H17119.3C13—O3—Pb199.2 (3)
C15—C16—H17119.3C13—O3—Pb2130.0 (3)
C16—C17—C20119.6 (4)Pb1—O3—Pb2107.69 (11)
C16—C17—C18116.4 (5)C13—O4—Pb188.3 (3)
C20—C17—C18124.0 (4)C18—O5—Pb1iii147.8 (4)
C24—C20—C17119.1 (4)C18—O6—Pb2iii121.9 (4)
C24—C20—C19117.6 (5)C12—O7—Pb1iv93.1 (3)
C17—C20—C19123.3 (4)C12—O8—Pb1iv93.7 (4)
C20—C24—C23119.4 (4)O3—Pb1—O5i78.12 (14)
C20—C24—C14119.2 (5)O3—Pb1—O273.26 (11)
C23—C24—C14121.4 (4)O5i—Pb1—O274.42 (14)
C22—C23—C24121.6 (5)O3—Pb1—O8ii93.29 (19)
C22—C23—H23119.2O5i—Pb1—O8ii154.69 (18)
C24—C23—H23119.2O2—Pb1—O8ii80.32 (17)
C21—C19—C20120.8 (5)O3—Pb1—O7ii73.96 (14)
C21—C19—H13119.6O5i—Pb1—O7ii144.51 (15)
C20—C19—H13119.6O2—Pb1—O7ii116.68 (13)
C19—C21—C22121.5 (5)O8ii—Pb1—O7ii49.58 (14)
C19—C21—H21119.2O3—Pb1—O451.57 (10)
C22—C21—H21119.2O5i—Pb1—O477.52 (14)
C32—C31—C30122.3 (6)O2—Pb1—O4121.87 (10)
C32—C31—H31118.8O8ii—Pb1—O4115.74 (14)
C30—C31—H31118.8O7ii—Pb1—O468.07 (13)
C31—C32—C27121.3 (6)O6i—Pb2—O379.40 (14)
C31—C32—H32119.4O6i—Pb2—N181.63 (14)
C27—C32—H32119.4O3—Pb2—N191.69 (11)
C26—C27—C28118.2 (5)O6i—Pb2—O295.01 (13)
C26—C27—C32122.9 (6)O3—Pb2—O267.62 (10)
C28—C27—C32118.9 (6)N1—Pb2—O2159.28 (11)
C25—C26—C27121.1 (6)O6i—Pb2—N2133.35 (14)
C25—C26—H26119.5O3—Pb2—N274.31 (11)
C27—C26—H26119.5N1—Pb2—N261.68 (14)
N1—C28—C27121.0 (5)O2—Pb2—N2109.14 (13)
N1—C28—C29118.4 (5)O6i—Pb2—O182.13 (15)
C27—C28—C29120.6 (5)O3—Pb2—O1110.68 (10)
N2—C29—C30122.5 (6)N1—Pb2—O1149.26 (13)
N2—C29—C28118.8 (4)O2—Pb2—O148.41 (11)
C30—C29—C28118.7 (5)N2—Pb2—O1143.27 (15)
Symmetry codes: (i) x+1, y1/2, z+1; (ii) x+1, y+1/2, z+2; (iii) x+1, y+1/2, z+1; (iv) x+1, y1/2, z+2.

Experimental details

Crystal data
Chemical formula[Pb2(C12H6O4)2(C12H8N2)]
Mr1022.92
Crystal system, space groupMonoclinic, P21
Temperature (K)293
a, b, c (Å)7.063 (3), 14.602 (5), 14.526 (5)
β (°) 94.922 (5)
V3)1492.6 (10)
Z2
Radiation typeMo Kα
µ (mm1)11.33
Crystal size (mm)0.29 × 0.15 × 0.09
Data collection
DiffractometerRigaku R-AXIS RAPID
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.141, 0.368
No. of measured, independent and
observed [I > 2σ(I)] reflections
14649, 6786, 6429
Rint0.036
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.024, 0.046, 0.91
No. of reflections6786
No. of parameters433
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.60, 1.06
Absolute structureFlack (1983), 3232 Friedel pairs
Absolute structure parameter0.011 (5)

Computer programs: PROCESS-AUTO (Rigaku, 1998), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL-Plus (Sheldrick, 1990).

Selected bond lengths (Å) top
Pb2—N12.622 (4)Pb1—O22.501 (4)
Pb2—N22.701 (4)Pb1—O32.405 (3)
Pb2—O12.756 (4)Pb1—O42.633 (3)
Pb2—O22.661 (4)Pb1—O5i2.488 (4)
Pb2—O32.600 (4)Pb1—O7ii2.588 (4)
Pb2—O6i2.464 (4)Pb1—O8ii2.577 (5)
Symmetry codes: (i) x+1, y1/2, z+1; (ii) x+1, y+1/2, z+2.
 

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