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In the title compound, [Pb(C8H4O4)(C24H16N2)]n, the benzene-1,4-dicarboxyl­ate (1,4-BDC) dianions link the PbII atoms to form a chain structure. The PbII atom is coordinated by 4,7-diphenyl-1,10-phenanthroline (L) and is also bonded to four 1,4-BDC O atoms, resulting in a very distorted cis-PbN2O4 octa­hedron. There are two 1,4-BDC half-anions in the asymmetric unit, both completed by inversion. Aromatic π–π stacking between L ligands in adjacent chains results in a two-dimensional supra­molecular layer structure [minimum centroid–centroid separation 3.464 (5) Å].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807051859/hb2600sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807051859/hb2600Isup2.hkl
Contains datablock I

CCDC reference: 667213

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.026
  • wR factor = 0.082
  • Data-to-parameter ratio = 16.6

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT154_ALERT_1_C The su's on the Cell Angles are Equal (x 10000) 3000 Deg. PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 2.55 Ratio PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for O4 PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C28
Alert level G PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K PLAT794_ALERT_5_G Check Predicted Bond Valency for Pb1 (2) 2.02
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 5 ALERT level C = Check and explain 3 ALERT level G = General alerts; check 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Comment top

The design and synthesis of coordination polymers is one of the most active areas of materials research. In this regard, many of the efforts have so far been devoted to the study of transition-metal based coordination polymers. However, relatively little attention has been paid to the coordination polymers of main group metal ions despite their interesting network topologies and properties (Fan & Zhu, 2007; Yang et al., 2007). Herein, we present a new Pb(II) coordination polymer, namely the title compound, (I), [Pb(1,4-BDC)(L)], where 1,4-BDC = the benzene-1,4-dicarboxylate dianion and L = 4,7-diphenyl-1,10-phenanthroline.

Selected bond lengths and angles are listed in Table 1. In compound (I) the PbII atom is six-coordinated by four carboxylate O atoms from two different 1,4-BDC ligands, and two N atoms from one L ligand (Fig. 1). This results in a very distorted cis-PbN2O4 octahedron (Table 1). The centrosymmetric 1,4-BDC dianions bridge neighboring Pb(II) atoms to form a chain structure and the L ligands are attached on both sides of the chains (Fig. 2). In addition, the neighboring chains interact through π-π forces between L ligands, leading to a two-dimensional supramolecular layer structure [minimum centroid-centroid separation = 3.464 (5) Å].

Related literature top

For studies on related lead(II) carboxylates, see: Fan & Zhu (2007); Yang et al. (2007).

Experimental top

A mixture of Pb(NO3)2 (2 mmol), 1,4-H2BDC (2 mmol) and L (2 mmol) were dissolved in 14 ml distilled water, followed by addition of triethylamine until the pH of the system was adjusted to about 5.8. The resulting solution was sealed in a 23-ml Teflon-lined stainless steel autoclave and heated at 455 K for 6 days under autogenous pressure. Afterwards, the reaction system was slowly cooled to room temperature. Colourless blocks 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

The design and synthesis of coordination polymers is one of the most active areas of materials research. In this regard, many of the efforts have so far been devoted to the study of transition-metal based coordination polymers. However, relatively little attention has been paid to the coordination polymers of main group metal ions despite their interesting network topologies and properties (Fan & Zhu, 2007; Yang et al., 2007). Herein, we present a new Pb(II) coordination polymer, namely the title compound, (I), [Pb(1,4-BDC)(L)], where 1,4-BDC = the benzene-1,4-dicarboxylate dianion and L = 4,7-diphenyl-1,10-phenanthroline.

Selected bond lengths and angles are listed in Table 1. In compound (I) the PbII atom is six-coordinated by four carboxylate O atoms from two different 1,4-BDC ligands, and two N atoms from one L ligand (Fig. 1). This results in a very distorted cis-PbN2O4 octahedron (Table 1). The centrosymmetric 1,4-BDC dianions bridge neighboring Pb(II) atoms to form a chain structure and the L ligands are attached on both sides of the chains (Fig. 2). In addition, the neighboring chains interact through π-π forces between L ligands, leading to a two-dimensional supramolecular layer structure [minimum centroid-centroid separation = 3.464 (5) Å].

For studies on related lead(II) carboxylates, see: Fan & Zhu (2007); Yang et al. (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 complete 1,4-BDC molecules, with displacement ellipsoids for the non-hydrogen atoms drawn at the 30% probability level. H atoms omitted for clarity. Symmetry codes: (i) 2 - x, 1 - y, 1 - z; (ii) 1 - x, 1 - y, 2 - z.
[Figure 2] Fig. 2. View of the chain structure of (I). The hydrogen atoms are omitted for clarity.
[Figure 3] Fig. 3. View of the supramolecular layer structure of (I). The hydrogen atoms are omitted for clarity.
catena-Poly[[(4,7-diphenyl-1,10-phenanthroline)lead(II)]-µ-benzene- 1,4-dicarboxylato] top
Crystal data top
[Pb(C8H4O4)(C24H16N2)]Z = 2
Mr = 703.69F(000) = 680
Triclinic, P1Dx = 1.811 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.855 (2) ÅCell parameters from 11906 reflections
b = 10.046 (2) Åθ = 3.0–27.5°
c = 13.539 (3) ŵ = 6.58 mm1
α = 100.36 (3)°T = 293 K
β = 101.14 (3)°Block, colorless
γ = 92.04 (3)°0.27 × 0.17 × 0.08 mm
V = 1290.2 (4) Å3
Data collection top
Rigaku R-AXIS RAPID
diffractometer
5855 independent reflections
Radiation source: rotating anode5326 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.026
Detector resolution: 10.0 pixels mm-1θmax = 27.5°, θmin = 3.0°
ω scansh = 1212
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
k = 1311
Tmin = 0.275, Tmax = 0.592l = 1717
12741 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.026Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.082H-atom parameters constrained
S = 1.12 w = 1/[σ2(Fo2) + (0.0487P)2 + 0.7324P]
where P = (Fo2 + 2Fc2)/3
5855 reflections(Δ/σ)max = 0.001
352 parametersΔρmax = 0.80 e Å3
0 restraintsΔρmin = 0.98 e Å3
Crystal data top
[Pb(C8H4O4)(C24H16N2)]γ = 92.04 (3)°
Mr = 703.69V = 1290.2 (4) Å3
Triclinic, P1Z = 2
a = 9.855 (2) ÅMo Kα radiation
b = 10.046 (2) ŵ = 6.58 mm1
c = 13.539 (3) ÅT = 293 K
α = 100.36 (3)°0.27 × 0.17 × 0.08 mm
β = 101.14 (3)°
Data collection top
Rigaku R-AXIS RAPID
diffractometer
5855 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
5326 reflections with I > 2σ(I)
Tmin = 0.275, Tmax = 0.592Rint = 0.026
12741 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0260 restraints
wR(F2) = 0.082H-atom parameters constrained
S = 1.12Δρmax = 0.80 e Å3
5855 reflectionsΔρmin = 0.98 e Å3
352 parameters
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
C10.7524 (5)0.5869 (5)0.5700 (4)0.0294 (9)
C20.8815 (4)0.5438 (4)0.5338 (3)0.0277 (9)
C31.0097 (5)0.5650 (5)0.6012 (4)0.0338 (10)
H31.01640.60880.66880.041*
C40.8726 (5)0.4795 (5)0.4329 (4)0.0342 (10)
H40.78720.46600.38770.041*
C50.5244 (5)0.6112 (5)0.8194 (4)0.0354 (10)
C60.5120 (5)0.5544 (5)0.9137 (3)0.0306 (9)
C70.4760 (5)0.6338 (5)0.9975 (4)0.0329 (10)
H70.46040.72430.99630.039*
C80.5374 (5)0.4184 (5)0.9160 (4)0.0339 (10)
H80.56300.36380.86050.041*
C90.5850 (6)0.7681 (5)0.3916 (4)0.0356 (11)
H90.53020.68690.36970.043*
C100.6482 (6)0.8187 (5)0.3207 (4)0.0380 (11)
H100.63880.76850.25460.046*
C110.7240 (5)0.9417 (5)0.3473 (4)0.0354 (10)
C120.7367 (5)1.0139 (5)0.4512 (3)0.0323 (10)
C130.6757 (5)0.9515 (4)0.5188 (3)0.0272 (9)
C140.6947 (5)1.0147 (4)0.6262 (3)0.0278 (9)
C150.7765 (5)1.1398 (4)0.6614 (3)0.0267 (9)
C160.8285 (5)1.2039 (5)0.5886 (4)0.0348 (10)
H160.87641.28880.61050.042*
C170.8095 (5)1.1436 (5)0.4884 (3)0.0331 (10)
H170.84481.18790.44310.040*
C180.7880 (5)0.9937 (5)0.2696 (4)0.0344 (10)
C190.9241 (6)1.0477 (5)0.2893 (4)0.0373 (11)
H190.97781.05600.35490.045*
C200.9818 (6)1.0897 (5)0.2135 (4)0.0419 (12)
H201.07331.12550.22800.050*
C210.9020 (7)1.0776 (6)0.1162 (5)0.0539 (15)
H210.93951.10640.06490.065*
C220.7686 (7)1.0238 (7)0.0951 (4)0.0540 (15)
H220.71611.01500.02900.065*
C230.7091 (6)0.9817 (6)0.1707 (4)0.0445 (13)
H230.61750.94590.15530.053*
C240.8039 (5)1.1944 (4)0.7674 (3)0.0289 (9)
C250.6614 (6)1.0051 (5)0.7875 (4)0.0369 (11)
H250.62230.96100.83120.044*
C260.8990 (5)1.3178 (5)0.8113 (3)0.0330 (10)
C271.0344 (7)1.3022 (6)0.8569 (5)0.0517 (14)
H271.06401.21610.86090.062*
C281.1262 (7)1.4166 (8)0.8970 (6)0.068 (2)
H281.21801.40640.92550.082*
C291.0815 (7)1.5449 (6)0.8945 (4)0.0484 (14)
H291.14291.62080.92220.058*
C300.9472 (7)1.5603 (6)0.8513 (5)0.0516 (15)
H300.91671.64680.85040.062*
C310.8564 (6)1.4469 (5)0.8087 (4)0.0409 (11)
H310.76561.45790.77800.049*
C320.7425 (6)1.1269 (5)0.8302 (3)0.0346 (10)
H320.75501.16220.89990.042*
N10.5995 (4)0.8299 (4)0.4880 (3)0.0324 (8)
N20.6370 (4)0.9488 (4)0.6886 (3)0.0303 (8)
O10.6379 (3)0.5309 (4)0.5201 (3)0.0397 (8)
O20.7607 (3)0.6793 (3)0.6469 (2)0.0337 (7)
O30.5268 (4)0.5278 (4)0.7384 (3)0.0436 (9)
O40.5308 (5)0.7365 (4)0.8253 (3)0.0573 (12)
Pb10.513080 (16)0.698420 (16)0.623266 (12)0.02661 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.022 (2)0.030 (2)0.037 (2)0.0013 (17)0.0068 (17)0.007 (2)
C20.021 (2)0.026 (2)0.037 (2)0.0003 (17)0.0054 (17)0.0096 (19)
C30.026 (2)0.039 (3)0.034 (2)0.0047 (19)0.0044 (18)0.004 (2)
C40.022 (2)0.041 (3)0.038 (2)0.0032 (19)0.0017 (18)0.009 (2)
C50.035 (3)0.040 (3)0.033 (2)0.006 (2)0.0092 (19)0.010 (2)
C60.034 (2)0.031 (2)0.026 (2)0.0036 (19)0.0058 (18)0.0033 (19)
C70.041 (3)0.024 (2)0.033 (2)0.0002 (19)0.009 (2)0.0032 (19)
C80.040 (3)0.027 (2)0.034 (2)0.001 (2)0.009 (2)0.0004 (19)
C90.046 (3)0.025 (2)0.030 (2)0.005 (2)0.004 (2)0.0043 (19)
C100.052 (3)0.034 (3)0.025 (2)0.000 (2)0.008 (2)0.002 (2)
C110.040 (3)0.033 (2)0.031 (2)0.004 (2)0.0015 (19)0.012 (2)
C120.041 (3)0.026 (2)0.028 (2)0.0030 (19)0.0024 (19)0.0066 (19)
C130.031 (2)0.023 (2)0.025 (2)0.0009 (17)0.0011 (17)0.0046 (17)
C140.031 (2)0.024 (2)0.027 (2)0.0005 (17)0.0020 (17)0.0042 (17)
C150.031 (2)0.024 (2)0.0244 (19)0.0007 (17)0.0064 (17)0.0023 (17)
C160.045 (3)0.025 (2)0.035 (2)0.007 (2)0.009 (2)0.0064 (19)
C170.047 (3)0.026 (2)0.027 (2)0.002 (2)0.0149 (19)0.0019 (18)
C180.042 (3)0.033 (2)0.029 (2)0.003 (2)0.006 (2)0.010 (2)
C190.043 (3)0.037 (3)0.030 (2)0.005 (2)0.009 (2)0.001 (2)
C200.044 (3)0.036 (3)0.047 (3)0.004 (2)0.021 (2)0.001 (2)
C210.067 (4)0.053 (4)0.051 (3)0.001 (3)0.023 (3)0.025 (3)
C220.062 (4)0.072 (4)0.032 (3)0.004 (3)0.010 (3)0.019 (3)
C230.042 (3)0.057 (3)0.034 (3)0.001 (3)0.004 (2)0.013 (3)
C240.035 (2)0.022 (2)0.029 (2)0.0057 (18)0.0069 (18)0.0001 (17)
C250.044 (3)0.037 (3)0.030 (2)0.005 (2)0.012 (2)0.004 (2)
C260.035 (3)0.032 (2)0.028 (2)0.0051 (19)0.0024 (18)0.0037 (19)
C270.045 (3)0.037 (3)0.063 (4)0.008 (2)0.001 (3)0.007 (3)
C280.044 (4)0.069 (5)0.076 (5)0.011 (3)0.017 (3)0.008 (4)
C290.058 (4)0.037 (3)0.042 (3)0.013 (3)0.007 (3)0.006 (2)
C300.066 (4)0.030 (3)0.056 (3)0.010 (3)0.005 (3)0.009 (3)
C310.040 (3)0.034 (3)0.046 (3)0.002 (2)0.003 (2)0.008 (2)
C320.048 (3)0.032 (2)0.023 (2)0.001 (2)0.0112 (19)0.0010 (19)
N10.040 (2)0.029 (2)0.0270 (18)0.0053 (17)0.0057 (16)0.0033 (16)
N20.035 (2)0.0245 (18)0.0317 (19)0.0026 (16)0.0066 (16)0.0074 (16)
O10.0213 (16)0.044 (2)0.049 (2)0.0040 (14)0.0113 (14)0.0056 (17)
O20.0278 (17)0.0351 (18)0.0357 (17)0.0032 (14)0.0082 (13)0.0018 (15)
O30.063 (3)0.0363 (19)0.0321 (17)0.0070 (18)0.0110 (17)0.0062 (16)
O40.100 (4)0.0288 (19)0.045 (2)0.008 (2)0.019 (2)0.0076 (17)
Pb10.02255 (9)0.02771 (10)0.03195 (10)0.00146 (6)0.00919 (6)0.00811 (7)
Geometric parameters (Å, º) top
C1—O21.251 (6)C17—H170.9300
C1—O11.253 (6)C18—C191.387 (7)
C1—C21.500 (6)C18—C231.394 (7)
C2—C41.387 (7)C19—C201.385 (7)
C2—C31.393 (6)C19—H190.9300
C3—C4i1.388 (7)C20—C211.380 (8)
C3—H30.9300C20—H200.9300
C4—C3i1.388 (7)C21—C221.361 (9)
C4—H40.9300C21—H210.9300
C5—O41.245 (6)C22—C231.393 (8)
C5—O31.259 (6)C22—H220.9300
C5—C61.512 (6)C23—H230.9300
C6—C71.379 (6)C24—C321.387 (7)
C6—C81.402 (7)C24—C261.486 (7)
C7—C8ii1.392 (7)C25—N21.329 (6)
C7—H70.9300C25—C321.403 (7)
C8—C7ii1.392 (7)C25—H250.9300
C8—H80.9300C26—C311.382 (7)
C9—N11.320 (6)C26—C271.385 (8)
C9—C101.397 (7)C27—C281.394 (9)
C9—H90.9300C27—H270.9300
C10—C111.372 (7)C28—C291.381 (9)
C10—H100.9300C28—H280.9300
C11—C121.442 (7)C29—C301.366 (9)
C11—C181.486 (7)C29—H290.9300
C12—C131.409 (6)C30—C311.387 (8)
C12—C171.423 (7)C30—H300.9300
C13—N11.364 (6)C31—H310.9300
C13—C141.452 (6)C32—H320.9300
C14—N21.353 (6)Pb1—N12.686 (4)
C14—C151.422 (6)Pb1—N22.677 (4)
C15—C241.410 (6)Pb1—O12.503 (4)
C15—C161.431 (6)Pb1—O22.418 (3)
C16—C171.357 (6)Pb1—O32.506 (4)
C16—H160.9300Pb1—O42.663 (4)
O2—C1—O1121.7 (4)C19—C20—H20120.4
O2—C1—C2119.9 (4)C22—C21—C20120.1 (5)
O1—C1—C2118.4 (4)C22—C21—H21119.9
O2—C1—Pb159.1 (2)C20—C21—H21119.9
O1—C1—Pb163.0 (2)C21—C22—C23121.2 (5)
C2—C1—Pb1171.9 (3)C21—C22—H22119.4
C4—C2—C3119.7 (4)C23—C22—H22119.4
C4—C2—C1119.7 (4)C22—C23—C18119.5 (5)
C3—C2—C1120.6 (4)C22—C23—H23120.3
C4i—C3—C2119.8 (5)C18—C23—H23120.3
C4i—C3—H3120.1C32—C24—C15118.0 (4)
C2—C3—H3120.1C32—C24—C26120.8 (4)
C2—C4—C3i120.5 (4)C15—C24—C26121.2 (4)
C2—C4—H4119.7N2—C25—C32124.1 (4)
C3i—C4—H4119.7N2—C25—H25118.0
O4—C5—O3123.5 (5)C32—C25—H25118.0
O4—C5—C6119.0 (5)C31—C26—C27119.3 (5)
O3—C5—C6117.5 (4)C31—C26—C24122.1 (5)
C7—C6—C8119.3 (4)C27—C26—C24118.6 (5)
C7—C6—C5121.2 (4)C26—C27—C28119.6 (6)
C8—C6—C5119.5 (4)C26—C27—H27120.2
C6—C7—C8ii121.5 (4)C28—C27—H27120.2
C6—C7—H7119.3C29—C28—C27120.4 (6)
C8ii—C7—H7119.3C29—C28—H28119.8
C7ii—C8—C6119.3 (4)C27—C28—H28119.8
C7ii—C8—H8120.4C30—C29—C28120.0 (5)
C6—C8—H8120.4C30—C29—H29120.0
N1—C9—C10123.1 (5)C28—C29—H29120.0
N1—C9—H9118.4C29—C30—C31119.9 (5)
C10—C9—H9118.4C29—C30—H30120.1
C11—C10—C9120.8 (4)C31—C30—H30120.1
C11—C10—H10119.6C26—C31—C30120.8 (5)
C9—C10—H10119.6C26—C31—H31119.6
C10—C11—C12117.1 (4)C30—C31—H31119.6
C10—C11—C18119.5 (4)C24—C32—C25119.4 (4)
C12—C11—C18123.5 (4)C24—C32—H32120.3
C13—C12—C17118.9 (4)C25—C32—H32120.3
C13—C12—C11118.1 (4)C9—N1—C13118.3 (4)
C17—C12—C11123.0 (4)C9—N1—Pb1119.5 (3)
N1—C13—C12122.5 (4)C13—N1—Pb1121.6 (3)
N1—C13—C14117.2 (4)C25—N2—C14117.1 (4)
C12—C13—C14120.4 (4)C25—N2—Pb1120.4 (3)
N2—C14—C15123.3 (4)C14—N2—Pb1121.8 (3)
N2—C14—C13118.1 (4)C1—O1—Pb190.5 (3)
C15—C14—C13118.6 (4)C1—O2—Pb194.5 (3)
C24—C15—C14118.0 (4)C5—O3—Pb196.3 (3)
C24—C15—C16123.0 (4)C5—O4—Pb189.3 (3)
C14—C15—C16119.0 (4)O2—Pb1—O152.76 (11)
C17—C16—C15121.5 (4)O2—Pb1—O383.20 (13)
C17—C16—H16119.3O1—Pb1—O383.93 (12)
C15—C16—H16119.3O2—Pb1—O490.28 (14)
C16—C17—C12121.4 (4)O1—Pb1—O4126.20 (13)
C16—C17—H17119.3O3—Pb1—O450.42 (12)
C12—C17—H17119.3O2—Pb1—N272.33 (12)
C19—C18—C23118.4 (5)O1—Pb1—N2116.45 (12)
C19—C18—C11123.2 (4)O3—Pb1—N2121.73 (12)
C23—C18—C11118.3 (5)O4—Pb1—N277.13 (12)
C20—C19—C18121.5 (5)O2—Pb1—N173.90 (12)
C20—C19—H19119.2O1—Pb1—N174.30 (13)
C18—C19—H19119.2O3—Pb1—N1154.98 (14)
C21—C20—C19119.3 (5)O4—Pb1—N1137.65 (12)
C21—C20—H20120.4N2—Pb1—N160.74 (12)
Symmetry codes: (i) x+2, y+1, z+1; (ii) x+1, y+1, z+2.

Experimental details

Crystal data
Chemical formula[Pb(C8H4O4)(C24H16N2)]
Mr703.69
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)9.855 (2), 10.046 (2), 13.539 (3)
α, β, γ (°)100.36 (3), 101.14 (3), 92.04 (3)
V3)1290.2 (4)
Z2
Radiation typeMo Kα
µ (mm1)6.58
Crystal size (mm)0.27 × 0.17 × 0.08
Data collection
DiffractometerRigaku R-AXIS RAPID
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.275, 0.592
No. of measured, independent and
observed [I > 2σ(I)] reflections
12741, 5855, 5326
Rint0.026
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.026, 0.082, 1.12
No. of reflections5855
No. of parameters352
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.80, 0.98

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

Selected geometric parameters (Å, º) top
Pb1—N12.686 (4)Pb1—O22.418 (3)
Pb1—N22.677 (4)Pb1—O32.506 (4)
Pb1—O12.503 (4)Pb1—O42.663 (4)
O2—Pb1—O152.76 (11)N2—Pb1—N160.74 (12)
O3—Pb1—O450.42 (12)
 

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