metal-organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2414-3146

catena-Poly[[(2,2′-bi­pyridine-κ2N,N′)lead(II)]-di-μ-bromido]

aCollege of Pharmaceutics and Material Engineering, Jinhua Polytechnic, Jinhua, Zhejiang 321007, People's Republic of China
*Correspondence e-mail: zbs_jy@163.com

Edited by M. Weil, Vienna University of Technology, Austria (Received 29 April 2016; accepted 12 May 2016; online 24 May 2016)

The polymeric title compound, [PbBr2(C10H8N2)]n, consists of 1[PbBr4/2] chains running parallel to [001]. Each PbII atom is additionally chelated by a 2,2′-bi­pyridine ligand, completing a distorted octa­hedral Br4N2 coordination set. In the crystal, weak C—H⋯Br hydrogen bonds and ππ stacking inter­actions link the [PbBr2(C10H8N2)]n chains into a three-dimensional supra­molecular structure.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

In the context of studies of metal complexes derived from halogen benzoic acids X-C6H4COOH, where X is F, Cl, Br or I, and ancilliary chelating ligands (Zhang et al., 2004[Zhang, B. S., Ying, T.-K. & Cheng, C.-G. (2004). Z. Kristallogr. New Cryst. Struct. 219, 483-484.]; Zhang, 2005[Zhang, B. S. (2005). Z. Kristallogr. New Cryst. Struct. 220, 73-74.], 2006[Zhang, B. S. (2006). Z. Kristallogr. New Cryst. Struct. 221, 355-356.]), we originally intended to synthesize a lead(II) complex derived from 6-bromo-2-pyridine­carb­oxy­lic acid and 2,2′-bi­pyridine (bpy). However, we accidentally obtained instead an 1:1 adduct of PbBr2 with bpy, [PbBr2(C10H8N2)]n (Fig. 1[link]), that supposedly formed due to decomposition of the acid under the applied solvothermal conditions.

[Figure 1]
Figure 1
A view of the chain of bromide-bridged PbII ions in the title compound extending parallel to [001]. Displacement ellipsoids are drawn at the 40% probability level [symmetry code (i) 1 − x, y, [{1\over 2}] − z].

Both the PbII atom and the chelating pby mol­ecule lie on a twofold rotation axis. In the crystal, Pb1II atoms are bridged by two pairs of Br1 ligands into 1[PbBr4/2] chains (Br—Pb—Br and Pb—Br—Pb angles are 89.87 (6) and 90.13 (6)°, respectively) with a Pb⋯Pb distance in the chain of 4.3434 (9) Å (Fig. 1[link]). The closest plane-to-plane distance between two bpy ligands of 3.376 (2) Å indicates the existence of ππ inter­actions, which results in the formation of a layered arrangement of the [PbBr2(C10H8N2)]n chains parallel to (100). The layers are associated through weak C—H⋯Br hydrogen bonds (Table 1[link], Fig. 2[link]) into an overall three-dimensional supra­molecular set-up.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C2—H2⋯Br1i 0.93 2.98 3.906 (9) 174
Symmetry code: (i) [x-{\script{1\over 2}}, -y+{\script{1\over 2}}, z-{\script{1\over 2}}].
[Figure 2]
Figure 2
A packing diagram of the title compound viewed along [001]. Dashed lines indicate C—H⋯Br hydrogen bonds.

The chain structure of the title compound resembles that of related cadmium compounds with composition [CdX2(phen)] (phen = 1,10-phenanthroline), X = Cl, Chen et al., 2003[Chen, H.-B., Zhou, Z.-H., Wan, H.-L. & Ng, S. W. (2003). Acta Cryst. E59, m845-m846.]; X = Br, (Zhang, 2007[Zhang, B.-S. (2007). Acta Cryst. E63, m1562.]) or [CdCl2(2,2-bpy)] (Zhou et al., 2003[Zhou, Y.-F., Xu, Y., Yuan, D.-Q. & Hong, M.-C. (2003). Acta Cryst. E59, m821-m823.]).

Synthesis and crystallization

Freshly prepared Pb(CH3COO)2·3H2O (0.1890 g 0.50 mmol), 2,2′-bi­pyridine (bpy) (0.0399 g 0.25 mmol), 6-bromo-2-pyridine­carb­oxy­lic acid (0.0504 g 0.25 mmol), and 15 ml CH3OH/H2O (1:2,v/v) were mixed and stirred for ca 2.0 h. Subsequently, the resulting suspension was heated in a 23 ml Teflon-lined stainless steel autoclave at 433 K for 7 days. After the autoclave was cooled to room temperature, yellow crystals with a cuboid form were obtained.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula [PbBr2(C10H8N2)]
Mr 523.19
Crystal system, space group Monoclinic, C2/c
Temperature (K) 293
a, b, c (Å) 16.249 (3), 9.878 (2), 8.2425 (16)
β (°) 104.79 (3)
V3) 1279.2 (4)
Z 4
Radiation type Mo Kα
μ (mm−1) 19.41
Crystal size (mm) 0.24 × 0.23 × 0.21
 
Data collection
Diffractometer Rigaku R-AXIS RAPID
Absorption correction Multi-scan (ABSCOR; Higashi, 1995[Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.])
Tmin, Tmax 0.013, 0.017
No. of measured, independent and observed [I > 2σ(I)] reflections 4632, 1053, 871
Rint 0.123
(sin θ/λ)max−1) 0.583
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.124, 1.21
No. of reflections 1053
No. of parameters 58
No. of restraints 21
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 1.64, −1.97
Computer programs: RAPID-AUTO (Rigaku, 1998[Rigaku (1998). RAPID-AUTO. Rigaku Corporation, Tokyo, Japan.]), CrystalStructure (Rigaku/MSC, 2002[Rigaku/MSC (2002). CrystalStructure. Rigaku/MSC. The Woodlands, Texas, USA.]), SHELXS97 and SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]) and SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]).

Structural data


Comment top

In the context of studies of metal complexes derived from halogen benzoic acids X-C6H4COOH, where X is F, Cl, Br or I, and ancilliary chelating ligands (Zhang et al., 2004; Zhang, 2005, 2006), we originally intended to synthesize a lead(II) complex derived from 6-bromo-2-pyridinecarboxylic acid and 2,2'-bipyridine (bpy). However, we accidentally obtained instead an 1:1 adduct of PbBr2 with bpy, [PbBr2(C10H8N2)]n, that supposedly formed due to decomposition of the acid under the applied solvothermal conditions. Both the PbII atom and the chelating pby molecule lie on a twofold rotation axis. In the crystal, Pb1II atoms are bridged by two pairs of Br1 ligands into 1[PbBr4/2] chains (Br—Pb—Br and Pb—Br—Pb angles are 89.87 (6) and 90.13 (6)°, respectively) with a Pb···Pb distance in the chain of 4.3434 (9) Å (Fig. 1). In the crystal, the closest plane-to-plane distance between two bpy ligands of 3.376 (2) Å indicates the existence of ππ interactions, which results in the formation of a layered arrangement of the [PbBr2(C10H8N2)]n chains parallel to (100). The layers are associated through weak C—H···Br hydrogen bonds (Table 1, Fig. 2) into an overall three-dimensional supramolecular set-up.

The chain structure of the title compound resembles that of related cadmium compounds with composition [CdX2(phen)] (phen = 1,10-phenantroline), X = Cl, Chen et al., 2003; X = Br, (Zhang, 2007) or [CdCl2(2,2-bpy)] (Zhou et al., 2003).

Experimental top

Freshly prepared Pb(CH3COO)2·3H2O (0.1890 g 0.50 mmol), 2,2'-bipyridine (bpy) (0.0399 g 0.25 mmol), 6-bromo-2-pyridinecarboxylic acid (0.0504 g 0.25 mmol), and 15 ml CH3OH/H2O (1:2,v/v) were mixed and stirred for ca 2.0 h. Subsequently, the resulting suspension was heated in a 23 ml Teflon-lined stainless steel autoclave at 433 K for 7 days. After the autoclave was cooled to room temperature, yellow crystals with a cuboid form were obtained.

Refinement top

Crystal data, data collection and structure refinement details are summarized in Table 2.

Structure description top

In the context of studies of metal complexes derived from halogen benzoic acids X-C6H4COOH, where X is F, Cl, Br or I, and ancilliary chelating ligands (Zhang et al., 2004; Zhang, 2005, 2006), we originally intended to synthesize a lead(II) complex derived from 6-bromo-2-pyridinecarboxylic acid and 2,2'-bipyridine (bpy). However, we accidentally obtained instead an 1:1 adduct of PbBr2 with bpy, [PbBr2(C10H8N2)]n (Fig. 1), that supposedly formed due to decomposition of the acid under the applied solvothermal conditions.

Both the PbII atom and the chelating pby molecule lie on a twofold rotation axis. In the crystal, Pb1II atoms are bridged by two pairs of Br1 ligands into 1[PbBr4/2] chains (Br—Pb—Br and Pb—Br—Pb angles are 89.87 (6) and 90.13 (6)°, respectively) with a Pb···Pb distance in the chain of 4.3434 (9) Å (Fig. 1). The closest plane-to-plane distance between two bpy ligands of 3.376 (2) Å indicates the existence of ππ interactions, which results in the formation of a layered arrangement of the [PbBr2(C10H8N2)]n chains parallel to (100). The layers are associated through weak C—H···Br hydrogen bonds (Table 1, Fig. 2) into an overall three-dimensional supramolecular set-up.

The chain structure of the title compound resembles that of related cadmium compounds with composition [CdX2(phen)] (phen = 1,10-phenanthroline), X = Cl, Chen et al., 2003; X = Br, (Zhang, 2007) or [CdCl2(2,2-bpy)] (Zhou et al., 2003).

Computing details top

Data collection: RAPID-AUTO (Rigaku, 1998); cell refinement: RAPID-AUTO (Rigaku, 1998); data reduction: CrystalStructure (Rigaku/MSC, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. A view of the chain of bromide-bridged PbII ions in the title compound extending parallel to [001]. Displacement ellipsoids are drawn at the 40% probability level [symmetry code (i) 1 - x, y, 1/2 - z].
[Figure 2] Fig. 2. A packing diagram of the title compound viewed down [001]. Dashed lines indicate C—H···Br hydrogen bonds.
catena-Poly[[(2,2'-bipyridine-κ2N,N')lead(II)]-di-µ-bromido] top
Crystal data top
[PbBr2(C10H8N2)]F(000) = 936
Mr = 523.19Dx = 2.717 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 4297 reflections
a = 16.249 (3) Åθ = 3.3–24.5°
b = 9.878 (2) ŵ = 19.41 mm1
c = 8.2425 (16) ÅT = 293 K
β = 104.79 (3)°Cuboid, yellow
V = 1279.2 (4) Å30.24 × 0.23 × 0.21 mm
Z = 4
Data collection top
Rigaku R-AXIS RAPID
diffractometer
1053 independent reflections
Radiation source: fine-focus sealed tube871 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.123
ω scansθmax = 24.5°, θmin = 3.3°
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
h = 1818
Tmin = 0.013, Tmax = 0.017k = 1111
4632 measured reflectionsl = 98
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)] = 0.043H-atom parameters constrained
wR(F2) = 0.124 w = 1/[σ2(Fo2) + (0.P)2 + 35.8179P]
where P = (Fo2 + 2Fc2)/3
S = 1.21(Δ/σ)max < 0.001
1053 reflectionsΔρmax = 1.64 e Å3
58 parametersΔρmin = 1.97 e Å3
21 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0010 (2)
Crystal data top
[PbBr2(C10H8N2)]V = 1279.2 (4) Å3
Mr = 523.19Z = 4
Monoclinic, C2/cMo Kα radiation
a = 16.249 (3) ŵ = 19.41 mm1
b = 9.878 (2) ÅT = 293 K
c = 8.2425 (16) Å0.24 × 0.23 × 0.21 mm
β = 104.79 (3)°
Data collection top
Rigaku R-AXIS RAPID
diffractometer
1053 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
871 reflections with I > 2σ(I)
Tmin = 0.013, Tmax = 0.017Rint = 0.123
4632 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.04321 restraints
wR(F2) = 0.124H-atom parameters constrained
S = 1.21 w = 1/[σ2(Fo2) + (0.P)2 + 35.8179P]
where P = (Fo2 + 2Fc2)/3
1053 reflectionsΔρmax = 1.64 e Å3
58 parametersΔρmin = 1.97 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
Pb10.50000.43060 (8)0.25000.0502 (5)
Br10.62002 (14)0.3951 (2)0.0295 (3)0.0700 (6)
C10.3595 (8)0.2242 (10)0.0180 (13)0.073 (6)
H10.33890.30780.06240.087*
C20.3177 (7)0.1061 (13)0.0845 (14)0.086 (5)
H20.26920.11060.17330.103*
C30.3485 (8)0.0188 (10)0.0181 (17)0.086 (5)
H30.32060.09790.06260.103*
C40.4210 (8)0.0256 (7)0.1147 (16)0.061 (4)
H40.44160.10920.15900.073*
C50.4628 (6)0.0925 (9)0.1811 (12)0.059 (4)
N10.4320 (7)0.2174 (8)0.1147 (12)0.055 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pb10.0539 (7)0.0463 (6)0.0447 (6)0.0000.0023 (4)0.000
Br10.0603 (14)0.0770 (12)0.0718 (12)0.0152 (10)0.0151 (9)0.0157 (9)
C10.074 (15)0.092 (13)0.043 (9)0.022 (11)0.002 (10)0.022 (9)
C20.060 (11)0.098 (10)0.101 (12)0.010 (9)0.022 (10)0.046 (10)
C30.060 (11)0.098 (10)0.101 (12)0.010 (9)0.023 (10)0.046 (10)
C40.063 (9)0.050 (6)0.083 (9)0.009 (6)0.041 (8)0.010 (6)
C50.060 (9)0.049 (6)0.081 (9)0.008 (6)0.042 (8)0.010 (6)
N10.045 (9)0.062 (8)0.059 (8)0.003 (7)0.011 (7)0.016 (7)
Geometric parameters (Å, º) top
Pb1—N12.504 (7)C1—H10.9300
Pb1—N1i2.504 (15)C2—C31.3900
Pb1—Br13.006 (2)C2—H20.9300
Pb1—Br1i3.006 (2)C3—C41.3900
Pb1—Br1ii3.128 (2)C3—H30.9300
Pb1—Br1iii3.128 (2)C4—C51.3900
Br1—Pb1iii3.128 (2)C4—H40.9300
C1—C21.3900C5—N11.3900
C1—N11.3900C5—C5i1.433 (17)
N1—Pb1—N1i65.5 (6)C2—C1—H1120.0
N1—Pb1—Br185.0 (3)N1—C1—H1120.0
N1i—Pb1—Br183.7 (6)C1—C2—C3120.0
N1—Pb1—Br1i83.7 (3)C1—C2—H2120.0
N1i—Pb1—Br1i85.0 (6)C3—C2—H2120.0
Br1—Pb1—Br1i166.60 (8)C2—C3—C4120.0
N1—Pb1—Br1ii155.8 (2)C2—C3—H3120.0
N1i—Pb1—Br1ii90.8 (4)C4—C3—H3120.0
Br1—Pb1—Br1ii97.52 (7)C5—C4—C3120.0
Br1i—Pb1—Br1ii89.87 (6)C5—C4—H4120.0
N1—Pb1—Br1iii90.8 (2)C3—C4—H4120.0
N1i—Pb1—Br1iii155.8 (4)C4—C5—N1120.0
Br1—Pb1—Br1iii89.87 (6)C4—C5—C5i122.73 (11)
Br1i—Pb1—Br1iii97.52 (7)N1—C5—C5i117.27 (9)
Br1ii—Pb1—Br1iii113.19 (9)C5—N1—C1120.0
Pb1—Br1—Pb1iii90.13 (6)C5—N1—Pb1119.9 (5)
C2—C1—N1120.0C1—N1—Pb1120.0 (5)
Symmetry codes: (i) x+1, y, z+1/2; (ii) x, y+1, z+1/2; (iii) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2···Br1iv0.932.983.906 (9)174
Symmetry code: (iv) x1/2, y+1/2, z1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2···Br1i0.932.983.906 (9)174
Symmetry code: (i) x1/2, y+1/2, z1/2.

Experimental details

Crystal data
Chemical formula[PbBr2(C10H8N2)]
Mr523.19
Crystal system, space groupMonoclinic, C2/c
Temperature (K)293
a, b, c (Å)16.249 (3), 9.878 (2), 8.2425 (16)
β (°) 104.79 (3)
V3)1279.2 (4)
Z4
Radiation typeMo Kα
µ (mm1)19.41
Crystal size (mm)0.24 × 0.23 × 0.21
Data collection
DiffractometerRigaku R-AXIS RAPID
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.013, 0.017
No. of measured, independent and
observed [I > 2σ(I)] reflections
4632, 1053, 871
Rint0.123
(sin θ/λ)max1)0.583
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.124, 1.21
No. of reflections1053
No. of parameters58
No. of restraints21
H-atom treatmentH-atom parameters constrained
w = 1/[σ2(Fo2) + (0.P)2 + 35.8179P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)1.64, 1.97

Computer programs: RAPID-AUTO (Rigaku, 1998), CrystalStructure (Rigaku/MSC, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

 

Acknowledgements

The authors gratefully acknowledge the financial support of the National Natural Science Foundation of China (grant No. 51343003).

References

First citationChen, H.-B., Zhou, Z.-H., Wan, H.-L. & Ng, S. W. (2003). Acta Cryst. E59, m845–m846.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationHigashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.  Google Scholar
First citationRigaku (1998). RAPID-AUTO. Rigaku Corporation, Tokyo, Japan.  Google Scholar
First citationRigaku/MSC (2002). CrystalStructure. Rigaku/MSC. The Woodlands, Texas, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationZhang, B. S. (2005). Z. Kristallogr. New Cryst. Struct. 220, 73–74.  CAS Google Scholar
First citationZhang, B. S. (2006). Z. Kristallogr. New Cryst. Struct. 221, 355–356.  CAS Google Scholar
First citationZhang, B.-S. (2007). Acta Cryst. E63, m1562.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationZhang, B. S., Ying, T.-K. & Cheng, C.-G. (2004). Z. Kristallogr. New Cryst. Struct. 219, 483–484.  CAS Google Scholar
First citationZhou, Y.-F., Xu, Y., Yuan, D.-Q. & Hong, M.-C. (2003). Acta Cryst. E59, m821–m823.  Web of Science CSD CrossRef IUCr Journals Google Scholar

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