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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 17;67(Pt 9):m1240–m1241. doi: 10.1107/S1600536811031710

Tetra­kis(picolinato-κ2 N,O)zirconium(IV) dihydrate

Maryke Steyn a,*, Hendrik G Visser a, Andreas Roodt a, T J Muller a
PMCID: PMC3200838  PMID: 22065566

Abstract

In the title compound, [Zr(C6H4NO2)4]·2H2O, the ZrIV atom is located on a crystallographic fourfold rotoinversion axis (Inline graphic) and is coordinated by four picolinate anions with Zr—O and Zr—N distances of 2.120 (2) and 2.393 (2) Å, respectively. An approximate square-anti­prismatic coordination polyhedron of the N,O-coordination ligand atoms is formed, with a distortion towards dodeca­hedral geometry. The crystal packing is stabilized by inter­molecular π–π inter­actions between adjacent picolinate rings [centroid–centroid distances = 3.271 (1) and 3.640 (2) Å], as well as O—H⋯O hydrogen bonds between the solvent mol­ecules and the coordinated ligands, thereby linking the mol­ecules into a supra­molecular three-dimensional network.

Related literature

For N,O- and O,O′-bidentate ligand complexes of zirconium and hafnium, see: Steyn et al. (2008); Viljoen et al. (2010a,b ). For relevant studies of N,O- and O,O′-bidentate ligands with other transition metal atoms, see: Graham et al. (1991); Mtshali et al. (2006); Roodt et al. (2011); Schutte et al. (2008); Steyn et al. (1997); Van Aswegen et al. (1991); Van der Westhuizen et al. (2010). graphic file with name e-67-m1240-scheme1.jpg

Experimental

Crystal data

  • [Zr(C6H4NO2)4]·2H2O

  • M r = 615.66

  • Tetragonal, Inline graphic

  • a = 11.083 (5) Å

  • c = 9.548 (5) Å

  • V = 1172.8 (10) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.54 mm−1

  • T = 100 K

  • 0.12 × 0.09 × 0.04 mm

Data collection

  • Bruker X8 APEXII 4K Kappa CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2004) T min = 0.942, T max = 0.977

  • 27234 measured reflections

  • 1477 independent reflections

  • 1271 reflections with I > 2σ(I)

  • R int = 0.074

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.100

  • S = 1.10

  • 1477 reflections

  • 87 parameters

  • 1 restraint

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.64 e Å−3

  • Δρmin = −0.92 e Å−3

Data collection: APEX2 (Bruker, 2010); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811031710/zq2119sup1.cif

e-67-m1240-sup1.cif (13.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031710/zq2119Isup2.hkl

e-67-m1240-Isup2.hkl (71.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O03—H03A⋯O2i 0.94 (2) 1.89 (2) 2.829 (3) 175 (5)

Symmetry code: (i) Inline graphic.

Acknowledgments

Financial assistance from the Advanced Metals Initiative (AMI) and the Department of Science and Technology (DST) of South Africa, as well as the New Metals Development Network (NMDN) and the South African Nuclear Energy Corporation Limited (Necsa) is gratefully acknowledged.

supplementary crystallographic information

Comment

The introduction of N,O-bidentate ligands with the oxine or aminovinylketone backbones significantly influences both steric and electronic properties of transition metal centres as illustrated by literature examples (Graham et al., 1991; Mtshali et al., 2006; Roodt et al., 2011; Schutte et al., 2008; Steyn et al., 1997; Van Aswegen et al., 1991; Van der Westhuizen et al., 2010). This study is part of ongoing research initiatives investigating coordination behaviour of O,O'- and N, O,-bidentate ligands with zirconium(IV) and hafnium(IV) for possible separation of these two metals from base ore sources (Steyn et al., 2008; Viljoen et al., 2010a,b).

The title compound, [Zr(C6H4NO2)4].2H2O, with C6H4NO2 as picolinic acid, crystallizes in the form of colourless cubic crystals in the tetragonal P42/n space group. The ZrIV atom, located on a crystallographic fourfold rotoinversion axis (4), is coordinated to four picolinic acid ligands (Fig. 1). The assymetric unit contains half a solvent molecule located on a twofold axis. The Zr—O and Zr—N bond lengths are 2.120 (2) Å and 2.393 (2) Å, respectively, with a N—Zr—O bite angle of 69.79 (7) °. The coordination polyhedron around the metal centre is an approximate square antiprism of the N,O-coordination ligand atoms, with a distortion towards dodecahedral geometry. The crystal packing is stabilized by intermolecular π-π interactions (Fig. 2), between adjacent picolinato rings, with interplanar and centroid-to-centroid distances of 3.271 (1) Å and 3.640 (2) Å, respectively. Further stabilization of the crystal structure is afforded by O—H···O hydrogen bonding (Fig. 3) between the carbonyl group of the picolinato ligands and the solvent water molecules. All of these interactions serve to link the molecules into a supramolecular three-dimensional network.

Experimental

Chemicals were purchased from Sigma-Aldrich and used as received. ZrCl4 (103.3 mg, 0.463 mmol) and picolinic acid (PicA) (175.2 mg, 1.423 mmol) was separately dissolved in DMF (2.5 ml ea) and heated to 60 °C. The PicA solution was added drop-wise to the zirconium solution and stirred at 60 °C for 30 minutes. The reaction solution was removed from heating, covered and left to stand for crystallization. White cubic crystals, suitable for single-crystal X-ray diffraction, formed after 30 days (yield: 178 mg, 86%).

Refinement

The aromatic H atoms were placed in geometrically idealized positions (C–H = 0.95 Å) and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C). The hydrogen atoms of the solvent water molecule were located on the Fourier difference map and refined isotropically. The highest residual electron density was located 0.74 Å from O1.

Figures

Fig. 1.

Fig. 1.

Representation of the title compound with displacement ellipsoids drawn at the 50% probability level. H atoms are presented as small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Graphical illustration of π–π interaction and stacking between different PicA-ligands of neighboring molecules to form a three-dimensional network (displacement ellipsoids are drawn at the 50% probability level). Hydrogen atoms and solvent water molecules omitted for clarity.

Fig. 3.

Fig. 3.

Graphical illustration of Zr(PicA)4 indicating O–H···O hydrogen bonding interaction as observed between the solvent molecules and the free carbonyl oxygen atoms from neighboring molecules (displacement ellipsoids are drawn at the 50% probability level).

Crystal data

[Zr(C6H4NO2)4]·2H2O Dx = 1.743 Mg m3
Mr = 615.66 Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P42/n Cell parameters from 9933 reflections
Hall symbol: -P 4bc θ = 2.6–28.4°
a = 11.083 (5) Å µ = 0.54 mm1
c = 9.548 (5) Å T = 100 K
V = 1172.8 (10) Å3 Cuboid, colourless
Z = 2 0.12 × 0.09 × 0.04 mm
F(000) = 624

Data collection

Bruker X8 APEXII 4K Kappa CCD diffractometer 1477 independent reflections
Radiation source: fine-focus sealed tube 1271 reflections with I > 2σ(I)
graphite Rint = 0.074
ω and φ scans θmax = 28.5°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Bruker, 2004) h = −14→13
Tmin = 0.942, Tmax = 0.977 k = −14→14
27234 measured reflections l = −12→12

Refinement

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)] = 0.037 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100 H atoms treated by a mixture of independent and constrained refinement
S = 1.10 w = 1/[σ2(Fo2) + (0.0415P)2 + 2.5407P] where P = (Fo2 + 2Fc2)/3
1477 reflections (Δ/σ)max < 0.001
87 parameters Δρmax = 0.64 e Å3
1 restraint Δρmin = −0.92 e Å3

Special details

Experimental. The intensity data were collected on a Bruker X8 ApexII 4 K Kappa CCD diffractometer using an exposure time of 40 s/frame. A total of 1709 frames were collected with a frame width of 0.5° covering up to θ = 28.40° with 99.5% completeness accomplished.
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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)

x y z Uiso*/Ueq
Zr1 0.25 0.25 0.75 0.01305 (15)
O1 0.41797 (14) 0.31522 (14) 0.82454 (18) 0.01305 (15)
O2 0.56146 (18) 0.33223 (18) 0.9859 (2) 0.0263 (4)
C3 0.4700 (2) 0.1154 (2) 1.1212 (3) 0.0195 (5)
H3 0.5415 0.144 1.1601 0.023*
N1 0.31289 (18) 0.13671 (18) 0.9505 (2) 0.0157 (4)
C2 0.4174 (2) 0.1737 (2) 1.0089 (3) 0.0169 (5)
C5 0.3088 (2) −0.0267 (2) 1.1131 (3) 0.0206 (5)
H5 0.2707 −0.0959 1.1461 0.025*
C6 0.2603 (2) 0.0372 (2) 1.0016 (3) 0.0178 (5)
H6 0.1891 0.01 0.961 0.021*
C4 0.4143 (2) 0.0137 (2) 1.1748 (3) 0.0222 (5)
H4 0.4473 −0.0269 1.251 0.027*
C1 0.4728 (2) 0.2822 (2) 0.9379 (3) 0.0183 (5)
O03 0.25 0.75 0.3385 (4) 0.0472 (9)
H03A 0.274 (4) 0.815 (3) 0.396 (4) 0.068 (15)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Zr1 0.01054 (17) 0.01054 (17) 0.0181 (2) 0 0 0
O1 0.01054 (17) 0.01054 (17) 0.0181 (2) 0 0 0
O2 0.0201 (9) 0.0257 (10) 0.0332 (11) −0.0070 (8) −0.0066 (8) 0.0008 (8)
C3 0.0170 (11) 0.0211 (12) 0.0205 (12) 0.0015 (9) −0.0014 (9) −0.0035 (10)
N1 0.0141 (9) 0.0136 (9) 0.0194 (10) −0.0005 (8) 0.0000 (8) −0.0002 (8)
C2 0.0145 (11) 0.0160 (11) 0.0203 (12) 0.0000 (9) 0.0007 (9) −0.0030 (9)
C5 0.0221 (12) 0.0178 (12) 0.0220 (13) 0.0026 (9) 0.0043 (10) 0.0027 (10)
C6 0.0158 (11) 0.0154 (11) 0.0223 (12) −0.0003 (9) 0.0005 (9) 0.0003 (9)
C4 0.0236 (13) 0.0240 (13) 0.0191 (13) 0.0056 (10) 0.0003 (10) 0.0020 (10)
C1 0.0148 (11) 0.0171 (11) 0.0231 (12) −0.0001 (9) 0.0006 (9) −0.0032 (9)
O03 0.059 (2) 0.038 (2) 0.045 (2) −0.0011 (18) 0 0

Geometric parameters (Å, °)

Zr1—O1i 2.1200 (18) C3—C4 1.384 (4)
Zr1—O1 2.1200 (18) C3—H3 0.93
Zr1—O1ii 2.1200 (18) N1—C6 1.340 (3)
Zr1—O1iii 2.1200 (18) N1—C2 1.349 (3)
Zr1—N1i 2.393 (2) C2—C1 1.511 (4)
Zr1—N1ii 2.393 (2) C5—C4 1.384 (4)
Zr1—N1iii 2.393 (2) C5—C6 1.386 (4)
Zr1—N1 2.393 (2) C5—H5 0.93
O1—C1 1.294 (3) C6—H6 0.93
O2—C1 1.218 (3) C4—H4 0.93
C3—C2 1.381 (4) O03—H03A 0.941 (19)
O1i—Zr1—O1 96.47 (3) N1i—Zr1—N1 129.78 (7)
O1i—Zr1—O1ii 96.47 (3) N1ii—Zr1—N1 73.76 (11)
O1—Zr1—O1ii 140.77 (10) N1iii—Zr1—N1 129.78 (7)
O1i—Zr1—O1iii 140.77 (10) C1—O1—Zr1 126.61 (15)
O1—Zr1—O1iii 96.47 (3) C2—C3—C4 118.7 (2)
O1ii—Zr1—O1iii 96.47 (3) C2—C3—H3 120.7
O1i—Zr1—N1i 69.79 (7) C4—C3—H3 120.7
O1—Zr1—N1i 145.95 (7) C6—N1—C2 118.2 (2)
O1ii—Zr1—N1i 73.05 (7) C6—N1—Zr1 126.65 (17)
O1iii—Zr1—N1i 78.95 (7) C2—N1—Zr1 114.94 (16)
O1i—Zr1—N1ii 145.95 (7) N1—C2—C3 122.8 (2)
O1—Zr1—N1ii 78.95 (7) N1—C2—C1 113.9 (2)
O1ii—Zr1—N1ii 69.79 (7) C3—C2—C1 123.3 (2)
O1iii—Zr1—N1ii 73.05 (7) C4—C5—C6 119.3 (2)
N1i—Zr1—N1ii 129.78 (7) C4—C5—H5 120.4
O1i—Zr1—N1iii 78.95 (7) C6—C5—H5 120.4
O1—Zr1—N1iii 73.05 (7) N1—C6—C5 122.1 (2)
O1ii—Zr1—N1iii 145.95 (7) N1—C6—H6 118.9
O1iii—Zr1—N1iii 69.79 (7) C5—C6—H6 118.9
N1i—Zr1—N1iii 73.76 (11) C3—C4—C5 118.9 (2)
N1ii—Zr1—N1iii 129.78 (7) C3—C4—H4 120.6
O1i—Zr1—N1 73.05 (7) C5—C4—H4 120.6
O1—Zr1—N1 69.79 (7) O2—C1—O1 124.4 (2)
O1ii—Zr1—N1 78.95 (7) O2—C1—C2 121.4 (2)
O1iii—Zr1—N1 145.95 (7) O1—C1—C2 114.2 (2)

Symmetry codes: (i) y, −x+1/2, −z+3/2; (ii) −x+1/2, −y+1/2, z; (iii) −y+1/2, x, −z+3/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O03—H03A···O2iv 0.94 (2) 1.89 (2) 2.829 (3) 175 (5)

Symmetry codes: (iv) y, −x+3/2, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZQ2119).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811031710/zq2119sup1.cif

e-67-m1240-sup1.cif (13.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031710/zq2119Isup2.hkl

e-67-m1240-Isup2.hkl (71.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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