Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Aug 28;66(Pt 9):m1178–m1179. doi: 10.1107/S1600536810031855

trans-Diaqua­bis­[5-carb­oxy-4-carboxyl­ato-2-(4-pyridinio)-1H-imidazol-1-ido-κ2 N 3,O 4]zinc(II)

Xia Li a,*, Ling-Zhi Du a, Ben-Lai Wu b, Hong-Yun Zhang b
PMCID: PMC3007913  PMID: 21588565

Abstract

In the title complex, [Zn(C10H6N3O4)2(H2O)2], the ZnII atom is located on a twofold rotation axis and is coordinated by two trans-positioned N,O-bidentate and zwitterionic 5-carb­oxy-4-carboxyl­ato-2-(4-pyridinio)-1H-imidazol-1-ide (H2PIDC) ligands and two water mol­ecules, defining a distorted octa­hedral environment. The complete solid-state structure can be described as a three-dimensional supra­molecular framework, stabilized by extensive hydrogen-bonding inter­actions involving the coordinated water mol­ecules, uncoordin­ated imidazole N atom, protonated pyridine N and carboxyl­ate O atoms of the H2PIDC ligands.

Related literature

For related structures, see: Li, Liu et al. (2009); Li, Wu et al. (2009). For the preparation of 2-(pyridin-4-yl)-1H-imidazole-4,5-dicarb­oxy­lic acid, see: Sun et al. (2006).graphic file with name e-66-m1178-scheme1.jpg

Experimental

Crystal data

  • [Zn(C10H6N3O4)2(H2O)2]

  • M r = 565.76

  • Monoclinic, Inline graphic

  • a = 7.4138 (9) Å

  • b = 20.204 (3) Å

  • c = 13.4778 (17) Å

  • β = 97.008 (1)°

  • V = 2003.7 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.31 mm−1

  • T = 173 K

  • 0.27 × 0.17 × 0.10 mm

Data collection

  • Rigaku Mercury CCD diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2000) T min = 0.754, T max = 0.878

  • 9235 measured reflections

  • 2488 independent reflections

  • 1957 reflections with I > 2σ(I)

  • R int = 0.031

Refinement

  • R[F 2 > 2σ(F 2)] = 0.031

  • wR(F 2) = 0.090

  • S = 1.04

  • 2488 reflections

  • 178 parameters

  • 1 restraint

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

  • Δρmax = 0.34 e Å−3

  • Δρmin = −0.37 e Å−3

Data collection: CrystalClear (Rigaku, 2000); cell refinement: CrystalClear; data reduction: CrystalClear; 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: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810031855/jh2196sup1.cif

e-66-m1178-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810031855/jh2196Isup2.hkl

e-66-m1178-Isup2.hkl (122.3KB, hkl)

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

Table 1. Selected bond lengths (Å).

Zn1—O2 2.0713 (15)
Zn1—O1 2.1407 (18)
Zn1—N1 2.1592 (17)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1B⋯N2i 0.82 (3) 2.08 (3) 2.898 (3) 178 (3)
N3—H3⋯O5ii 0.88 1.89 2.755 (2) 169
O4—H4A⋯O3 0.89 (2) 1.58 (2) 2.459 (2) 173 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

This work was supported by the National Natural Science Foundation of China (20771094, 20671083), the Science and Technology Key Task of Henan Province (0524270061) and the China Postdoctoral Science Foundation (20070410877).

supplementary crystallographic information

Comment

Multifunctional connector 2-(pyridin-4-yl)-1H-imidazole-4,5-dicarboxylate acid (H3PIDC), a rigid N-heterocyclic carboxylate, has great potential for coordinative interactions and hydrogen bonding, showing more interesting traits in the construction of MOFs. It can be successively deprotonated to generate various species with different proton numbers, and hence may result in a large diversity of supramolecular architectures. Very recently, we have reported several supramolecular architectures (Li, Wu et al., 2009; Li, Liu et al., 2009) base on ligand 2-(pyridin-4-yl)-1H-imidazole-4,5-dicarboxylic acid. As an extension of our previous investigations, we have isolated a new Zn(II) complex, [Zn(H2PIDC)2(H2O)2], (I), by the reaction of H3PIDC and Zn(II) diacetate under the hydrothermal condition. We report here the single-crystal structure of this complex.

As shown in Fig. 1, the molecule of (I) is a discrete neutral monomer, in which the Zn atom resides on a crystallographic inversion centre and the asymmetric unit contains one-half of the [Zn(H2PIDC)2(H2O)2] formula unit. Each Zn atom is six-coordinated by N2O4 with two chelating rings from two H2PIDC ligands arranged symmetrically in the equatorial plane and two water molecules occupying the apical sites, showing a distorted octahedral geometry (Table 1). In this complex, one carboxyl group and imidazole group are deprotonated and the pyridyl group is protonated, and the ligand bears a formal charge of -1, and the uncoordinated carboxylate atoms O3 and O4 form an intramolecular hydrogen bond (Table 2). All non-H atoms in the imidazole-4,5-dicarboxyl group are nearly coplanar [the mean deviation is 0.075 (3) Å], and the dihedral angle between imidazole group and pyridine group is 11.4 (2) °.

A three-dimensional supramolecular network is constructed via hydrogen-bonding interactions involving the coordinated water molecules, uncoordinated imidazole N atom, protonated pyridine N and carboxylate O atoms of the H2PIDC- ligands (Table 2 and Fig. 2).

Experimental

A mixture of zinc diacetate dihydrate (0.022 g, 0.1 mmol), 2-(pyridin-4-yl)-1H-imidazole-4,5-dicarboxylic acid (0.024 g, 0.1 mmol) (Sun et al., 2006), NaOH (0.004 g, 0.1 mmol) and water (10 ml) was sealed into a Teflon-lined stainless autoclave and heated at 413 K for 3 days, then cooled to room temperature gradually and colourless block crystals of (I) were obtained. Analysis calculated for C20H16ZnN6O10: C 42.46, H 2.85, N 14.85; found: C 42.82, H 2.73, N 14.70.

Refinement

H atoms attached to N and O atoms were located in a difference Fourier maps and refined as riding in their as-found relative positions, with Uiso(H) = 1.5Ueq(O,N). Other H atoms were positioned geometrically with C—H = 0.95 Å and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

A view of the molecular of (I), showing the atom-labelling scheme and displacement ellipsoids at the 30% probability level.

Fig. 2.

Fig. 2.

The crystal packing of (I), showing the three-dimensional hydrogen-bonding network, H atoms have been omited for clarity.

Crystal data

[Zn(C10H6N3O4)2(H2O)2] F(000) = 1152
Mr = 565.76 Dx = 1.875 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
a = 7.4138 (9) Å θ = 2.5–28.3°
b = 20.204 (3) Å µ = 1.31 mm1
c = 13.4778 (17) Å T = 173 K
β = 97.008 (1)° Block, colorless
V = 2003.7 (4) Å3 0.27 × 0.17 × 0.10 mm
Z = 4

Data collection

Rigaku Mercury CCD diffractometer 2488 independent reflections
Radiation source: fine-focus sealed tube 1957 reflections with I > 2σ(I)
graphite Rint = 0.031
ω scan θmax = 28.3°, θmin = 2.5°
Absorption correction: multi-scan (CrystalClear; Rigaku, 2000) h = −9→9
Tmin = 0.754, Tmax = 0.878 k = −26→26
9235 measured reflections l = −17→17

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)] = 0.031 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090 H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0453P)2 + 2.1588P] where P = (Fo2 + 2Fc2)/3
2488 reflections (Δ/σ)max < 0.001
178 parameters Δρmax = 0.34 e Å3
1 restraint Δρmin = −0.37 e Å3

Special details

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)

x y z Uiso*/Ueq
Zn1 0.2500 0.2500 0.5000 0.02158 (12)
O1 0.1031 (3) 0.21527 (11) 0.36331 (14) 0.0405 (5)
N1 −0.0003 (2) 0.26283 (8) 0.56460 (13) 0.0181 (3)
C1 0.0872 (3) 0.37351 (10) 0.51444 (16) 0.0230 (4)
O2 0.1956 (2) 0.34788 (7) 0.46161 (13) 0.0296 (4)
N2 −0.2095 (2) 0.28420 (8) 0.67035 (13) 0.0204 (4)
C2 −0.2007 (3) 0.40644 (10) 0.68011 (17) 0.0239 (4)
O3 0.0612 (2) 0.43586 (7) 0.51721 (13) 0.0355 (4)
N3 −0.2067 (3) 0.03644 (9) 0.68078 (15) 0.0283 (4)
H3 −0.2203 −0.0056 0.6953 0.034*
C3 −0.0184 (3) 0.32960 (9) 0.57348 (15) 0.0184 (4)
O4 −0.1528 (3) 0.46001 (7) 0.63823 (14) 0.0368 (4)
C4 −0.1451 (3) 0.34251 (9) 0.63948 (15) 0.0192 (4)
O5 −0.2869 (2) 0.40756 (8) 0.75300 (12) 0.0322 (4)
C5 −0.1194 (3) 0.23786 (9) 0.62332 (15) 0.0184 (4)
C6 −0.1542 (3) 0.16745 (9) 0.63892 (15) 0.0180 (4)
C7 −0.2469 (3) 0.14843 (10) 0.71861 (17) 0.0250 (5)
H7 −0.2949 0.1811 0.7587 0.030*
C8 −0.2687 (3) 0.08256 (11) 0.73901 (17) 0.0278 (5)
H8 −0.3279 0.0698 0.7946 0.033*
C9 −0.1247 (3) 0.05237 (11) 0.60116 (18) 0.0311 (5)
H9 −0.0866 0.0184 0.5597 0.037*
C10 −0.0947 (3) 0.11772 (10) 0.57857 (17) 0.0251 (5)
H10 −0.0343 0.1288 0.5226 0.030*
H1B −0.008 (4) 0.2148 (13) 0.353 (2) 0.030*
H1A 0.135 (4) 0.1903 (13) 0.324 (2) 0.030*
H4A −0.080 (3) 0.4538 (12) 0.5916 (16) 0.030*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Zn1 0.0248 (2) 0.01734 (18) 0.0245 (2) 0.00358 (13) 0.01053 (13) 0.00102 (13)
O1 0.0245 (9) 0.0669 (14) 0.0305 (10) 0.0044 (9) 0.0054 (8) −0.0200 (9)
N1 0.0208 (8) 0.0139 (8) 0.0206 (8) 0.0008 (6) 0.0066 (7) 0.0011 (6)
C1 0.0266 (11) 0.0175 (10) 0.0261 (11) 0.0015 (8) 0.0088 (9) 0.0026 (8)
O2 0.0361 (9) 0.0201 (7) 0.0366 (9) 0.0046 (7) 0.0203 (7) 0.0067 (7)
N2 0.0216 (9) 0.0161 (8) 0.0250 (9) −0.0002 (7) 0.0085 (7) −0.0004 (7)
C2 0.0263 (11) 0.0184 (10) 0.0280 (11) 0.0016 (8) 0.0077 (9) −0.0012 (8)
O3 0.0493 (11) 0.0144 (7) 0.0482 (11) 0.0022 (7) 0.0275 (9) 0.0071 (7)
N3 0.0356 (11) 0.0140 (8) 0.0359 (11) −0.0042 (7) 0.0074 (8) 0.0035 (7)
C3 0.0209 (10) 0.0140 (9) 0.0212 (10) 0.0006 (7) 0.0063 (8) 0.0004 (7)
O4 0.0576 (12) 0.0155 (7) 0.0430 (10) 0.0036 (7) 0.0291 (9) −0.0001 (7)
C4 0.0222 (10) 0.0144 (9) 0.0220 (10) 0.0007 (7) 0.0062 (8) 0.0013 (7)
O5 0.0417 (10) 0.0220 (8) 0.0370 (9) 0.0018 (7) 0.0215 (8) −0.0053 (7)
C5 0.0204 (10) 0.0153 (9) 0.0199 (10) −0.0008 (7) 0.0045 (8) 0.0015 (7)
C6 0.0186 (10) 0.0145 (9) 0.0213 (10) −0.0013 (7) 0.0034 (8) 0.0016 (7)
C7 0.0309 (12) 0.0183 (10) 0.0275 (11) −0.0017 (8) 0.0101 (9) −0.0008 (8)
C8 0.0324 (12) 0.0239 (11) 0.0287 (12) −0.0055 (9) 0.0109 (10) 0.0054 (9)
C9 0.0411 (14) 0.0190 (10) 0.0353 (13) −0.0016 (9) 0.0137 (10) −0.0037 (9)
C10 0.0312 (12) 0.0195 (10) 0.0266 (11) −0.0023 (8) 0.0115 (9) −0.0011 (8)

Geometric parameters (Å, °)

Zn1—O2 2.0713 (15) C2—O4 1.290 (3)
Zn1—O2i 2.0713 (15) C2—C4 1.481 (3)
Zn1—O1 2.1407 (18) N3—C9 1.336 (3)
Zn1—O1i 2.1407 (18) N3—C8 1.335 (3)
Zn1—N1i 2.1592 (17) N3—H3 0.8800
Zn1—N1 2.1592 (17) C3—C4 1.395 (3)
O1—H1B 0.82 (3) O4—H4A 0.885 (16)
O1—H1A 0.78 (3) C5—C6 1.466 (2)
N1—C5 1.353 (3) C6—C7 1.398 (3)
N1—C3 1.362 (2) C6—C10 1.397 (3)
C1—O2 1.249 (3) C7—C8 1.372 (3)
C1—O3 1.276 (2) C7—H7 0.9500
C1—C3 1.478 (3) C8—H8 0.9500
N2—C5 1.352 (3) C9—C10 1.379 (3)
N2—C4 1.355 (2) C9—H9 0.9500
C2—O5 1.236 (3) C10—H10 0.9500
O2—Zn1—O2i 180.0 C9—N3—C8 121.80 (19)
O2—Zn1—O1 92.00 (8) C9—N3—H3 119.1
O2i—Zn1—O1 88.00 (8) C8—N3—H3 119.1
O2—Zn1—O1i 88.00 (8) N1—C3—C4 108.82 (17)
O2i—Zn1—O1i 92.00 (8) N1—C3—C1 118.85 (17)
O1—Zn1—O1i 180.0 C4—C3—C1 132.32 (18)
O2—Zn1—N1i 99.47 (6) C2—O4—H4A 114.6 (16)
O2i—Zn1—N1i 80.53 (6) N2—C4—C3 108.85 (17)
O1—Zn1—N1i 89.17 (7) N2—C4—C2 121.34 (18)
O1i—Zn1—N1i 90.83 (7) C3—C4—C2 129.67 (18)
O2—Zn1—N1 80.53 (6) N1—C5—N2 114.27 (17)
O2i—Zn1—N1 99.47 (6) N1—C5—C6 125.79 (18)
O1—Zn1—N1 90.83 (7) N2—C5—C6 119.94 (18)
O1i—Zn1—N1 89.17 (7) C7—C6—C10 117.99 (18)
N1i—Zn1—N1 180.0 C7—C6—C5 119.26 (18)
Zn1—O1—H1B 123.2 (19) C10—C6—C5 122.73 (18)
Zn1—O1—H1A 129 (2) C8—C7—C6 120.1 (2)
H1B—O1—H1A 105 (3) C8—C7—H7 120.0
C5—N1—C3 103.85 (16) C6—C7—H7 120.0
C5—N1—Zn1 147.69 (13) N3—C8—C7 120.1 (2)
C3—N1—Zn1 104.67 (12) N3—C8—H8 119.9
O2—C1—O3 122.40 (19) C7—C8—H8 119.9
O2—C1—C3 118.55 (18) N3—C9—C10 120.6 (2)
O3—C1—C3 119.02 (18) N3—C9—H9 119.7
C1—O2—Zn1 111.87 (13) C10—C9—H9 119.7
C5—N2—C4 104.20 (17) C9—C10—C6 119.3 (2)
O5—C2—O4 121.93 (19) C9—C10—H10 120.4
O5—C2—C4 120.28 (19) C6—C10—H10 120.4
O4—C2—C4 117.77 (19)
O2—Zn1—N1—C5 −170.7 (3) N1—C3—C4—N2 −1.3 (2)
O2i—Zn1—N1—C5 9.3 (3) C1—C3—C4—N2 177.0 (2)
O1—Zn1—N1—C5 97.4 (3) N1—C3—C4—C2 174.4 (2)
O1i—Zn1—N1—C5 −82.6 (3) C1—C3—C4—C2 −7.3 (4)
N1i—Zn1—N1—C5 37 (16) O5—C2—C4—N2 10.2 (3)
O2—Zn1—N1—C3 −19.40 (13) O4—C2—C4—N2 −171.3 (2)
O2i—Zn1—N1—C3 160.60 (13) O5—C2—C4—C3 −165.1 (2)
O1—Zn1—N1—C3 −111.28 (14) O4—C2—C4—C3 13.5 (4)
O1i—Zn1—N1—C3 68.72 (14) C3—N1—C5—N2 −1.2 (2)
N1i—Zn1—N1—C3 −171 (100) Zn1—N1—C5—N2 150.2 (2)
O3—C1—O2—Zn1 166.35 (18) C3—N1—C5—C6 179.3 (2)
C3—C1—O2—Zn1 −15.4 (3) Zn1—N1—C5—C6 −29.3 (4)
O2i—Zn1—O2—C1 24 (100) C4—N2—C5—N1 0.4 (2)
O1—Zn1—O2—C1 110.06 (17) C4—N2—C5—C6 179.97 (19)
O1i—Zn1—O2—C1 −69.94 (17) N1—C5—C6—C7 164.9 (2)
N1i—Zn1—O2—C1 −160.45 (16) N2—C5—C6—C7 −14.7 (3)
N1—Zn1—O2—C1 19.55 (16) N1—C5—C6—C10 −13.6 (3)
C5—N1—C3—C4 1.5 (2) N2—C5—C6—C10 166.9 (2)
Zn1—N1—C3—C4 −163.20 (14) C10—C6—C7—C8 3.5 (3)
C5—N1—C3—C1 −177.10 (19) C5—C6—C7—C8 −175.1 (2)
Zn1—N1—C3—C1 18.2 (2) C9—N3—C8—C7 −0.8 (4)
O2—C1—C3—N1 −3.1 (3) C6—C7—C8—N3 −2.2 (3)
O3—C1—C3—N1 175.2 (2) C8—N3—C9—C10 2.6 (4)
O2—C1—C3—C4 178.8 (2) N3—C9—C10—C6 −1.2 (4)
O3—C1—C3—C4 −3.0 (4) C7—C6—C10—C9 −1.8 (3)
C5—N2—C4—C3 0.6 (2) C5—C6—C10—C9 176.7 (2)
C5—N2—C4—C2 −175.55 (19)

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1B···N2ii 0.82 (3) 2.08 (3) 2.898 (3) 178 (3)
N3—H3···O5iii 0.88 1.89 2.755 (2) 169.
O4—H4A···O3 0.89 (2) 1.58 (2) 2.459 (2) 173 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JH2196).

References

  1. Li, X., Liu, W., Wu, B.-L. & Zhang, H.-Y. (2009). Acta Cryst. E65, m820–m821. [DOI] [PMC free article] [PubMed]
  2. Li, X., Wu, B. L., Niu, C. Y., Niu, Y. Y. & Zhang, H. Y. (2009). Cryst. Growth Des.9, 3423–3431.
  3. Rigaku (2000). CrystalClear Rigaku Corporation, Tokyo, Japan.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Sun, T., Ma, J.-P., Huang, R.-Q. & Dong, Y.-B. (2006). Acta Cryst. E62, o2751–o2752.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810031855/jh2196sup1.cif

e-66-m1178-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810031855/jh2196Isup2.hkl

e-66-m1178-Isup2.hkl (122.3KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES