supplementary materials
catena-Poly[[diaquazinc(II)]-
-4,4'-(methylenedioxy)dibenzoato]
Zinc(II) acetate dihydrate (0.066 g, 0.3 mol), bis(4-benzoateoxyl)methane
(0.058 g, 0.2 mmol), sodium hydroxide (0.016 g, 0.4 mmol) and water (14 ml)
were placed in a 23 ml Teflon-lined autoclave, and the autoclave was heated at
423 K for 3 d. After cooling slowly to room temperature at a rate of 10 K h-1, colourless crystals of (I) were obtained.
C-bound H atoms were treated as riding, with C—H = 0.93 and 0.97Å and
Uiso(H) = 1.2 times Ueq(C). O-bound H atoms were located in
a difference Fourier map and refined as riding in their as-found relative
positions; Uiso(H) = 1.5Ueq(O).
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, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL-Plus (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).
catena-Poly[[diaquazinc(II)]-µ-4,4'-(methylenedioxy)dibenzoato]
top
Crystal data top
| [Zn(C15H10O6)(H2O)2] | F(000) = 396 |
| Mr = 387.63 | Dx = 1.705 Mg m−3 |
| Monoclinic, P2/c | Mo Kα radiation, λ = 0.71069 Å |
| Hall symbol: -P 2yc | Cell parameters from 3185 reflections |
| a = 13.496 (1) Å | θ = 2.1–27.4° |
| b = 4.931 (1) Å | µ = 1.67 mm−1 |
| c = 12.357 (1) Å | T = 293 K |
| β = 113.352 (1)° | Block, colourless |
| V = 755.0 (2) Å3 | 0.21 × 0.19 × 0.15 mm |
| Z = 2 | |
Data collection top
Rigaku R-AXIS RAPID diffractometer | 1696 independent reflections |
| Radiation source: fine-focus sealed tube | 1461 reflections with I > 2σ(I) |
| graphite | Rint = 0.027 |
| Detector resolution: 10 pixels mm-1 | θmax = 27.5°, θmin = 3.3° |
| ω scans | h = −10→17 |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | k = −6→5 |
| Tmin = 0.707, Tmax = 0.780 | l = −15→15 |
| 4318 measured reflections | |
Refinement top
| 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)] = 0.032 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.075 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.0304P)2 + 0.2993P] where P = (Fo2 + 2Fc2)/3 |
| 1696 reflections | (Δ/σ)max < 0.001 |
| 118 parameters | Δρmax = 0.25 e Å−3 |
| 0 restraints | Δρmin = −0.30 e Å−3 |
Crystal data top
| [Zn(C15H10O6)(H2O)2] | V = 755.0 (2) Å3 |
| Mr = 387.63 | Z = 2 |
| Monoclinic, P2/c | Mo Kα radiation |
| a = 13.496 (1) Å | µ = 1.67 mm−1 |
| b = 4.931 (1) Å | T = 293 K |
| c = 12.357 (1) Å | 0.21 × 0.19 × 0.15 mm |
| β = 113.352 (1)° | |
Data collection top
Rigaku R-AXIS RAPID diffractometer | 1696 independent reflections |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | 1461 reflections with I > 2σ(I) |
| Tmin = 0.707, Tmax = 0.780 | Rint = 0.027 |
| 4318 measured reflections | θmax = 27.5° |
Refinement top
| R[F2 > 2σ(F2)] = 0.032 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.075 | Δρmax = 0.25 e Å−3 |
| S = 1.06 | Δρmin = −0.30 e Å−3 |
| 1696 reflections | Absolute structure: ? |
| 118 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
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| | x | y | z | Uiso*/Ueq | Occ. (<1) |
| Zn1 | 0.0000 | 0.02532 (7) | 0.2500 | 0.03611 (14) | |
| O3 | 0.48509 (13) | 1.0388 (3) | 0.65056 (14) | 0.0430 (4) | |
| O4 | 0.06484 (17) | −0.2446 (4) | 0.17945 (17) | 0.0484 (5) | |
| O2 | 0.07014 (13) | 0.2515 (3) | 0.46679 (14) | 0.0420 (4) | |
| O1 | 0.12200 (13) | 0.2746 (3) | 0.31887 (13) | 0.0406 (4) | |
| C5 | 0.39531 (18) | 0.8759 (5) | 0.60267 (19) | 0.0351 (5) | |
| C7 | 0.22564 (18) | 0.6856 (4) | 0.58165 (19) | 0.0356 (5) | |
| H7 | 0.1685 | 0.6754 | 0.6055 | 0.043* | |
| C1 | 0.13275 (18) | 0.3401 (4) | 0.42419 (18) | 0.0331 (5) | |
| C8 | 0.5000 | 1.1980 (7) | 0.7500 | 0.0451 (8) | |
| H8A | 0.4375 | 1.3138 | 0.7330 | 0.054* | 0.50 |
| H8B | 0.5625 | 1.3138 | 0.7670 | 0.054* | 0.50 |
| C2 | 0.22362 (18) | 0.5269 (4) | 0.48823 (19) | 0.0328 (5) | |
| C6 | 0.31099 (19) | 0.8591 (5) | 0.6403 (2) | 0.0379 (5) | |
| H6 | 0.3119 | 0.9624 | 0.7037 | 0.046* | |
| C3 | 0.3096 (2) | 0.5481 (5) | 0.4528 (2) | 0.0434 (6) | |
| H3 | 0.3092 | 0.4453 | 0.3896 | 0.052* | |
| C4 | 0.3942 (2) | 0.7180 (5) | 0.5100 (2) | 0.0447 (6) | |
| H4 | 0.4515 | 0.7273 | 0.4863 | 0.054* | |
| H2 | 0.069 (3) | −0.244 (7) | 0.110 (3) | 0.100 (13)* | |
| H1 | 0.085 (2) | −0.374 (6) | 0.210 (2) | 0.046 (8)* | |
Atomic displacement parameters (Å2) top| | U11 | U22 | U33 | U12 | U13 | U23 |
| Zn1 | 0.0455 (2) | 0.0276 (2) | 0.0380 (2) | 0.000 | 0.01943 (18) | 0.000 |
| O3 | 0.0416 (9) | 0.0491 (10) | 0.0364 (9) | −0.0115 (8) | 0.0132 (7) | 0.0005 (7) |
| O4 | 0.0832 (14) | 0.0311 (10) | 0.0397 (10) | 0.0128 (9) | 0.0338 (10) | 0.0040 (8) |
| O2 | 0.0471 (9) | 0.0448 (9) | 0.0359 (9) | −0.0096 (8) | 0.0183 (7) | 0.0003 (7) |
| O1 | 0.0538 (10) | 0.0371 (9) | 0.0338 (9) | −0.0057 (8) | 0.0205 (8) | −0.0074 (7) |
| C5 | 0.0361 (12) | 0.0332 (11) | 0.0337 (12) | −0.0026 (10) | 0.0114 (10) | 0.0052 (10) |
| C7 | 0.0367 (12) | 0.0370 (12) | 0.0370 (12) | −0.0021 (10) | 0.0189 (10) | −0.0009 (10) |
| C1 | 0.0404 (12) | 0.0269 (10) | 0.0293 (11) | 0.0039 (9) | 0.0110 (10) | 0.0010 (9) |
| C8 | 0.045 (2) | 0.0317 (17) | 0.051 (2) | 0.000 | 0.0109 (16) | 0.000 |
| C2 | 0.0379 (12) | 0.0304 (11) | 0.0301 (11) | −0.0009 (9) | 0.0135 (9) | 0.0015 (9) |
| C6 | 0.0445 (13) | 0.0378 (12) | 0.0338 (12) | −0.0033 (10) | 0.0179 (11) | −0.0055 (10) |
| C3 | 0.0488 (14) | 0.0483 (14) | 0.0398 (13) | −0.0055 (12) | 0.0246 (12) | −0.0078 (11) |
| C4 | 0.0447 (14) | 0.0506 (14) | 0.0483 (14) | −0.0037 (12) | 0.0285 (12) | −0.0033 (12) |
Geometric parameters (Å, °) top
| Zn1—O1 | 1.9582 (18) | C7—C2 | 1.386 (3) |
| Zn1—O1i | 1.9582 (18) | C7—C6 | 1.387 (3) |
| Zn1—O4 | 1.975 (2) | C7—H7 | 0.9300 |
| Zn1—O4i | 1.975 (2) | C1—C2 | 1.487 (3) |
| O3—C5 | 1.377 (3) | C8—O3ii | 1.404 (2) |
| O3—C8 | 1.404 (2) | C8—H8A | 0.9700 |
| O4—H2 | 0.88 (4) | C8—H8B | 0.9700 |
| O4—H1 | 0.74 (3) | C2—C3 | 1.396 (3) |
| O2—C1 | 1.239 (3) | C6—H6 | 0.9300 |
| O1—C1 | 1.292 (3) | C3—C4 | 1.366 (3) |
| C5—C4 | 1.380 (3) | C3—H3 | 0.9300 |
| C5—C6 | 1.392 (3) | C4—H4 | 0.9300 |
| | | |
| O1—Zn1—O1i | 102.26 (11) | O1—C1—C2 | 115.52 (19) |
| O1—Zn1—O4 | 99.87 (9) | O3—C8—O3ii | 112.0 (3) |
| O1i—Zn1—O4 | 132.40 (8) | O3—C8—H8A | 109.2 |
| O1—Zn1—O4i | 132.40 (8) | O3ii—C8—H8A | 109.2 |
| O1i—Zn1—O4i | 99.87 (9) | O3—C8—H8B | 109.2 |
| O4—Zn1—O4i | 95.27 (13) | O3ii—C8—H8B | 109.2 |
| C5—O3—C8 | 119.93 (16) | H8A—C8—H8B | 107.9 |
| Zn1—O4—H2 | 130 (2) | C7—C2—C3 | 118.3 (2) |
| Zn1—O4—H1 | 119 (2) | C7—C2—C1 | 122.2 (2) |
| H2—O4—H1 | 111 (3) | C3—C2—C1 | 119.5 (2) |
| C1—O1—Zn1 | 109.52 (14) | C7—C6—C5 | 118.8 (2) |
| O3—C5—C4 | 113.8 (2) | C7—C6—H6 | 120.6 |
| O3—C5—C6 | 126.0 (2) | C5—C6—H6 | 120.6 |
| C4—C5—C6 | 120.2 (2) | C4—C3—C2 | 120.8 (2) |
| C2—C7—C6 | 121.5 (2) | C4—C3—H3 | 119.6 |
| C2—C7—H7 | 119.3 | C2—C3—H3 | 119.6 |
| C6—C7—H7 | 119.3 | C3—C4—C5 | 120.4 (2) |
| O2—C1—O1 | 121.1 (2) | C3—C4—H4 | 119.8 |
| O2—C1—C2 | 123.4 (2) | C5—C4—H4 | 119.8 |
| | | |
| O1i—Zn1—O1—C1 | 86.84 (14) | O1—C1—C2—C7 | 158.0 (2) |
| O4—Zn1—O1—C1 | −135.58 (15) | O2—C1—C2—C3 | 159.3 (2) |
| O4i—Zn1—O1—C1 | −29.01 (18) | O1—C1—C2—C3 | −21.1 (3) |
| C8—O3—C5—C4 | −176.2 (2) | C2—C7—C6—C5 | 1.0 (3) |
| C8—O3—C5—C6 | 3.1 (3) | O3—C5—C6—C7 | 179.5 (2) |
| Zn1—O1—C1—O2 | −1.0 (3) | C4—C5—C6—C7 | −1.2 (3) |
| Zn1—O1—C1—C2 | 179.28 (14) | C7—C2—C3—C4 | 0.9 (4) |
| C5—O3—C8—O3ii | 64.94 (16) | C1—C2—C3—C4 | −180.0 (2) |
| C6—C7—C2—C3 | −0.9 (3) | C2—C3—C4—C5 | −1.2 (4) |
| C6—C7—C2—C1 | −179.9 (2) | O3—C5—C4—C3 | −179.3 (2) |
| O2—C1—C2—C7 | −21.7 (3) | C6—C5—C4—C3 | 1.3 (4) |
| Symmetry codes: (i) −x, y, −z+1/2; (ii) −x+1, y, −z+3/2. |
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H1···O1iii | 0.74 (3) | 2.13 (3) | 2.851 (3) | 167 (3) |
| O4—H2···O2iv | 0.88 (4) | 1.78 (4) | 2.657 (3) | 177 (4) |
| C8—H8A···Cg3v | 0.97 | 2.97 | 3.741 (3) | 137 |
| C8—H8B···Cg3vi | 0.97 | 2.97 | 3.741 (3) | 137 |
| Symmetry codes: (iii) x, y−1, z; (iv) x, −y, z−1/2; (v) x, y+1, z; (vi) −x+1, y+1, −z+3/2. |
Table 1
Selected geometric parameters (Å, °) top| Zn1—O1 | 1.9582 (18) | Zn1—O4 | 1.975 (2) |
| | | |
| O1—Zn1—O1i | 102.26 (11) | O1i—Zn1—O4 | 132.40 (8) |
| O1—Zn1—O4 | 99.87 (9) | O4—Zn1—O4i | 95.27 (13) |
| Symmetry codes: (i) −x, y, −z+1/2. |
Table 2
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H1···O1ii | 0.74 (3) | 2.13 (3) | 2.851 (3) | 167 (3) |
| O4—H2···O2iii | 0.88 (4) | 1.78 (4) | 2.657 (3) | 177 (4) |
| C8—H8A···Cg3iv | 0.97 | 2.97 | 3.741 (3) | 137 |
| C8—H8B···Cg3v | 0.97 | 2.97 | 3.741 (3) | 137 |
| Symmetry codes: (ii) x, y−1, z; (iii) x, −y, z−1/2; (iv) x, y+1, z; (v) −x+1, y+1, −z+3/2. |
The authors thank the Key Project of the Chinese Ministry of Education (No.
308008) and the Analysis and Testing Foundation of Northeast Normal University
for financial support.
Chen, X.-M. & Liu, G.-F. (2002). Chem. Eur. J. 8, 4811-4817.
Han, L., Zhou, Y., Zhao, W.-N., Li, X. & Liang, Y.-X. (2009). Cryst. Growth Des. 9, 660-662.
Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.
Li, X.-M., Dong, Y.-H., Wang, Q.-W. & Liu, B. (2007). Acta Cryst. E63, m1839–m1840.
Rigaku (1998). PROCESS-AUTO. Rigaku Corporation, Tokyo, Japan.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Recently, the area of metal-organic framework materials has become one of the intense research activity for their fascinating structural diversities and potential applications in catalysis, nonlinear optics and molecular sensing. As an important family of multidentate O-donor ligands, organic aromatic polycarboxylate ligands have been extensively employed in the preparation of metal-organic complexes because of their potential properties and intriguing structural topologies (Han et al., 2009; Li et al., 2007; Chen et al., 2002). Herein, we report the structure of the title complex with bis(4-benzoateoxyl)methane and zinc, [Zn(C15H10O6)(H2O)2] (I).
Single-crystal X-ray diffraction analyses revealed Zn(II) is tetra-coordinated and exhibits tetrahedral coordination environment supplied by two bis(4-benzoateoxyl)methane O atoms and two water molecules (Fig. 1). The Zn—O bond lengthes are in the normal range (Table 1). The bis(4-benzoateoxyl)methane ligand adopts bidentate coordinated modes and bond with two zinc ions to form a chain. Adjacent chains are linked by O—H···O hydrogen bonds and C—H···π interactions into a three-dimensional supramolecular network structure (Fig. 2, Table 2).