An unprecedented T4(1)4(2)5(2) water topology

An unprecedented T4(1)4(2)5(2) water topology

Inorganic Chemistry Communications 15 (2012) 252–255 Contents lists available at SciVerse ScienceDirect Inorganic Chemistry Communications journal h...

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Inorganic Chemistry Communications 15 (2012) 252–255

Contents lists available at SciVerse ScienceDirect

Inorganic Chemistry Communications journal homepage: www.elsevier.com/locate/inoche

An unprecedented T4(1)4(2)5(2) water topology Xiao-zhao Tian, Yu-mei Song, Gong-ming Sun, Hai-xiao Huang, Wen-yuan Xu, Xue-feng Feng, Feng Luo ⁎ College of Biology, Chemistry and Material Science, East China Institute of Technology, Fuzhou, 344000 Jiangxi, China

a r t i c l e

i n f o

Article history: Received 13 September 2011 Accepted 23 October 2011 Available online 3 November 2011 Keywords: Hydrothermal synthesis Zn(II) compound Water structure

a b s t r a c t Herein, a special water cluster was observed in a metal-organic framework, namely [Zn(μ-(H2O)2)(L) (BDC)]·5H2O (1, L = 2-(pyridine-4-yl)-1H-benzo[d]imidazole, H2BDC = terephthalic acid). In this ice-like water cluster, tetramer water clusters are combined together by sharing one corner to give rise to the T4(1) water structure, while the pentamer water clusters are located on two sides of this T4(1) water chain by sharing two edges with two tetramer water clusters, thus resulting in the overall T4(1)4(2)5(2) water topology. © 2011 Elsevier B.V. All rights reserved.

Water – a basal composition of vital system – has received explosive scientific interest during the past few years due not only to its elegant water morphologies but also to its unusual properties in many physical, chemical, and biological processes. In the past decades, isolated small water clusters such as (H2O)10[1], (H2O)12[2], and (H2O)21[3] have been extensively disclosed both theoretically and experimentally. Recently, more attention has been paid to the infinite 1D and 2D water morphologies, lying between small water clusters and bulk water/ice [4–7]. In the realm of water morphology, the water tetramer is popular, and we have witnessed a large number of water structures containing water tetramer such as T4(0)A2 [8], T4(1) [9,10],and T4(2)6(2) [11,12]. But recently, experimental and academic studies on the water pentamers are also becoming remarkable [13–16]. However, by contrast to the productive water morphologies based on water tetramer, the water pentamer involving water morphologies is less developed, and until now only limited cases are revealed, such as T5(0) [13], T5(1) [14],T5(2) [15],and L38(10)5(2)4(2)4(1) [16]. Thereby, exploring new 1D and 2D water morphology based on water pentamer will be very interesting but a big challenge. In this work, we presented an unprecedented water pentamer involving water morphology defined as T4(1)4(2)5(2), wherein the ratio of water tetramer and pentamer is 2:1. Polymer 1 was synthesized by the hydrothermal reaction of Zn (NO3)2, H2BDC, L, in the ratio of 1:1:1 and 6 ml H2O at 160 °C for 3 days [17]. The phase purity of the bulk samples is confirmed by EA and XRD studies (see Supplementary Data, Fig. S1). The TG analysis suggests the loss of guest water molecules is about 30–210° (exp. 15.8%, calc. 16.3%), and the loss of coordination water molecules cause the chemical decomposition of this compound, see Fig. S2.

⁎ Corresponding author. Tel./fax: + 86 794 8258320. E-mail address: [email protected] (F. Luo). 1387-7003/$ – see front matter © 2011 Elsevier B.V. All rights reserved. doi:10.1016/j.inoche.2011.10.038

The single crystal X-ray diffraction shows that polymer 1 crystallizes in monoclinic, P21/c space group [18]. As shown in Fig. 1, the Zn(II) ions are five-coordinated by two BDC 2 −oxygen atoms, one L nitrogen, and two terminal water molecules, resulting in the axiselongated triangular bipyramidal geometry, where Zn–O(water) lengths range from 2.139(3) Å to 2.121(3) Å, Zn–O(BDC 2 −) lengths range from 1.981(2) Å to 2.007(2) Å, and Zn–N(L) length is 2.067(3) Å. Along a direction, the Zn(II) ions are in-turn bridged by BDC2 −ligands to create the 1D chain structure. Through hydrogen bonds of O1-HA (water)···O5(BDC2 −)/2.746 Å/170.25°, O1-HB (water)···O4(BDC2 −)/ 2.761 Å/160.97°, O2-HA(water)···O5(BDC2 −)/2.654 Å/168.46° between water molecules and BDC2 −oxygen atoms, these 1D chains are combined together to give rise to the 2D supramolecular net (Fig. 2). The 3D stacking architecture shows a solvent-accessible void space of 601.6 Å3, equal to 24.9% of the cell volume (Fig. 3), which is filled with free water molecules. A clear insight into this water structure is shown in Figs. 4 and 5. H2O(7), H2O(8) and two H2O(9) molecules composed of a water tetramer by H-bonds of O7-H7B···O9/2.751 Å/162.94°, O8-H8B···O9/ 2.752 Å/171.56°, O9-H9B···O7/2.750 Å/168.06°, O9-H9A···O8/2.754 Å/ 174.49°. The H-bond lengths of water tetramer are at the average value of 2.752 Å. As shown in Fig. 4, O9 displays four-fold H-bond, and adjacent tetramers share H2O(9) to create a T4(1) tape. The dihedral angle between the adjacent water tetramers is 89.64°, nearly a vertical pattern. The water pentamer consists of H2O(7), H2O(8), H2O(9), H2O(10) and H2O(11), through hydrogen bonds of O7-H7A···O11/2.730 Å/141.54°, O8-H8B···O9/2.752 Å/ 171.56°, O9-H9B···O7/2.750 Å/168.06°, O10H10A···O8/2.782 Å/172.66°, and O10-H10B···O11/3.088 Å/ 173.12°. O10 deviates of 0.408 Å from the plane built by O7, O8, O9 and O11. The O···O···O angle in pentamers are O7···O9···O8/110.43°, O9··· O8···O10/114.18°, O8···O10···O11 /96.21°, O10···O11···O7/113.39°, and O11···O7···O9/104.04°, closing to a regular polygon shape. The average H-bond lengths in this water pentamer is 2.820 Å, comparable with that such as 2.74 Å [13], 2.82 Å [14], 2.84 Å [15], and 2.81 Å [16], observed in other pentamers.

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Fig. 1. The coordination surroundings of Zn(II) ions and the guest water molecules in 1. The hydrogen atoms linked to C atoms are omitted for clarity. Atoms are colored as follows: C/green, N/blue, Zn/pink, O/red, H/ purple.

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Furthermore, these water pentamers via sharing two edges with two tetramers generate the T4(2)5(2) water tape with the dihedral angle of 120.38° and 123.73°(Fig. 5). Combined with the abovedefined T4(1) water structure, the overall water structure is defined as a T4(1)4(2)5(2) tape. On the whole, the average H-bond length in the T4(1)4(2)5(2) cluster is 2.801 Å, comparable to the ice II phase (2.77–2.84) Å [16]. The FTIR spectroscopic studies reveals a band centered about 3225 cm − 1, attributed to the O–H stretching frequency of the water cluster. Generally speaking, the O–H stretching vibration in ice appears at 3220 cm − 1, while in liquid it shifts to 3280 and 3490 cm − 1[11]. Therefore, the O–H stretching frequency of the water cluster in 1 is more like ice with a slight variation attributable to its surroundings. This result is well consistent with the analysis of average H-bond lengths. In literatures, we find two cases composed of both water tetramers and water pentamers. In one case defined as L38(10)5(2)4(2) 4(1) (Fig. S3a) [19], water tetramers connect to water pentamers through sharing one edge to give a 1D T4(2)5(2) tape, while water tetramers are isolated from each other. In the other case [20], the combination of water tetramers and water pentamers constructs a complicated 2D water layer morphology (Fig. S3b). By contrast, for the first time, a tape water structure built on water tetramers and water pentamers is observed in 1. Moreover, the water tape is stabilized by hydrogen bonds between water structure and host framework: N2(L)–H···O7, N3 (L)–H···O8, O2–H···O10, O3–H···O11 (Fig. 6). The N(L)–O distances are 2.784 Å and 2.825 Å respectively, indicating a relatively strong interactions in this structure as the normally N···O distance

Fig. 2. H-bonded layer structure of polymer 1.

Fig. 3. Viewed down c axis, the 3D stacking architecture displays the channels that host water molecules.

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Fig. 4. View of the T4(1) water structure.

Fig. 5. View of the T4(1)4(2)5(2) water structure.

in N–H···O hydrogen bonds are in range of 2.81 Å–3.04 Å [21–22]. The distances of O2···O10 and O3···O11 are 2.905 Å and 2.841 Å respectively.

In summary, in this work we present the synthesis and structure of a 1D Zn(II) compound and a novel water structure filled in the channel. The stacking fashion suggests the potential porous

Fig. 6. View of the water cluster filled in the hole of the host framework through hydrogen bonds.

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coordination compounds of 1 and the guest water molecules observed in 1 display a highly rare T4(1)4(2)5(2) pattern. To some extent, this work has enriched the database of water chemistry and given a new insight into the water structure. Moreover, the 1D system involving potential porosity is very interesting, as this kind of materials usually perform dynamic porous properties [23]. Acknowledgements This work was supported by the Doctoral Start-up Fund of East China Institute of Technology, the Foundation of Jiangxi Educational Committee (no. GJJ11153), the Natural Science Foundation of Jiangxi Province of China (no. 2010GQH0005), the China Postdoctoral Science Foundation (no. 20100480725), and the Foundation of Key Laboratory of Radioactive Geology and Exploration Technology Fundamental Science for National Defense (2010RGET07). Appendix A. Supplementary material Supplementary data to this article can be found online at doi:10. 1016/j.inoche.2011.10.038. References [1] M. Yoshizawa, T. Kusukawa, M. Kawano, T. Ohhara, I. Tanaka, K. Kurihara, N. Niimura, M. Fujita, Endohedral clusterization of ten water molecules into a “molecular ice” within the hydrophobic pocket of a self-assembled cage, J. Am. Chem. Soc. 127 (2005) 2798–2799. [2] X.L. Wang, H.Y. Lin, B. Mu, A.X. Tian, G.C. Liu, Encapsulation of discrete (H2O)12 clusters in a 3D three-fold interpenetrating metal-organic framework host with (3,4)-connected topology, Dalton Trans. 27 (2010) 6187–6189. [3] M.L. Cao, J.J. Wu, H.J. Mo, B.H. Ye, Template trapping and crystal structure of the magic number (H2O)21 cluster in the tetrahedral hole of a nanoscale global ion packed in a face-centered cubic pattern, J. Am. Chem. Soc. 10 (2009) 3458–3459. [4] S.Q. Zang, Y. Su, C.Y. Duan, Y.Z. Li, H.Z. Zhu, Q.J. Meng, Coexistence of chiral hydrophilic and achiral hydrophobic channels in one multi-helical-array metal-organic framework incorporating helical water cluster chains, Chem. Commun. (2006) 4997–4999. [5] N.S. Oxtoby, A.J. Blake, N.R. Champness, C. Wilson, Water superstructures within organic arrays; hydrogen-bonded water sheets, chains and clusters, Chem. Eur. J. 11 (2005) 4643–4654. [6] L. Infantes, S. Motherwell, Water clusters in organic molecular crystals, CrystEngComm 4 (2002) 454–461.

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