Guo-Li
Zheng
b,
Guo-Cheng
Yang
c,
Shu-Yan
Song
a,
Xue-Zhi
Song
a and
Hong-Jie
Zhang
*a
aState Key Laboratory of Application of Rare Earth Resources Utilization, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, PR China. E-mail: hongjie@ciac.jl.cn; Fax: +86 431 85698041; Tel: +86 431 85262127
bKey Laboratory of Catalysis and Materials Science of the State Ethnic Affairs Commission & Ministry of Education, Hubei Province, South-Central University for Nationalities, Wuhan, 430074, PR China
cSchool of Chemistry and Life Science, Changchun University of Technology, Changchun 130012, PR China
First published on 21st October 2013
A novel porous MOF based on the layer framework and p-sulfonatocalix[4]arene nanocapsule has been established, which is assembled by molecule recognition. The channel structure of compound 1 shows the proton-conductive property with 5.42 × 10−7 S cm−1 at 298 K and 95% relative humidity.
Recently calixarenes as building blocks have been widely used to construct various MOFs due to their interesting biological behaviors and potential applications in materials science.5,6 The self-assembly of calixarenes with metal ions and organic molecules, can afford various supramolecular wonderful structures, such as porous structures,7 molecular capsules,8 bilayers,9 2D and 3D coordination polymers.10 Proton conductivities in MOFs materials need proton carries such as NH4+, H3O+ or H+ given by acid or OH groups, and hydrogen-bond networks for proton conductions. The p-sulfonatocalix[n]arenes (n = 4, 5, 6, 8) possess many sulfonate groups and OH groups, which not only ligate the metal ions into multidimensional frameworks possible, but also may be available to further act as proton carries. A survey of the Cambridge Structural Database shows that most of MOFs based on the p-sulfonatocalix[n]arenes possess plenty of water molecules and OH groups inside the frameworks. In addition, many macromolecular sulfonic acid polymers as proton conductors have been established.11 Recently, a MOF (the trisodium salt of 2,4,6-trihydroxy-1,3,5-benzenetrisulfonate) that conducts protons with sulfonate groups had been reported.3a All above results indicate MOFs based on p-sulfonatocalix[4]arenes are appealing candidates for proton conductions.
Our group has been pursuing supramolecular porous structures built from p-sulfonatocalix[n]arene.12 The cavity of p-sulfonatocalix[n]arene structure suggests that the design of new porous MOFs based on p-sulfonatocalix[n]arenes can rely on molecular recognition. When suitable guests, such as tetraphenylphosphonium cations,13a phenanthroline,13b pyridine N-oxide,13c [Cu(bpdo)3]2+ (2,2′-bipyridine-N,N′-dioxide, bpdo),12aetc., are employed in these systems, porous materials can be expected. In this paper, a new supramolecular MOF which contains continuous water molecules inside the pores has been prepared by molecular recognition; and the proton conductivity of porous material has also been investigated.
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1
:
3
:
2 (pH = 3.5) was dissolved in 20 ml hot water. Red crystals of compound 1 were obtained after volatilizing at room temperature for a few days (0.0446 g, yield: 57%, based on p-sulfonato-calix[4]arenes). Microanalysis (CHN) was not feasible due to the highly hydrated nature of the complexes
, triclinic, a = 17.0111(11) Å, b = 17.6763(12) Å, c = 20.7596(15) Å, α = 70.1290(10)°, β = 70.3930(10)°, γ = 89.5450(10)°,V = 5490.4(6) Å3, Z = 2, T = 193 K, λ = 0.71073 Å, Rint = 0.0341. A total of 39
319 reflections were collected in the range 1.25 < θ < 25, of which 19
243 were unique. GOF = 0.961, R1 = 0.1306, wR2 (all data) = 0.2774. One of the sulfonate groups (at Fig. S4†) was refined by disorder. Non-hydrogen atoms were refined anisotropically. The free water molecules were removed before the cited solvent accessible volume was calculated by Platon.14 Large water inside the channels and weak diffraction quality of compound 1 are responsible for the relatively high value of agreement factor R1. CCDC 885465 contains the supplementary crystallographic data for this paper.
The powder X-ray diffraction (XRD) of compound 1 was examined on a Rigaku-Dmax 2500 diffractometer using Cu Kα radiation (λ = 0.15405 nm). Fourier transform infrared (FTIR) spectra were measured within the 4000–400 cm wavenumber range using a Perkin-Elmer model 580B IR spectrophotometer with the KBr pellet technique. Thermogravimetric analysis (TGA) was performed on a SDT2960 analyzer (Shimadzu, Japan) up to 800 °C at a heating rate of 10 °C min−1 under N2.
The powders were prepared by grinding the sample into a homogeneous powder with a mortar and pestle. The powders were then added to a standard 11 mm die, sandwiched between two stainless steel electrodes and pressed at 5000 kg for 2 min; the pellet was 11 mm in diameter and 1.16 mm in thickness. Measurements were carried out using an impedance and gain-phase analyzer (PARSTAT 2273, Ametek, USA), 1 Hz–1 MHz, with a two-probe electrochemical cell and an applied ac voltage of 10–100 mV (unless otherwise stated). Measurements were taken in the temperature range of 25–85 °C with 95% relative humidity. Conductivity was calculated using the following equation:
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| Fig. 2 The packing diagram of compound 1 down the a axis, showing the channel structure, the dissociative water molecules are omitted for clarity. | ||
The Cu and L (4,4′-bipyridine-N,N′-dioxide) form a layered structure based on (4, 4) topology which is composed of bowl shape cavities (Fig. 4 and Fig. S3†). The four rigid modules of L make up the bowl frameworks, these L modules are bridged by four copper centers. All the copper centers in the layer structure are octahedrally coordinated, which are ligated by two water molecules and four oxygen atoms of L. The bowl can be likened to a calix[4]arene with a cone conformation, in which each copper center is related to a methylene group on the backbone of a calix[4]arene (Fig. S3†). In the metallacalix[4]arenes 1, the four copper atoms build up an almost equilateral square with Cu⋯Cu distances of 12.378, 12.276, 12.365 and 12.274 Å, which make the layer as a suitable host for the supramolecular capsules (Fig. 4). The host layer and the guest capsules are held together through charge-assisted π⋯π interactions with the centroid⋯centroid distances of 3.762, 3.500, 3.612 and 3.507 Å (Fig. S4† and Fig. 5). In addition, the hydrogens of the L interact through C–H⋯O hydrogen bonds to the neighboring sulfonic groups of p-sulfonatocalix[4]arenes with the distances from 2.692 to 2.999 Å.
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| Fig. 4 A layered structure consisting of the L and the copper ions with (4, 4) topology as host for p-sulfonatocalix[4]arene nanocapsules. | ||
All the cavities of the layers are occupied by the p-sulfonatocalix[4]arenes of supramolecular capsules (Fig. 6). The up-rim of neighbouring bowl shape cavities are oriented in opposite directions, which template the up-rim neighboring calixarenes are also oriented in opposite directions. The noteworthy aspect of the title complex is that when the structure is viewed along the a and b axis, the whole framework forms pores constructed by the capsules and metal–organic cation framework (MOCF), which is clearly shown in Fig. 2 and Fig. S1.† The interlayer separations of 1 is about 18 Å. Different to traditional porous materials, the porous material is sustained exclusively by weak interactions. The solvent-accessible volumes of the unit cells of 1 was estimated, (PLATON program)11 to be 2836.2 Å3, which is approximately 51.7% of the unit-cell volume (5490.4 Å3).
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| Fig. 6 All the cavities of the layers occupied by the p-sulfonatocalix[4]arenes, all the hydrogen atoms are omitted for clarity. | ||
Recently, p-sulfonatocalix[4]arene templated by Ag-hexamethylenetetramine coordination polymer forming a porous structure was reported by our group.12a Different to the above mentioned structure, this MOCF not only acts as template, but also act as hosts for calixarene capsules. The surface of the pores are lined exclusively with oxygen atoms of sulfonate groups and OH groups. Significantly, these groups serve to anchor free water molecules into pores forming a potential hydrogen-bond transfer pathway.
We are interested in the proton conductivity of metal–organic frameworks based on calixarenes. The conductivity of 1 was carried out and determined from the semicircle in the Nyquist plot, as shown in Fig. S6.† The proton conductivity of 1 was 5.42 × 10−7 S cm−1 at 298 K and 95% relative humidity (RH) (Table S1†). The temperature dependence of the proton conductivity of 1 at 95% RH was shown in Fig. 7. Although the proton conductivity of compound 1 is lower compared with other known MOF material (8 × 10−3 S cm−1 at 298 K and 98% RH),2e our study reveals that the use of hydrophilic calixarenes with metal ions appears promising for producing proton conductive materials. The proton conductivity of compound 1 increased with increasing temperature. The activation energy was 0.39 eV, as determined from least-square fit of the slope. Therefore, proton conduction in compound 1 could be classified mainly as the Grotthuss mechanism. Hydrogen-bonded networks are formed along three-dimensional channels with the sulfonate groups, OH groups and water molecules. The contribution to the proton conductivity in compound 1 is thought to be these hydrogen-bonded networks.
Footnote |
| † Electronic supplementary information (ESI) available: Synthesis of compounds 1 and 2, crystallographic information, supplementary figures, XRD and TGA of the compounds. CCDC 885465. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c2ce26075a |
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