Jingui
Duan
*a,
Masakazu
Higuchi
bc,
Changchang
Zou
a,
Wanqin
Jin
a and
Susumu
Kitagawa
*b
aState Key Laboratory of Materials-Oriented Chemical Engineering, College of Chemistry and Chemical engineering, Nanjing Tech University, Nanjing, 210009, China. E-mail: duanjingui@njtech.edu.cn
bInstitute for Integrated Cell-Material Sciences (WPI-iCeMS), Kyoto University, Yoshida, Sakyo-ku, Kyoto 606-8501, Japan. E-mail: kitagawa@icems.kyoto-u.ac.jp
cJapan Science and Technology Agency, PRESTO 4-1-8 Honcho, Kawaguchi, Saitama 332-0012, Japan
First published on 24th June 2015
Two new porous coordination polymers (PCPs), ([Cu6(L)4·(H2O)6]·10DMA·4EtOH, (1) and [Cu5(L)2 (OH)2·(H2O)2·DMA2]·2DMA·EtOH·2H2O (2), were solvothermally synthesized and structurally characterized. Interestingly, their variable architectures controlled by solvent system exhibit a structural progression from an unusual non-crystallographic (NC) net to a (4,6)-connected framework with fsh topology. Moreover, the combination of 3D channels of about 3.0 × 7.2, 4.7 × 9.5, and 6.3 × 7.8 Å2, and functional –OH groups in 2′ lead to good selectivity of CO2 over CH4 (26-55 by IAST) at 273 K.
In addition, exposed functional sites and an optimized pore size play important roles in selective gas capture, due to the enhanced ability of host–guest interactions and also maximum size exclusion effects.6 The immobilization of functional sites (such as open metal sites and alkylamines) into PCPs was considered as rational design.7 Moreover, by introducing some specific substituent groups, e.g. –NH2, –COOH on the pore surface also worked well.8 However, there is a dearth of research on the investigation of the impact of open –OH groups in PCPs, because of the difficulty of getting open –OH sites after coordination assembly.9
We are interested in the design and construction of porous coordination polymers with functional pores for the recognition of energy gas molecules, and identifying a series of water and chemical stable frameworks for expected feasible gas storage and separation.10 Here, continuing our work, we report the syntheses of two new PCPs, ([Cu6(L)4·(H2O)6]·10DMA·4EtOH, (1, the desolvated solid is named as 1′), and [Cu5(L)2(OH)2·(H2O)2·DMA2]·2DMA·EtOH·2H2O (2, the desolvated solid is named as 2′), (H6L = 1,3,5-tris(3-carboxy-4-hydroxylphenyl)benzene), based upon a ligand with an –OH functional group. Interestingly, their variable architectures controlled by solvent system exhibit a structural progression from an unusual NC net to a (4,6)-connected framework with fsh topology. In addition, PCP 2 bearing a suitable pore size, as well as an open –OH site shows high selectivity of CO2 over CH4 (25–55) at 273 K (Scheme 1).
A solvothermal reaction of H6L and Cu(NO3)2·6H2O in DMA/EtOH afforded green crystals of ([Cu6(L)4·(H2O)6]·10DMA·4EtOH. The phase purity of them was confirmed by comparing their experimental powder X-ray diffraction pattern to that calculated based on the single-crystal structures. X-ray diffraction analysis reveals that the L3− ligand in 1 is connected by three copper paddlewheels, and each cluster is bridged by four carboxylate groups from four different ligands, forming a highly symmetrical fan-like sub-structure (Fig. 1). The double layers of fan-like structures share their edges with each other to generate a 1D channel with a diameter of 15.6 Å. In addition, all of the inserted –OH groups are well-aligned inside the channels of 1 (Fig. 1d). For the easy understanding of the connection of this structure, we simply assign the Cu2(ArCOO)4 units as 4-connected nodes, and L3− units as 3-connected linkers. The 3-c nodes come in pairs in which each of them is connected to the same three 4-c nodes. Clearly there is a net automorphism that simply involves interchanging those two vertices, leaving the rest fixed.11 Thus, the generated topology of 1 is an example of a non-crystallographic (NC) net that is different to the another two (3,4)-connected nets of HKUST-1(tbo)12 and MOF-14 (pto).13 This significant change can be explained as being due to the shift of the coordination site from the 4- to 3-position of the benzene ring. The total accessible volume of desolvated 1 is ca. 71.1%, calculated using the PLATON program.14 Additionally, the powder X-ray diffraction (PXRD) pattern showed that the peak positions of the as-synthesized phase are the same as the simulated data, but the peak intensity, especially for the [2 0 0] peak, is different. This is because 1 exhibits a stronger preferential orientation along the [2 0 0] direction.15 Meanwhile, with very good reliability factors (Rp = 0.0252 and Rwp = 0.0553), Le Bail analysis of the PXRD pattern shows that the refined parameters are very close to the data from the single crystal, reflecting good phase purity and also a well-defined structure (Fig. S8†).
[Cu5(L)2(OH)2·(H2O)2·DMA2]·2DMA·EtOH·2H2O (2) was harvested from a DMA/EtOH/H2O solvent system. Interestingly, crystallographic analysis revealed that 2 crystallizes in P space group (Fig. 2). The asymmetric unit of 2 includes one half Cu(II) atom (Cu1) on an inversion centre, two other Cu(II) atoms in general positions, one partially deprotonated L ligand, one –OH group, one coordinated water molecule and one coordinated DMA molecule (Fig. 2a). The coordination numbers of these three copper atoms are 4, 5 and 5, respectively. The coordination geometry of Cu1 is a slightly distorted pentahedron, and is completed by two oxygen atoms from bridged –OH groups, two oxygen atoms from the carboxylate groups, and one coordinated water molecule. Meanwhile, the coordination geometry of Cu2 is completed by one oxygen atom from a bridged –OH group, three oxygen atoms from the carboxylate groups, and one coordinated DMA molecule. Last but not least, a rare and planar coordination square around Cu3 is finished by two phenols oxygen atoms and two carboxylate oxygen atoms. In addition, one ligand is connected by five Cu atoms, forming a porous 3D framework. Thus, a high density of open metal sites can be expected in 2, due to the existence of the original open metal site and also the sites from the removal of coordinated DMA and water. In addition, free –OH groups can also be found inside the channel as shown in Fig. 2d. Compared with the significant channel in 1, the structure of 2 with 3D intercrossed channels of about 3.0 × 7.21, 4.72 × 9.52, and 6.37 × 7.81 Å2 indicates a suitable pore size for CO2 separation (kinetic parameter of CO2: 3.3 Å). The total accessible volume of desolvated 2 is ca. 41.5%, calculated using the PLATON program.14 In addition, after soaking 2 in water for 1 day, the PXRD profiles show the integrity of the framework (Fig. S9†), which is a rare result for carboxylate- and Cu-based PCPs. In order to further understand the connection of 2, the Cu4(ArCOO)4(OH)2 and Cu(ArCOO)2(ArO)2 clusters were simplified as 4- and 2-connected nodes, where the L4− ligands are 4-connected linkers (Fig. 2c). However, it is usual to subsume 2-connected vertices into a link, and then the generated basic unit of 2 can be assigned as a hexatopic carboxylate linker that joins 4-connected nodes. Considering the 4-c branch points of the L4− unit, the framework shows a (4,6)-c net with fsh topology (Fig. 2e).
Interestingly, comparing the synthesis conditions of these two PCPs (changing the solvent systems, while the other conditions were intentionally held constant), we found that the solvent systems induced the changed coordination of the ligand, as well as the structural progression. In order to confirm this point, the following experiments were conducted and the observations from PXRD (Fig S7 and S11†) are detailed in Table 1: (1) when DMA/EtOH (2 mL, 4:
2 ) is used as a solvent system, 1 with phase purity can be obtained at 65 °C, but not at 90 °C and 130 °C; (2) when a very small amount of water was added to the DMA/EtOH system (2 mL, DMA
:
EtOH
:
H2O = 4
:
2
:
0.5), we got purified 2 at 65 °C; (3) when we increased the amount of water in the solvent system from 4
:
2
:
0.5 to 4
:
2
:
2, only 2 could be generated at 65 and 90 °C and (4) when the amount of water increased to a very high level (4
:
2
:
12), no PCPs could be formed at the three temperatures. Thus, different solvent systems regulate the formation of different environments for the assembly of Cu(II) and the linking modes of the H6L ligand. In 1, only the carboxylate groups coordinated to the Cu(II) paddlewheel nodes, whereas, in 2, three different coordination geometries were bridged by the carboxylate groups and also an –OH group from the ligand. Therefore, the ligand can be simplified as three- and four-connected linkers in 1 and 2, respectively. Then, a structural progression from an unusual NC net to a (4,6)-connected framework with fsh topology was well observed (Fig. 3). Herein, more theoretical and experimental efforts are required for finding the role of water in influencing the coordination self-assembly, but we can make a preliminary conclusion: the volumetric ratio of water in a mixed solvent system may influence the solvation process and coordination kinetics in solution. This is maybe due to water being a kind of special ligand that can result in a new balance of the kinetics and thermodynamics of the final product.4,16
Temperature, time and solvent | DMA![]() ![]() ![]() ![]() |
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4![]() ![]() ![]() ![]() |
4![]() ![]() ![]() ![]() |
4![]() ![]() ![]() ![]() |
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|
65 °C, 48 h | 1 | 2 | 2 | × |
90 °C, 48 h | × | × | 2 | × |
130 °C, 48 h | × | × | × | × |
Encouraged by the porous and functional sites in the PCPs, the gas adsorption of them was measured. Before the gas sorption experiments, the activation of these two structures was explored. Unfortunately, desolvated 1′ collapsed, and did not show any gas uptake. Meanwhile, compound 2′ showed a little CO2 gas uptake (25 cm3 g−1) at 1 bar and 195 K. The PXRD pattern of desolvated 2′ indicated structural change after the activation. However, interestingly, 2′ did not show any uptake of O2, CH4, C2H4 and C2H6 (Fig. S14†). Thus, the unique gas adsorption isotherms show the possibility of the selective capture of CO2 by 2′. The adsorption isotherms of CO2 and CH4 in 2′ were collected at 273 K to 9 bar. The maximum uptakes of them reached 1.82 mmol g−1 and 0.35 mmol g−1, respectively. In order to explore the selectivity of 2′, ideal adsorbed solution theory was employed to predict multi-component adsorption behaviors from the experimental pure-gas isotherms. The predicted adsorption selectivity for equimolar CO2/CH4 mixtures in 2′ as a function of bulk pressure is presented in Fig. 4. The selectivity of CO2 over CH4 is very sensitive to loading and shows two steps in the changes of selectivity: a quick decrease of CO2 selectivity in the low pressure region, and a slow increase at high pressure (22–55). This high selectivity can be explained as a result of the good combination of suitable pore size, open metal sites and functionalized –OH groups in 2′. In addition, based on the IAST model and similar conditions, these selectivities are higher than those of the reported adsorbent materials (Zn2(NDC)2(DPNI) (30),17 Zn5(BTA)6(TDA)2 (37),18 Cu-BTC (6–10),19 zeolites 13× (2–24)20 and comparable with the performance of our previously reported amide-functionalized materials of NJU-Bai3 (25–60),10b indicating a selective removal of CO2 from natural gas.
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Fig. 4 High pressure gas adsorption isotherms and the Dual-site Langmuir–Freundlich fit lines of CO2 and CH4 in 2′ at 273 K. The green lines show the IAST predicted selectivity of CO2 over CH4. |
Footnote |
† Electronic supplementary information (ESI) available: Synthesis and characterization of PCPs, PXRD, TGA, IR, and sorption isotherms. CCDC for the two PCPs: 1023464–1023465. For ESI and crystallographic data in CIF or other electronic format. See DOI: 10.1039/c5ce00762c |
This journal is © The Royal Society of Chemistry 2015 |