Stephen Adie
Adalikwu
,
Venkata Suresh
Mothika
,
Arpan
Hazra
and
Tapas Kumar
Maji
*
Molecular Materials Laboratory, Chemistry & Physics of Materials Unit, School of Advanced Materials (SAMat), Jawaharlal Nehru Centre for Advanced Scientific Research, Jakkur, Bangalore-560064, India. E-mail: tmaji@jncasr.ac.in; Web: http://www.jncasr.ac.in/tmaji/
First published on 26th March 2019
A 2D porous MOF, {[Cu(1,2,3-btc)(bpe)(H2O)]·H2O}n (1), has been synthesized using a mixed linker system. The structural determination showed non-coordinated carboxylate groups decorating the pore surface. The desolvated MOF (1a) with pendant carboxylate groups was used as a template for the stabilization of Pd nps (2–3 nm) and the resulting composite Pd(0)@1a showed efficient catalytic activity for the Suzuki–Miyaura C–C coupling reaction.
Compound {[Cu(1,2,3-btc)(bpe)·H2O]·H2O}n, (1) was synthesized using the liquid phase diffusion method at room temperature (see ESI† for details). 1 crystallizes into the triclinic space group P and single crystal X-ray analysis showed that 1 is a 2D coordination network of a Cu(II) bridged by bpe and 1,2,3-btc linkers (Table 1 in the ESI†). The asymmetric unit of 1 contains a five coordinated CuII center with a square pyramidal geometry and it is connected to two bpe, two 1,2,3-btc linkers and one water molecule, resulting in 1 having a 2D square grid-like structure (Fig. 1a). Each CuII center is bridged by two monodentate oxygen (O2 and O3) atoms from the 1 and 3 carboxylate groups of the 1,2,3-btc linkers and forms a 1D {Cu(1,2,3-btc)}n chain, whereas the carboxylic acid group in the 2 position of 1,2,3-btc remains pendent on one side. These 1D chains are linked by the bpe pillars (N1 and N2) along the c- axis resulting in a 2D rectangular grid-like structure along the ac plane (Fig. 1b). The bond distances of Cu1–N1, Cu1–N2, Cu1–O2, Cu1–O3 and Cu1–O1W are 2.006(8), 1.983(7), 1.940(5), 1.955(5) and 2.378(7) Å, respectively (Table 2 in ESI†). It is interesting to note that alternately two successive 1D chains {Cu(1,2,3-btc)}n with one-sided pendent carboxylic acid groups face each other in the 2D rectangular grid. This arrangement provides two different types of coordination spaces in the 2D grid; one oval shaped pore in which two free ‘COOH’ groups are facing each other and a rectangular pore decorated by the –(CH2)2– part of the bpe and benzene rings of the 1,2,3-btc linkers (Fig. 1c). The former pore is hydrophilic in nature and occupied by the guest water molecules, and the later pore is rather hydrophobic. The 2D sheets are packed in an ABCD⋯ABCD (Fig. S1†) manner, which is reinforced by the π⋯π interaction between the bpe pillars and the hydrogen bonding via the coordinated water molecules O1W⋯O4 from a free carboxylate and also through the guest water molecules O4W which connect O1⋯O6 to form a 3D structure. In the network, the CuII⋯CuII separation along the bpe and 1,2,3-btc linking parts are 13.300(2) Å and 10.025(2) Å respectively, and the longest neighboring CuII⋯CuII separation between the 2D sheet is 16.159(2) Å.
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Fig. 1 (a) The asymmetric unit of 1 and (b) its 2D grid like structure. (c) The 3D-framework with water molecules of 1. Red balls indicate guest water molecules. |
To determine the framework stability and phase purity of 1, thermogravimetric analysis (TGA) and X-ray powder diffraction (PXRD) studies were carried out. TGA shows a weight loss of about 6.94% in the temperature range of 87–157 °C, corresponding to the loss of two water molecules (calculated weight loss 7.12%) (Fig. S2†). The desolvated compound 1a is stable up to 190 °C without further weight loss. The PXRD pattern of as-synthesized 1 shows identical peaks corresponding to the simulated pattern indicating the phase purity of the sample (Fig. 2a). Furthermore, diffraction patterns of the dehydrated and rehydrated samples were observed to be similar, suggesting the thermal/hydrolytic stability of the framework (Fig. 2a). To investigate the permanent porosity of 1, the desolvated framework 1a was subjected to gas adsorption studies. The N2 adsorption measurement for 1a at 77 K shows a type-II adsorption profile (Fig. S3†), whereas the CO2 adsorption study at 195 K reveals a gradual uptake up to P = 1 atm (Fig. 2b). Both the sorption profiles suggest a diffusion barrier for the adsorbate molecules owing to the smaller pore size. The final uptake amount for CO2 was found to be ∼50 mL g−1, which corresponds to one molecule of CO2 per formula unit. It is interesting to note that the CO2 profile demonstrates substantial hysteresis in the desorption, representing the strong interaction of CO2 with 1a and this is also reflected in the high value of the isosteric heat of adsorption (qst′Φ found to be 27.66 kJ mol−1) as calculated using Dubinin–Radushkevich (DR) equation.40 This strong interaction could be attributed to the interaction of CO2 with unsaturated Cu(II) sites and the free carboxylic oxygen atoms decorating the pore surface. MOF 1a is non-porous to N2, as evident from the type-II N2 gas adsorption isotherm measured at 77 K. Thus, the standard method for BET surface area calculation using N2 adsorption isotherms was not possible.
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Fig. 2 (a) PXRD patterns of 1: (i) simulated; (ii) as-synthesized; (iii) dehydrated; and (iv) rehydrated. (b) CO2 adsorption isotherm of 1a (red) and Pd(0)@1a (black) at 195 K up to 1 atm. |
The regular and periodic arrangements of square grid-like nanopores with free carboxylic acid groups of 1,2,3-btc makes 1a a potential template for the stabilization of metal nps such as Pd(0) for fabrication of np@MOF composite materials. A schematic representation of the stabilization of Pd(0) nps through the electrostatic interaction of free carboxylic acid groups of 1a is shown in Fig. 3. K2PdCl4 salt was adsorbed into 1a through the solution impregnation method (see ESI† for details) and reduced using NaBH4, resulting in the Pd(0)@1a composite. The transmission electron microscopy (TEM) image of Pd(0)@1a shows a uniform coverage of Pd(0) nps with the size ranging from 2–3 nm (determined using DigitalMicrograph software) throughout the MOF matrix (Fig. 4a and b). The energy-dispersive X-ray analysis (EDAX) of the Pd(0)@1a composite indicates the presence of both Pd(0) and Cu(II) in the composite (Fig. S4†). The PXRD pattern of Pd(0)@1a shows (Fig. 4c) that all of the characteristic peaks of 1a are retained in the composite, suggesting that the framework is intact after the stabilization of Pd(0) nps and also reveals the high stability of 1a in aqueous solutions. The additional peak at 6.8° observed in Pd(0)@1a could be due to a slight rearrangement in the structure. Furthermore, the CO2 adsorption measurements of Pd(0)@1a at 195 K show a lower uptake of CO2 in comparison to 1a, this may be attributed to the filling of some of the pores of 1a with Pd(0) nps thereby reducing the available pores for CO2 adsorption (Fig. 2b). These results clearly indicate that 1a is a robust and efficient scaffold for the stabilization of metal nps. The X-ray photoelectron spectrum (XPS) of Pd(0)@1a shows transitions that correspond to Pd(3d5/2) and Pd(3d3/2) at 339.3 and 344.25 eV, respectively, suggesting the zero-valent oxidation state of Pd(0) nps in Pd(0)@1a (Fig. 4d).39 The diffraction of Pd(0) nps in the composite is observed to be very weak owing to very small size of the nps and the high crystallinity of 1a in comparison (Fig. 4c inset). The loading of Pd(0) nps in the MOF was found to be 3.2 wt%, as determined using inductively coupled plasma-optical emission spectrometry (ICP-OES) investigation. Uniformly distributed Pd(0) nps of sizes 2–3 nm in the Pd(0)@1a composite would be a potential candidate for heterogeneously catalyzed industrially important organic reaction such as the Suzuki–Miyaura C–C coupling.41 Initial experiments were performed with iodobenzene and phenylboronic acid as the aryl halide and aryl boronic acid in the presence of a mild base such as Cs2CO3 (Table 1). In a typical reaction, a mixture of iodobenzene (aryl halide) (0.098 mmol), phenylboronic acid (aryl boronic acid) (0.147 mmol), Cs2CO3 (0.294 mmol), and the Pd(0)@1a catalyst (1.5 mg) were stirred in tetrahydrofuran (THF) at 60 °C for 24 h. The reaction mixture was filtered and washed with water; the filtrate was extracted with dichloromethane, concentrated under reduced pressure and analyzed using gas chromatography-mass spectrometry (GC-MS) and 1H-NMR spectroscopy. Interestingly, the GC-MS revealed almost complete conversion of iodobenzene into biphenyl, no other peaks corresponding to precursors or impurities were observed (Fig. S5 & S6†). Encouraged by the results, further experiments were carried out to investigate the effect of the electronic groups on the aryl halide, keeping the phenylboronic acid constant. All of the reactions were smooth and went to near completion in the case of both the electron withdrawing and electron donating groups, and the results are summarized in Table 1 (Fig. S7–S11†). To determine the importance of Pd(0) nps in the catalytic reaction, we performed blank reactions using 1a under identical conditions. However, no products were observed suggesting the importance of the Pd(0) nps being present over the MOF matrix of 1a for catalyzing the reaction. We have also studied the time dependent progress of the reaction for the formation of biphenyl using the Pd(0)@1a catalyst. As seen in Fig. S12,† a gradual increase in the product formation was observed. To check the leaching of Pd(0) nps into the solution, after the fourth catalytic reaction (24 h) the filtrate was studied using ICP-MS analysis. The ICP data suggest the presence of a very small amount of Pd in the solution (2 ppm), suggesting a very slight leaching of Pd during the catalytic reaction. Apparently, a homogeneous reaction mechanism occurring through the leached Pd(0) nps could contribute in parallel to the dominant Pd(0)@1a assisted heterogeneous catalytic process. Pd(0)@1a was observed to show an excellent conversion of aryl halide to biphenyl with no apparent decrease in the yields for up to four catalytic cycles, suggesting the high recyclability of the catalyst (Fig. S13†). Moreover, no considerable agglomeration of Pd(0) nps was observed, even after four catalytic cycles. As seen in Fig. S14,† the particle size ranges from 2–3 nm, however, very few particles of 5 nm size were observed suggesting that insignificant nps agglomeration occurred during the catalytic reaction. Furthermore, the stability of Pd(0)@1a after four catalytic cycles was studied using PXRD measurements. As seen in Fig. S15,† all of the diffraction peaks that were characteristic of 1a were retained in recycled catalyst with only a slight broadening or change to the intensities suggesting the considerable stability of the framework. These results suggest that 1a acts as an efficient scaffold for the stabilization of Pd(0) nps through the pendant carboxylate oxygen atom with reduced leaching or agglomeration effects, resulting in efficient conversions even after several catalytic cycles.
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Fig. 3 Schematic diagram showing the interaction of the pendent ‘COOH’ groups with the Pd(0) nps in the MOF pore and the stabilization. |
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1881659. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c8dt04766a |
This journal is © The Royal Society of Chemistry 2019 |