Yu Yinab,
Jing Zhua,
Xiao-Qin Liu*a,
Peng Tana,
Ding-Ming Xuea,
Zhi-Min Xinga and
Lin-Bing Sun*a
aState Key Laboratory of Materials-Oriented Chemical Engineering, College of Chemistry and Chemical Engineering, Nanjing Tech University, Nanjing 210009, China. E-mail: liuxq@njtech.edu.cn; lbsun@njtech.edu.cn
bSchool of Environmental and Chemical Engineering, Jiangsu University of Science and Technology, Zhenjiang 212003, China
First published on 15th July 2016
Fabrication of bifunctional Cu(I)/Ce(IV) sites in mesoporous silica SBA-15 requires a series of complicated steps, including introduction of the Ce(III) precursor, calcination to generate Ce(IV), further introduction of the Cu(II) precursor, and repeated calcination to generate Cu(I). This traditional method has low efficiency and wastes energy. Here we provide a highly efficient, convenient and green strategy for the fabrication of bifunctional Cu(I)/Ce(IV) sites in mesoporous silica SBA-15, for the first time. The precursors CuCl2 and CeCl3 were simultaneously introduced into SBA-15. Based on a guests-redox strategy, both the reduction of CuCl2 to CuCl and the oxidation of CeCl3 to CeO2 could be realized in one calcination step. This strategy avoids the repeated modification process, and guarantees a high Cu(I) yield of ∼59% without generation of toxic gas. In addition, the resultant materials show excellent performance in gas separation of C2H4 from C2H6.
It is reported that Ce(IV) sites can disperse into various geometric positions and utilize the surface of the support effectively.11–13 Moreover, Ce(IV) may be beneficial to the stability and degree of dispersion of the active metal sites. As a result, Ce(IV) sites are widely used as assistant agents in bifunctional materials.14,15 In general, Ce(III) salts used as precursors are first introduced into the support and calcined, leading to the generation of a host with modified Ce(IV) sites. Another metallic precursor such as a Cu(II) salt is then introduced, followed by the second calcination to generate Cu(I) sites. Evidently, this traditional approach to the fabrication of bifunctional Cu(I)/Ce(IV) sites on the support is rather complicated. Therefore, it is highly desirable to develop a facile approach to generate bifunctional Cu(I)/Ce(IV) sites on the support.
Herein we report for the first time a strategy for simultaneously constructing bifunctional Cu(I)/Ce(IV) sites on SBA-15 mesoporous silica by using a guests-redox interaction (Scheme 1). The precursors, both CuCl2 and CeCl3, were introduced into SBA-15 in a solid-state grinding step, followed by calcination at 350 °C under argon atmosphere. Thus, a bifunctional material, named Cu–Ce/SBA-15, was obtained. During the calcination process, CeCl3 worked as a reducing agent and was oxidized to CeO2. Meanwhile, CuCl2 worked as an oxidant and was reduced to CuCl. Besides the Cu and Ce species, the other elements in the samples are unable to take part in the redox reaction. In particular, the Si element derived from the support has no redox capability. This strategy allows the modification of SBA-15 with bifunctional Cu(I)/Ce(IV) sites in one step, which avoids repeated calcination. More importantly, the Cu(I) yield is as high as ∼59% without any harmful Cl2 generated. The present strategy offers an efficient, energy-saving and green way to fabricate supported Cu(I)/Ce(IV) sites on SBA-15. We also demonstrate that the bifunctional materials exhibit excellent performance in the gas separation of C2H4 from C2H6. Both the capacity and the selectivity are superior to the performance of materials modified with only Cu(I) sites.
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Scheme 1 Promoting the conversion yield of CuCl2 to CuCl from ∼15% to ∼59% in silica nanopores using the guests-redox strategy. |
The N2 adsorption–desorption isotherms were measured using an ASAP 2020 system at −196 °C. Prior to analysis, the samples were evacuated at 150 °C for 4 h. The Brunauer–Emmett–Teller (BET) surface area was calculated as the relative pressure ranged from 0.04 to 0.20. The total pore volume was derived from the amount adsorbed at the relative pressure of about 0.99. The pore size distributions were calculated by the Barrett–Joyner–Halenda (BJH) method according to the adsorption branches.
X-ray photoelectron spectroscopy (XPS) analysis was conducted on a Physical Electronic PHI-550 spectrometer equipped with an Al Kα X-ray source (hν = 1486.6 eV) and was operated at 10 kV and 35 mA.
TG analysis was performed in an argon flow from room temperature to 800 °C on a thermobalance (STA-490C, NETZSCH).
Excluding 8Cu–8Ce/SBA-15, the N2 sorption isotherms of the samples are clearly classified as type IV, with an H1 hysteresis loop, which are characteristic of materials with cylindrical mesopores (Fig. 2A). Fig. 2B shows the pore size distributions of the samples. The corresponding surface areas, pore volumes and pore diameters are shown in Table 1. The pore diameter of SBA-15 is 9.2 nm. With the introduction of bifunctional sites, the pore diameters increase slightly to 9.9 nm, then return to 9.2 nm with the increase of the Cu/Ce content. For the samples of 4Cu/SBA-15 and 4Ce/SBA-15, the pore diameters are 8.4 nm. In addition, for the bifunctional samples, the surface areas and pore volumes decrease gradually, from 500 to 142 m2 g−1 and from 0.891 to 0.259 cm3 g−1, respectively, with the increase of the Cu/Ce content. The surface area is 360 m2 g−1 for the sample of 4Cu/SBA-15, and 250 m2 g−1 for the sample of 4Ce/SBA-15. The pore volume is 0.625 cm3 g−1 for the sample of 4Cu/SBA-15, and 0.415 cm3 g−1 for the sample of 4Ce/SBA-15. It is seen that the introduction of metal sites does not destroy the pore characteristics of SBA-15, except for 8Cu–8Ce/SBA-15. The slight changes in the pore characteristics indicate the successful introduction of metal sites.
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Fig. 2 (A) N2 adsorption–desorption isotherms and (B) pore size distributions of SBA-15 and modified samples. |
Sample | SBET (m2 g−1) | Vp (cm3 g−1) | Dp (nm) |
---|---|---|---|
SBA-15 | 658 | 1.093 | 9.2 |
1Cu–1Ce/SBA-15 | 500 | 0.891 | 9.9 |
2Cu–2Ce/SBA-15 | 456 | 0.760 | 9.9 |
4Cu–4Ce/SBA-15 | 310 | 0.523 | 9.9 |
8Cu–8Ce/SBA-15 | 142 | 0.259 | 9.2 |
4Cu/SBA-15 | 360 | 0.625 | 8.4 |
4Ce/SBA-15 | 250 | 0.415 | 8.4 |
For the sample of 4Cu–4Ce/SBA-15, periodic mesopores with uniform pore size and wall thickness can be deduced from the white-dark contrast of the TEM image (Fig. S1†). This also confirms that the ordered structure of mesoporous silica is well preserved after the introduction of bimetal sites. Fig. S2 and S3† show the SEM image and EDX spectrum of the sample 4Cu–4Ce/SBA-15. As shown in the EDX spectrum, Cu and Ce elements are both present in the silica nanopores. Further, judging from the elemental mapping images, Ce and Cu elements are well dispersed throughout the silica nanopores.
The wide-angle XRD patterns of all the samples are presented in Fig. 1B. There are peaks at 28.1°, 33.1°, 47.5° and 56.5° derived from CeO2 (JCPDS no. 34-0394) appearing for the sample 4Ce/SBA-15. For the sample 4Cu/SBA-15, the peaks at 28.4°, 33.1°, 47.5° and 56.5° are features of CuCl (JCPDS no. 18-0439), and the peaks at 32.4° and 39.6° are characteristic of CuCl2·3Cu(OH)2 (JCPDS no. 34-0394). This indicates that a large amount of Cu(II) sites have not been successfully reduced. When it comes to the bifunctional sample 4Cu–4Ce/SBA-15, the patterns are completely different. Crystalline phases of CeO2 and CuCl with the same peak positions coexist. In addition, there is no peak characteristic of Cu(II) sites. This implies that, with the help of the reducing agent, the reduction process from Cu(II) to Cu(I) sites was carried out more thoroughly. In addition, the metal content has an important effect on the guests-redox strategy. For the sample 8Cu–8Ce/SBA-15, a series of disordered peaks emerged. The patterns of samples that were simply ground, without any thermal treatment, are shown in Fig. S4† for reference. It was found that the disordered peaks that resulted from the CuCl2·2H2O and CeCl3·6H2O precursors decomposed incompletely.
The valence states of Cu species in 4Cu/SBA-15 and 4Cu–4Ce/SBA-15 were further investigated by X-ray photoelectron spectroscopy (XPS). Fig. S6† depicts the regions of the Cu high-resolution spectra. The wide peaks ranging from 930 eV to 938 eV are ascribed to Cu 2p3/2. The accompanying satellite peaks ranging from 940 to 950 eV are characteristic of Cu 2p1/2. The existence of satellite peaks indicates that the samples probably contain Cu(II) species. Further analysis of the peaks of Cu 2p2/3 was conducted. As shown in Fig. 3A and B, the results obtained from curve-fitting present two peaks at 932.9 eV and 935.1 eV, which can be respectively ascribed to Cu 2p3/2+ and Cu 2p3/22+.18–21 According to further integral calculations, the Cu(I) yield is 15% for the sample 4Cu/SBA-15 (Table 2), and 59% for the sample 4Cu–4Ce/SBA-15. In order to confirm these vital results, titration experiments were also carried out to measure the Cu(I) yield. The Cu(I) yield is 14% for the sample 4Cu/SBA-15, and 56% for the sample 4Cu–4Ce/SBA-15. It is evident that the results derived from titration correlate well with those from XPS. It is noteworthy that by use of the guests-redox strategy, the Cu(I) yield is dramatically promoted from ∼15% to ∼59%. In addition, the valence states of the Ce species were also measured, and the results are shown in Fig. S5.† As depicted, the Ce(IV) yield is 61% (Table 2) for the sample 4Cu–4Ce/SBA-15, which is close to the Cu(I) yield. This coincidence implies that the guests-redox strategy results in reactions with the same molar ratio.
Sample | Amount of Cua (mmol g−1) | Cu(I) contentb (%) | Amount of Cee (mmol g−1) | Ce(IV) contentf (%) from XPS | |
---|---|---|---|---|---|
From titrationc | From XPSd | ||||
a Amount of Cu introduced per gram of SBA-15.b Calculated from the equation of Cu(I)/[Cu(I) + Cu(II)].c Determined by titration.d Calculated from the XPS results.e Amount of Ce introduced per gram of SBA-15.f Calculated from the XPS results. | |||||
4Cu/SBA-15 | 4 | 14% | 15% | 0 | — |
4Ce/SBA-15 | 0 | — | — | 4 | — |
1Cu–1Ce/SBA-15 | 1 | 53% | — | 1 | — |
2Cu–2Ce/SBA-15 | 2 | 53% | — | 2 | — |
4Cu–4Ce/SBA-15 | 4 | 56% | 59% | 4 | 61% |
8Cu–8Ce/SBA-15 | 8 | 42% | — | 8 | — |
2CuCl2 → 2CuCl + Cl2 | (1) |
The weight loss due to CuCl2 reduction continues from 270 °C to 650 °C. A similar process for CuCl2·2H2O decomposition has been reported before.8 A distinct process is also observed for the conversion of CeCl3·6H2O in the sample Ce/SBA-15. During the thermal treatment, the existence of crystalline or adsorbed hydrates should give rise to hydrolysis reactions, which leads to the formation of cerium oxides.28 As described above, the decomposition of CeCl3·6H2O starts with the hydrolysis reaction, then generates CeO2 from 120 °C to 600 °C. In contrast to the samples above, the bifunctional material 4Cu–4Ce/SBA-15 shows a quite different conversion route. A simultaneous weight loss attributed to the conversion of CuCl2 to CuCl, and CeCl3 to CeO2, can be observed between 120 °C and 700 °C. According to the XPS results, CuCl2 and CeCl3 react in the same molar ratio, and the byproduct is probably HCl as shown in eqn (2).
CuCl2 + CeCl3 + 2H2O → CeO2 + CuCl + 4HCl | (2) |
It is interesting to note that the conversion of CuCl2 to CuCl, and CeCl3 to CeO2, could be carried out in one calcination step, and HCl becomes the gaseous byproduct; no longer is any toxic Cl2 generated.
To further verify the feasibility of the guests-redox strategy, the free energy change of eqn (2) was calculated. As shown in eqn (S9),† the free energy change for the process at 623.15 K and 101.325 kPa is below zero. This proves that the process can occur. However, the free energy change for the process under standard conditions of 273.15 K and 101.325 kPa is over zero (eqn (S10)†). This indicates that the process is a thermodynamically disfavored reaction, and could never occur at standard conditions.
Since this is so, what could be responsible for the enhanced C2H4/C2H6 selectivity of our materials? π complexation adsorption is described as one of the most promising methods to separate C2H4/C2H6 with high selectivity. It is reported that Cu(I) sites can form the π complexation force with the CC bond in C2H4. In contrast, the bond energy between Cu(I) and C2H6 arises from the van der Waals force. The π complexation force is evidently stronger than the van der Waals force. Based on such a mechanism, C2H4 could be preferentially adsorbed on the Cu(I) sites. Thus, studies have been devoted to the optimization of the π complexation adsorption. Dispersion of Cu(I) on mesoporous silica has been identified as an efficient method. Although mesoporous silica can only form the van der Waals force with C2H4 and C2H6, the large surface areas generated by the pores of mesoporous silica could be used to disperse the Cu(I) sites. Dispersed Cu(I) sites can come into contact with more C2H4 molecules than aggregated sites. In the present work, it is clear that the predominant sites responsible for C2H4/C2H6 separation are accessible Cu(I) species. The main function of the pore characteristics of the mesoporous silica SBA-15 is to make the Cu(I) species more accessible on the surface. It therefore follows that, on a support of mesoporous silica SBA-15, the more Cu(I) species are present, the better the separation performance. From this detailed analysis of the present work, we conclude that the C2H4/C2H6 selectivity is mainly dependent on the precise content of Cu(I) in SBA-15.
Footnote |
† Electronic supplementary information (ESI) available: Experimental section, supplementary results. See DOI: 10.1039/c6ra14091b |
This journal is © The Royal Society of Chemistry 2016 |