Weiwei Xu,
Ai Du*,
Jun Tang,
Peng Yan,
Xiaoguang Li,
Zhihua Zhang,
Jun Shen and
Bin Zhou*
Shanghai Key Laboratory of Special Microstructure Materials and Technology, School of Physics Science and Engineering, Tongji University, Shanghai 200092, P. R. China. E-mail: zhoubin863@.tongji.edu.cn; duai@tongji.edu.cn; Fax: +86-21-65986071; Tel: +86-21-65982762
First published on 10th September 2014
Uniform and highly dispersed Cu- or Cu2O-doped SiO2 aerogels were synthesized via an in situ alcohothermal reduction strategy. The initial templates containing an accurately controllable doping fraction were prepared through a co-gelation method. After alcohothermal reduction and CO2 supercritical drying, a similar morphology of the resulting samples to the initial templates was retained. The entire reducing process was systematically studied through comparative experiments, separately using ethanol, ethylene glycol and glycerol as reducing agents, with the corresponding converted products obtained being cubic Cu2O- and Cu-contained silica composites. The specific surface area of the resulting products ranged from 500 m2 g−1 to 850 m2 g−1. The related microstructure evolution mechanism was comprehensively studied through analysis of the pore-size distribution. The high specific surface area and controlled doping amount make it suitable for possible use in specific applications, such as high efficiency photocatalysis and backlight targets.
In this work, the in situ alcohothermal reduction method was employed to synthesize homogeneous Cu/SiO2 composite aerogels with an accurately controllable doping fraction. The Cu(II)-contained silica gel templates were prepared through a propylene oxide pre-reaction method, with the Cu(II) compound and silica colloidal particles simultaneously cross-linked into the homogeneous binary gel frameworks. Significantly, the mole ratio of Cu to Si could be accurately controlled and could reach as high as 20% via this method. Afterward, the Cu(II)-contained silica gels were directly reduced by the alcohothermal method with a different alcohol as a reducing agent. Finally, Cu- or Cu2O-doped SiO2 aerogels were obtained after supercritical fluid drying. According to our knowledge, to date, there has been no related report about the in situ alcohothermal reduction of metal-based gels in composite networks. In addition, the uniform nanoparticles size and high dispersion of the resulting products not only exhibit a better performance, but also provide a quantitative media to study the mechanism in photocatalysis or ICF backlights.
The propylene oxide pre-reaction method was used to synthesize the Cu(II)-contained silica composite templates according to the following procedure. First, tetramethoxysilane, acetonitrile, deionized water, and propylene oxide with the volume ratio of 1:
1
:
0.018
:
0.63 were mixed together for pre-reaction. The solution was then poured into another mixture of CuCl2·2H2O (2.264 g), acetonitrile (20 ml), and water (1.972 ml). Following mixing, propylene oxide (3 ml) was added into the mixed solution, and stirred for several minutes. Finally, homogeneous dark-green gels were obtained after sufficient hydrolysis and condensation of the precursors within 30 min at 35 °C. The wet gels were aged for at least 48 h and then sealed together with 35 ml of reducing agent in a Teflon-lined stainless-steel autoclave (50 ml). The autoclave was heated to 200 °C, at a rate of 1 °C min−1, dwelling there for 10 h and undergoing natural cooling. The resulting products were washed with ethanol several times, and then dried with CO2 supercritical drying. In order to systematically study the whole reducing process, ethanol, ethylene glycol, and glycerol were separately used as reducing agents. In this paper, the initial aerogel templates and corresponding products reduced by ethanol, ethylene glycol, and glycerol were marked as AG-1, AG-2, AG-3, and AG-3, respectively.
The surface morphologies of the samples were examined by a scanning electron microscope (SEM, Philips-XL30), which was additionally equipped with an energy dispersive X-ray spectrometer (EDS). A high-resolution transmission electron microscope (TEM, JEOL JEM-2010) was used to characterize the microstructure. The components and crystal structure of the resulting products were detected by X-ray diffraction (XRD, Rigaku D/Max-RB). The specific surface area and pore structure parameters of the aerogels were obtained from nitrogen sorption isotherms tested at 77 K, using a Quantachrome Autosorb-1 analyzer. The Brunauer–Emmett–Teller (BET) and Barrett–Joyner–Halenda (BJH) methods were used, respectively, to calculate the specific surface area and pore size distribution.
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Scheme 1 Schematic of the formation of Cu(II)-contained silica gels and the subsequent alcohothermal reduction process. |
As shown in the following equation, a similar ring-opening addition reaction of the propylene oxide was conducted in different precursor solutions. In this reaction, PO acts as an irreversible proton capture agent, and two products are generated with similar chemistry structural formulas.
![]() | (1) |
In the TMOS system, H+ was the hydrolysis product of TMOS, and was then combined with the oxygen atom on the epoxy group. Due to the instability of the hydroxylating carbon–oxygen ring, the ring-opening reaction and the subsequent nucleophilic addition process of the methoxyl group easily occurred, which partly accelerated formation of the silica gel network.29 It is notable that the hydrolysis product, –OCH3, exhibited weak electronegativity and that as the solution was in an acidic environment, the ring-opening addition reaction tended to take place first, with the alkoxyalcohol product mainly being the second item.30,31 When the two solutions were mixed together, there was a similar reaction on PO and hydrogen halide, which were produced by the hydrolysis of [Cu(H2O)n(OH)x−n]2+. However, the strong electronegativity of the chloride ion made the major reaction tend to generate the chloroalcohol product with the first form of the structural formula, as shown in eqn (1).32 A homogeneous and coherently supported binary gel with randomly interconnected networks was obtained through the co-gelation process previously mentioned.
![]() | (2) |
As shown in Fig. 1, a macroscopic difference in the resulting products is apparent. From the left to right, the samples with separate densities of 230 mg cm−3, 340 mg cm−3, 263.6 mg cm−3, and 237.7 mg cm−3 are, respectively, the initial aerogels (blue, AG-1) and the corresponding reducing products of ethanol (yellow, AG-2), ethylene glycol (dark red, AG-3), and glycerol (brick red, AG-4), based on the solvothermal method. Distinctly, the gels had different shrinkages during the whole process, which could be explained as follows. On the one hand, the Cu(II) component can recombine under high-temperature and high-pressure conditions. On the other hand, damage by the capillary forces to the porous structure was unavoidable during the drying process. In addition, the reaction between the Cu(II) particles and the alcohol reducing agent is a complex process. Whether the monolithic structure could be reserved is mainly determined by the tolerance of the silica frameworks to the alcohothermal process.
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Fig. 1 Photographs of the samples: (a) Cu(II)-contained silica composite gels (left image) and different reduction products; (b) the corresponding aerogels after CO2 drying. |
In order to analyze the crystal phase composition of Cu(II)-contained silica composites and the converted products, X-ray diffraction (XRD) patterns were obtained, as shown in Fig. 2. The initial composite aerogels (Fig. 2a) exhibited a broad diffraction peak around 22°, which was associated with amorphous silica and which appeared in subsequent diffraction curves (Fig. 2b–d). After ethanol-thermal reduction, obvious diffraction peaks (Fig. 2b) at 2θ values of 29.6°, 36.5°, 42.3°, 61.5°, and 73.4° were present as the cubic Cu2O phase (PDF#075-4299). When ethylene glycol and glycerol were used as reducing agents, similar diffraction peaks appeared at 43.3°, 50.4°, and 74.1° and were indexed as the (111), (200), and (220) diffraction of cubic Cu (PDF#04-0836). By contrast, the peak intensity in Fig. 2d is stronger than that in Fig. 2c, which reveals that the copper nanoparticles in the glycerol system exhibit a higher crystalline structure than that of ethylene glycol under the same conditions. In addition, the average crystal grain size was estimated from the XRD patterns by using Jade software with the Scherrer equation,35 and the related values were 9.9 nm (Fig. 2c) and 22.4 nm (Fig. 2d) respectively, which are consistent with the TEM results.
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Fig. 2 XRD patterns of composite aerogels: (a) Cu(II)-contained silica composites, and related products with different reducing agents: (b) ethanol, (c) ethylene glycol, (d) glycerol. |
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Fig. 3 The SEM images of the resulting aerogels: (a) Cu(II)-contained silica composites; (b) after ethanol reduction; (c) after ethylene glycol reduction; and (d) after glycerol reduction. |
Specimen | Bulk density (mg cm−3) | BET (m2 g−1) | Average pore size (nm) | Grain size (nm) | Doping fraction |
---|---|---|---|---|---|
AG-1 | 230 | 631 | 17.5 | — | 19.91% |
AG-2 | 340 | 846.4 | 10.4 | 8.6 | 18.6% |
AG-3 | 263.6 | 722.1 | 23.09 | 9.9 | 17.8% |
AG-4 | 237.7 | 531.2 | 19.42 | 22.4 | 13.8% |
The microstructures of various aerogels were characterized using transmission electron microscopy (TEM). These nanocomposites clearly displayed the typical microstructure of common aerogels, i.e., that of nanoparticles clustered together to form a mesoporous structure. As shown in Fig. 4a, the initial aerogels are mainly composed of small spherical particles with a diameter of about 1–10 nm, and both the components are uniformly dispersed without any obvious aggregation of colloidal particles. However, after ethanol-thermal reduction, the shape of the skeleton is similar to that of the randomly distributed root, and some Cu2O submicron particles are detected in the networks, as shown in Fig. 4b. This could be explained by the nucleation and growth of Cu2O nanocrystal particles being easily realized under high-temperature and high-pressure conditions. In contrast, Fig. 4c and d demonstrate that the Cu nanocrystal particles are uniformly dispersed in the networks, and that there is no clear aggregation in the primary structure. During the reaction process, the framework of the Cu(II) component was gradually consumed under reducing conditions, and the corresponding copper nanoparticles with a weak interaction were simultaneously obtained. Interestingly, the copper colloidal particles reduced by glycerol have a larger grain size than those reduced by ethylene glycol, which reveals that glycerol has a stronger reducibility compared with ethylene glycol.36,37
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Fig. 4 TEM images of (a) Cu(II)-contained silica composite aerogels and the corresponding products with different reducing agents: (b) ethanol, (c) ethylene glycol, and (d) glycerol. |
Nitrogen adsorption/desorption isotherms of the resulting samples were obtained by the Brunauer–Emmett–Teller (BET) method. As described in Fig. S1,† the initial aerogels and corresponding samples reduced by ethanol, ethylene glycol, and glycerol exhibited similar typical IV isotherms and narrow H1-type hysteresis loops, which are consistent with the mesoporous structure. The specific surface areas were 631.1 m2 g−1, 846.4 m2 g−1, 722.1 m2 g−1, and 531.2 m2 g−1, respectively. In addition, Fig. 5a shows the corresponding cumulative pore volumes and size distribution as that calculated from the desorption branch of the isotherm applying the BJH theory. The initial Cu(II)-contained silica aerogels exhibited a broad pore size distribution, mainly in the mesopore range (10–50 nm), which represents the typical characterization of most mesoporous aerogel materials. After the ethanol-thermal process, some micropores (≤2 nm) that give rise to the surface area appeared.38 Meanwhile, the main-peak value of the mesopore transformed from 35.82 nm down to 17.75 nm, compared with the AG-1 sample. The change of pore size distribution could be reasonably explained by two factor: (1) the generated micropores were mostly attributed to the in situ pore-fabrication during the conversion process from the Cu(II) to the Cu2O component; (2) the shift of the main-peak position was mainly caused by the obvious shrinkage of the obtained wet gels during the supercritical drying caused by the unavoidable capillary forces, which could be visibly certified from the related photographs of the ethanol-reduced wet gels and the final aerogels in Fig. 1. As for sample AG-3, a similar pore-size distribution to the initial ones is shown in Fig. 5a. The main peak was still at about 35 nm, while an additional sub-peak at 24 nm appeared after the ethylene glycol-thermal reduction. Interestingly, we found that the pore-size distribution of the AG-4 sample exhibited a narrower distribution, and the peak value dropped down to 24.6 nm, which was approximately the same as the sub-peak of AG-3. In regards the as-described change of pore-size distribution, this could be explained by the reaction mildly taking place when ethylene glycol was used as a reducing agent, and the colloidal frameworks then essentially underwent internal stress, so that the reduced sample exhibited a similar pore-size distribution as that of the initial templates. As for the generation of some small mesopores, except for the inevitable bulk shrinkage during CO2 supercritical drying, this is mostly attributed to the filling and further fusion effects of the converted copper nanoparticles, whereby the initial pores were partly filled with the primary copper nanoparticles, which then gradually fused into larger sized ones. In contrast, the glycol provided stronger reducing conditions for the initial templates, and the reduced copper nanocrystal particles in the existing mesopores were then easily aggregated into larger ones. More importantly, the colloidal skeletons could barely tolerate the internal stress caused by the reaction between the Cu(II) compound and glycerol, with the consequence that the composite frameworks partly shrunk, and even collapsed to varying degrees, following the mechanism described in Fig. 5b. Consequently, this reaction condition might not only result in macroscopic shrinkage of the bulk, but could also lead to a decrease in the specific surface area.
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Fig. 5 The distribution and formation mechanism of the hierarchical pores of the resulting composite aerogels. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra06633b |
This journal is © The Royal Society of Chemistry 2014 |