Shuaiyu
Jiang‡
a,
Xiaodan
Yang‡
a,
Jun
Chen
a,
Xianran
Xing
a,
Lianzhou
Wang
b and
Ranbo
Yu
*ab
aDepartment of Physical Chemistry, University of Science and Technology Beijing, Beijing 100083, PR China
bNanomaterials Centre, School of Chemical Engineering and AIBN, The University of Queensland, St. Lucia, Brisbane, QLD 4072, Australia. E-mail: ranboyu@ustb.edu.cn; Fax: +86-10-62332525; Tel: +86-10-62332525
First published on 27th October 2015
Macro/nano-composite CeO2 spheres with variable diameters of 30–300 μm assembled from nanoparticles of 5–8 nm were synthesized through the calcination of the well assembled spherical Ce(COOH)3 precursor. The controlled hydrolysis of DMF is the key factor for both the crystallization of Ce(COOH)3 and the formation of its macrospheres. These hierarchical CeO2 macrospheres possess pretty high specific surface areas of up to ∼190 m2 g−1 and show an excellent ability to remove Cr(VI) from aqueous solution. Moreover, when substituted with Bi(III), the oxygen storage capacity (OSC) of these CeO2 spheres could be improved sharply to 3243.75 μmol [O] g−1. With an easy-to-manipulate macroscale spherical morphology, these materials are easily recycled. This synthesis opens a promising route for high performance metal oxides.
CeO2 possesses remarkable properties due to its abundant oxygen vacancy defects, high oxygen storage capacity and ability to relatively easily shuttle between III and IV oxidation states. It has been extensively studied and employed in many applications, such as an active component of three-way catalysts (TWCs),10–12 photocatalysts for water oxidation,13 oxygen ion conductors in solid oxide fuel cells,14–16 and ultraviolet (UV) blocking materials in UV shielding.17 Because of the improvement in the redox properties, the specific surface area to volume ratio, and transport properties with respect to condensed bulk materials, nanostructured and porous CeO2 or CeO2-based compounds have attracted special attention.18–28 Recently, various nano-sized CeO2 compounds have been obtained. However, improvement of the surface area was not obvious. On the other hand, synthesis of mesoporous CeO2 could give a surface area up to 200 m2 g−1,21 but the random product morphology was not desirable for further applications. To build up hierarchical 3D nanostructures would be a promising route to CeO2 with larger specific surface areas and desirable morphologies. Mesoporous CeO2 microspheres with uniform flower-like morphologies were synthesized by using glucose and acrylamide as templates, but their surface area is only 92.2 m2 g−1.27 We explored new routes to build 3D multi-shell hollow structures.13,28 Although these structures show good performance as catalysts, their lower specific surface area of ∼95 m2 g−1 is still not desirable. Therefore a facile route for the growth of CeO2 with both high surface area and uniform morphology is still in need.
In this work, an in situ structure directing formation strategy is adopted in the synthesis of hierarchically macrospherical Ce(COOH)3 precursors by controlling the hydrolysis of DMF. The macrospherical Ce(COOH)3 precursors could be easily transformed into perfect CeO2 macrospheres upon calcination. The obtained CeO2 macrospheres possessed a high surface area and showed an excellent ability to remove Cr(VI) from aqueous solution. Moreover, when doped with Bi(III), the oxygen storage capacity (OSC) of the CeO2 increased significantly with no obvious decrease of the surface area.
The OSC measurements were carried out at 500 °C. The measurements were carried out in a flow reactor system equipped with Solenoid valves for rapid introduction of (4%)CO + (1%)Ar + He or (2%)O2 + (1%)Ar + He pluses. Typically, 30 mg powders were loaded into a 1.0 cm id. quartz tube reactor and a total gas flow rate of 300 cm3 min−1 was employed. The signals of the outlet gas were detected by using an on-line quadrupole mass spectrometer (Omnistar 200). Prior to CO step measurements, the sample was heated in (2%)O2 + (1%)Ar + He at 773 K for at least 20 min. The sample was further purged in pure He for 30 min to remove oxygen from the system and then exposed to (4%)CO + (1%)Ar + He. The accumulated amount of CO2 per gram of catalyst was monitored as a function of time.
The morphology and structure of the precursors and final products were characterized by using the field emission scanning electron microscope (FE-SEM) and the high-resolution transmission electron microscope (HRTEM). It can be observed that by adjusting the hydrothermal synthesis conditions, general and hollow macrospheres of the precursor and the CeO2 could be obtained. Fig. 2a shows most of the as-synthesized Ce(COOH)3 precursor possesses a uniform spherical morphology with the average size of 300 μm, upon calcination at 350 °C these Ce(COOH)3 transformed into CeO2 spheres without any obvious shrinkage or destruction of the spherical morphologies (Fig. 2b). From the HRTEM image it can be seen that these CeO2 macrospheres are composed of many crystalline CeO2 nanoparticles with an average diameter of 5–8 nm. The hollow CeO2 macrospheres could also be obtained by calcining the as-prepared Ce(COOH)3 hollow macrospheres (Fig. 2c and d).
In this synthesis, DMF plays a crucial role in the formation of the microspheres. In the acid system, DMF might hydrolyze into formic acid and dimethylamine as follows:
(1) |
The formic acid would react with cerium sources to form Ce(COOH)3, and dimethylamine might act as the structure-directing agent to help the microsphere assembly. To determine the detailed effect of DMF, the following comparison processes have been tested. When formic acid was used instead of DMF, under the same reaction conditions, only a cluster of cerium formate just like Irish diamond could be obtained. And when formic acid and dimethylamine were used together, microrods of cerium formate with rough-and-tumble diameters could be synthesized but no macrosphere assembly could be observed (Fig. S3†). Obviously, both the hydrolysis process and products of DMF are dominant for the formation of Ce(COOH)3 macrospheres. Apparently, to realize the morphology control of the Ce(COOH)3 precursor it is necessary to control the hydrolysis rate of DMF. Because acid will enhance the hydrolysis of DMF, acetic acid and ethanol were used as the solvents, respectively. Under different hydrolysis rates of DMF, the formation of hollow and general hierarchical Ce(COOH)3 macrospheres was achieved, respectively (Fig. 2).
To gain insight into the formation process of cerium formate macrospheres, time-dependent experiments were performed. Products were collected at different stages from the reaction mixture once the precipitate had begun to appear in solution, and their morphologies were subjected to FE-SEM investigation. However, for the general Ce(COOH)3 macrospheres, it is difficult to capture the product images at different reaction stages, because the formation of the macrospheres is too fast after the Ce(COOH)3 nucleation. For the hollow Ce(COOH)3 macrospheres, the first sample was taken immediately after the formation of precipitate when reacted for 90 min, and the powder comprised broom-like microrods (Fig. S4a†). In this phase, the cerium formate formed a pyramid first, and then the top end was split into nanorods (Fig. S4a†). After 15 min, the nanorods with diameters of about 40 nm and lengths up to 6 μm began to self-assemble into microspheres. Although the nanorods grew thicker, the diameter of the microspheres remained constant. Hollow microspheres formed over the following 1.5 h (Fig. S4b†), which grew evidently bigger after 6 hours. From these four obvious morphology evolutionary stages a possible formation process is proposed as shown in Fig. 3. At first, the hydrolysis of the DMF led to the nucleation of Ce(COOH)3, which further grew into one-dimensional nanorods. With the increase of reaction time the concentration of organic amine increased, which would probably result in the increase of surface energy of the Ce(COOH)3 nanorods. To decrease the surface energy the bundles formed after treatment for 1.5 h. These bundles gradually organized into microspheres when the reaction time was extended to 3 h, which is possibly related to the structure-directing effect of the organic amine. Through the association with carboxylic acid and amino groups, hydrogen bonding patterns may direct the structure formation in the solution, generating specific supramolecular crystal architectures held together by networks of H-bonds.30,31 At the end of the reaction (12 h), a hollow macrosphere was observed. The N2 adsorption–desorption isotherms of Ce(COOH)3 and CeO2 macrospheres are given in the ESI(Fig. S5–8†), respectively. These isotherms lie between type-I and type-IV. The pore size distribution curves are shown in the inset to their own adsorption–desorption isotherm figures. The average pore diameters are shown in the ESI.† The distribution of the pore diameters is multistage. After calcination, the pore size distribution becomes wider. The BET surface areas of CeO2 macrospheres and hollow macrospheres calculated from these isotherms are 185.1 m2 g−1 and 154.7 m2 g−1, respectively.
Clean water, free of toxic chemicals and pathogens, is vital to the world's health, and is also a critical feedstock in a variety of key industries. Some nanostructured metal oxides showed higher capacities for toxic ions and organic pollutant removal from water than bulk materials.32–34 Moreover, as the size of these oxides was several to hundred micrometers, the solid/liquid separation would be fairly easy. With the high specific surface area and hierarchical porous structure, the capacity for Cr(VI) removal from aqueous solutions of the as-synthesized CeO2 macrospheres was investigated. Chromium is considered as one of the primary highly toxic pollutants in water resources and its efficient removal from water is of great importance. Fig. S9† shows that when 0.05 g of the as-obtained CeO2 was added to 25 mL of chromium solution with an initial concentration of 21.00 mg L−1 and adjusted to pH = 3 at room temperature (20 °C), the adsorption capacity was measured as 7.9 mg Cr g−1, and the adsorption rate could reach 80%, especially, when the initial concentration of the chromium solution is 10 mg L−1, the adsorption rate could achieve 97%. The Cr removal ability of the hierarchical CeO2 macrospheres is much higher than that (adsorption rate: 65%) of the 3D flower-like CeO2 micro/nanocomposite structures.33
The total oxygen storage capacity (OSC) can express the maximum OSC and contains information on the overall reducibility of the solid. The OSC values of the as-synthesized CeO2 macrospheres and hollow macrospheres were measured as 1471.43 and 1168.75 μmol [O] g−1, respectively. For comparison, the OSC of the commercial cerium oxides with a particle size of about 50 nm and the BET specific surface area of 24.97 m2 g−1 has also been measured, and the corresponding OSC value of 611.61 μmol [O] g−1 was obtained, which is much lower than that of the as-synthesized CeO2 macrospheres. The possible reason is the higher surface area of the as-synthesized CeO2 macrospheres enhanced the oxygen storage capacity.
It is reported that when CeO2 is doped with Bi(III), the OSC can be improved, due to the increase of the surface oxygen vacancies.35 So in this work, further research studies on Bi(III) doped CeO2 macrospheres are also explored. The XRD pattern of Bi/CeO2 macrospheres (Fig. 4a) indicates the face-centered cubic phase of CeO2 has been maintained. The BET specific surface area of Bi/CeO2 could reach 192.7 m2 g−1 (Fig. S10†). EDX analysis (Fig. S11 and Table S1†) shows that the amount of Bi(III) is 4% (atom%). The FE-SEM image (Fig. 4b) shows the Bi/CeO2 macrospheres are uniform and in good distribution. There is no obvious change in the spherical morphologies after Bi(III) was doped. In the Raman spectra (Fig. 4c), a peak shift and a shoulder at around 490 cm−1 can be observed after Bi(III) was doped. These proved that the Bi(III) might be incorporated into the structure of CeO2. The OSC of the corresponding materials achieves much higher values, 3243.75 μmol [O] g−1. The dynamic OSC comparison of the CeO2 and the Bi/CeO2 macrospheres (Fig. 4d) at different temperatures in the range of 200 °C–600 °C indicated that the Bi doped sample shows much better performance than pure CeO2 macrospheres.
Fig. 4 Bi doped CeO2 macrospheres: (a) XRD patterns, (b) FE-SEM image, and Raman spectra (c) and D-OSC (d) of CeO2 and Bi/CeO2 macrospheres. |
Footnotes |
† Electronic supplementary information (ESI) available: The TG-DSC isotherm, crystal structure, the N2 adsorption–desorption isotherms, FE-SEM images, SEM-EDAX. See DOI: 10.1039/c5qi00140d |
‡ These authors contributed equally to this work. |
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