Sol–gel synthesis of mesoporous spherical zirconia

Yulei Changa, Chen Wangc, Tongxiang Liang*a, Chunsong Zhaob, Xi Luob, Ting Guoa, Jianghong Gongb and Hui Wu*b
aState Key Laboratory of New Ceramics and Fine Processing, Institute of Nuclear and New Energy Technology, Tsinghua University, Beijing, 100084, China. E-mail: huiwu@tsinghua.edu.cn; txliang@tsinghua.edu.cn
bState Key Laboratory of New Ceramics and Fine Processing, School of Materials Science and Engineering, Tsinghua University, Beijing, 100084, China
cBeijing Key Laboratory of Fine Ceramics, Institute of Nuclear and New Energy Technology, Tsinghua University, Beijing, 100084, China

Received 10th November 2015 , Accepted 30th November 2015

First published on 1st December 2015


Abstract

Mesoporous spherical zirconia (ZrO2) with a surface area of 113 m2 g−1 and average pore size of 5.0 nm is prepared by a sol–gel method with ZrOCl2·8H2O precursors and Sodium Dodecyl Sulfonate (SDS) templates with subsequent annealing at 500 °C in air. After calcination at 700 °C, the tetragonal phase transfers to monoclinic zirconia and the surface area is reduced to 26 m2 g−1. The mesoporous spherical structure, which is assembled by aggregation of the ZrO2 nanoparticles, is confirmed by characterization using low and wide-angle X-ray diffraction, Transmission Electron Microscopy (TEM) and Scanning Electron Microscopy (SEM). Mesoporous ZrO2 with a surface area of 113 m2 g−1 has a higher adsorption for Cs ion (357 mg g−1). For the 700 °C calcinated ZrO2, the absorption capacity at equilibrium is only 188 mg g−1.


Introduction

Inorganic nanomaterials with mesoporous structures have received great attention due to large surface areas, easy functionalization, possibilities for applications in catalysis1,2 and other favourable characteristics. Mesoporous materials with controllable morphologies, pore sizes, and variable composition are highly desired for their advanced applications.3 While silica of mesoporous structure4,5 was successfully applied in many fields, synthesis of mesoporous materials of a board range of transition metal oxides have aroused scientists' interests for multiple applications,6,7 since transition metal oxides can be effectively applied as catalyst supports,8,9 chemical sensors,10,11 solid oxide fuel cells12 and photocatalystic materials.13 ZrO2 has better ion transfer performance and the concentration of oxygen vacancy because it has both acid sites and basic sites on surface. ZrO2 can acts as not only the carrier but the catalyst for some reactions. Introducing a mesoporous structure into the transition metal oxides is a promising route to upgrade the properties.

As nuclear energy is developed rapidly nowadays, radioactive waste has become a big problem. Many countries are devoted to researching into ADS (accelerator driven systems) reactor14 which is designed to accomplish the high level radioactive waste (HLW) disposal. When choosing the matrix used in the ADS fuel to absorb radioactive waste, the thermal and mechanical properties, activation with neutrons, and chemical compatibility with neighboring materials, irradiation resistance should be considered.15 ZrO2, MgO, MgAl2O4 and Y3Al5O12 are usually considered as inert matrix for inert matrix fuel (IMF), among which, ZrO2 is a promising candidate because of its excellent mechanical properties, including high strength, high hardness and high fracture toughness. Currently ZrO2–Minor Actinides (MA) fuel is manufactured by infiltration route, the first step is the production of ZrO2 kernels using sol–gel method, and then the calcinated ZrO2 kernels are immersed in actinide solution so that the infiltrated kernels are obtained.16 This infiltration method does have two limitations, (1) the ratio of MA to the matrix is too low and cannot be chosen freely, i.e., the content of MA, that can be infiltrated, is determined by the porosity of the kernels. (2) The size and distribution of pores in the ZrO2 after calcinated are heterogeneous, resulting in the maldistribution of MA. The uneven distribution of MA further degrades properties of fuels. Nevertheless the ZrO2 with mesoporous structure have a promising to enhance volume and homogeneity of adsorption for MA.

There are different ways to compound mesoporous ZrO2, broadly separated into hydrothermal synthesis,17,18 non-hydration method,19 sol–gel method20,21 and soft or hard template method.22 Hudson and Knowles et al.23 use CTMAB (hexadecyl trimethyl ammonium bromide) as template and ZrOCl2 as the source of zirconium to react in the alkaline aqueous solution and then the precursor was calcinated in hydrothermal synthesis reactor to compound mesoporous ZrO2. Pacheco et al.24 used dodecyl dihydrogen phosphate as template and zirconium(IV) ethoxide as the source of zirconium to prepare mesoporous ZrO2 in acid isopropyl alcohol solution. Dong et al.25 invented a hard template method to prepare mesoporous oxide and the process was described as followed. Firstly, uniform mesoporous silica spheres prepared by Unger's method26 are used as the template for the formation of mesoporous carbon sphere by the nanocasting technology,27 and then mesoporous ZrO2 are obtained by templating the specific precursor with carbon sphere whereafter. Lu et al.28 use sol–gel method to synthesis yttria-stabilized mesoporous ZrO2. However, a facile technique that is easy to practice and inexpensive to synthesis uniform and high surface area sphere-shaped ZrO2 with inner mesoporous structure is still lacking. In this work, we present a simple and practicable facile sol–gel approach with the aid of structure-directing surfactant to synthesize ZrO2 nanoparticles with mesoporous structure. We use low-cost material ZrOCl2 (zirconium oxychloride) and CO(NH2)2 (carbamide) as raw materials to prepare mesoporous zirconia by sol–gel method29 with the aid of SDS (sodium dodecyl sulfate)30 as template. Moreover, a novel and interesting structure is found in the ZrO2 powders. An amount of zirconia spheres are obtained and mesopore spreading on sphere. The specific surface area of mesoporous ZrO2 is quite high comparing with samples of the precious methods and becomes higher after aging in ammonia solution.

Experimental

Chemicals

ZrOCl2 (≥99.0%), SDS (Sodium Dodecyl Sulfonate), CO(NH2)2 (≥99.0%) (carbamide) and ammonia solution (25–28%) are purchased from Sinopharm Chemical reagent Co. Ltd. All chemicals are used as received without further purification.

Preparation

The following synthesis procedure is employed for the preparation of mesoporous zirconia nanoparticles. (1) 3.759 g SDS is dissolved in 400 ml deionized water. The SDS solution is then stirred on the magnetic stirring apparatus for about 3 h until SDS is totally dissolved in H2O as solution A. (2) 0.25 mol (15.02 g) carbamide and 0.1 mol (32.21 g) ZrOCl2 are dissolved in 100 ml deionized water as solution B. (3) We inject solution B into solution A using injection pump in a rate of 0.6 ml min−1, meanwhile, the mixture solution is heated in water bath to 75 °C. After injecting all the solution B into A, solution C is obtained with 28.0 mmol L−1 SDS and 0.5 mol L−1 carbamide and 0.2 mol L−1 ZrOCl2. (4) The C solution is turned to be viscous sol after reacting for 12 h at 75 °C. Afterward, the viscous sol is dried for 24 h at 80 °C in air atmosphere under atmospheric pressure to obtain a porous solid mass (xerogel). (5) The porous solid mass is calcinated under air at 500 °C and 700 °C for 5 h and naturally cooled under air condition to remove the SDS surfactant and then the desired mesoporous ZrO2 particles are obtained.

Characterization

The X-ray diffraction (XRD) analyses are used to identify the crystalline phase of the sample, which are performed on a SmartLab diffractometer (Cu Kα radiation, λ = 1.5406 Å) with an operating voltage of 40 kV and a current of 40 mA. Morphological characterization is obtained by means of scanning electron microscope (SEM) using MERLIN VP Compact with an accelerating voltage of 1.0 kV. When conducting the SEM analyses, a small quantity of ZrO2 powder was dispersed in ethyl alcohol under ultrasound so that the nanoparticle can be dispersed homogeneously. Transmission electron microscopy (TEM) is accomplished using Tecnai G2 TEM with the operating voltage of 200 kV. Nitrogen adsorption/desorption isotherms are obtained using a BEL Japan Inc. Belsorp-HP surface area analyser at 77 K. The surface areas are calculated by the Brunauer–Emmett–Teller (BET) method and the pore size distributions are calculated by the Barrett–Joyner–Halenda (BJH) method from the adsorption/desorption isotherm. The samples are prepared by ultrasonic dispersing the material in methanol and then dripped one drop on a carbon coated copper grid when doing TEM.

Adsorption experiments

The cesium ion (Cs+) adsorption on ZrO2 is investigated. Cesium is supplied as cesium chloride from Sigma-Aldrich company. Stock solutions of the test reagent are prepared by dissolving CsCl in distilled water, the initial concentration is 150 mg L−1, and the initial pH is adjusted to the value of 7.0 using dilute solution of sodium hydroxide. 40 mg of ZrO2 adsorbent is added into the solution at 25 °C. Then, the suspension is stirred for 5 hours. After centrifugation, the residual quantity of Cs+ is determined by ICP-AES. The absorption capacity qe (mg g−1) at equilibrium is calculated: qe = (C0Ce)V/W, where C0 (mg L−1) and Ce (mg L−1) are the concentrations of Cs+ at initial and equilibrium, respectively. V (L) and W (g) are the volume of solution and the mass of adsorbent, respectively.

Results and discussion

X-ray diffraction

As we can see in Fig. 1(a), the as-synthesized particles are amorphous. Two phase transformations are observed with increasing calcination temperature. The first one is a transformation from the amorphous state to crystalline tetragonal zirconia, which finished at about 500 °C. The second phase transformation is from tetragonal to monoclinic zirconia, which occurred after calcination at 700 °C. This transition from the amorphous to the metastable tetragonal phase and then to the thermodynamically stable monoclinic phase only after heating at higher temperatures is common and has been reported for zirconia particles.31,32 For the first phase transformation, it is commonly accepted that the short-range order in the amorphous phase is more similar to the tetragonal rather than the monoclinic phase.32 Thus, initial crystallization at 500 °C yields the metastable tetragonal phase, its XRD pattern correspond to the well crystallized with tetragonal phases (PDF number: 89-6976), the primary crystal size is 6.4 nm as calculated by applying the Scherrer equation on the (011) diffraction peak. It has been reported that below a critical grain size, tetragonal rather than monoclinic becomes the thermodynamically preferred phase due to differences in the surface energies of the polymorphs. This critical size has been reported to be typically of the order of 10–20 nm.31
image file: c5ra23782c-f1.tif
Fig. 1 (a) XRD pattern of the synthesized mesoporous-assembled ZrO2 nanoparticles; (b) XRD pattern in the low angle range of the synthesized mesoporous-assembled ZrO2 nanoparticles.

Small-angle diffraction of ZrO2 calcinated at 500 °C and 700 °C is done for the purpose of testing if there is mesoporous structure in this sample. The result is shown in Fig. 1(b). After calcinated at 500 °C, there is a peak and the beginning of the pattern which means there are mesopores in the material. But the peak intensity is reduced when the sample is calcinated at 700 °C, this means some mesopores disappeared.

Scanning electron microscope (SEM) and transmission electron microscopy (TEM)

Fig. 2 shows that the obtained material is spherical particles with the size ranged from 100 nm to 300 nm. The inset of Fig. 2 indicates that the surface of particles is not smooth and the spherical particles are agglomerates, i.e., they are composed of many tiny particles.
image file: c5ra23782c-f2.tif
Fig. 2 SEM image of synthesized particles after calcinated at 500 °C, showing regular sphere morphologically.

The shape and size of ZrO2 nanoparticles are controlled by synthesis method, stabilizer or surfactant,32 it is generally accepted that ZrO2 particles are formed in two step mechanism.33 First, ZrO2 precursors are hydrolyzed and polymerized to form small primary particles in the size range of 1–10 nm, and then aggregate to form the final particles. As diffusion-limited aggregation mostly leads to disordered particles with no structural porosity, in Fig. 2, one spherical particle is composed of many tiny particles, thus, the present reaction is believed to proceed via reaction-limited aggregation.

Fig. 3 is the TEM and SAED images of ZrO2 spherical particles after calcinated at 500 °C. As shown in Fig. 3(a) and (b), the particle is obviously spherical and many pores (about 5.0 nm in the length scale) spreading over the spheres, each sphere is composed of hundreds of individual tiny nanoparticles with an average diameter of about 5 nm, it can be conclude that the mesopore is created by assembly of zirconia nanoparticles. During calcination at 500 °C, amorphous zirconia transfers to tetragonal phase, rearrangement of the individual nanoparticles could occur, which results in the formation of strong covalent bridges between the particles. This covalent bonding between particles could be responsible for the high thermal stability of the mesoporous ZrO2 nanoparticles. Thus, ZrO2 nanocrystallites assembled to form thick mesoporous walls.


image file: c5ra23782c-f3.tif
Fig. 3 (a) Low magnification TEM image of ZrO2 sphere shows that big sphere is consist of tiny particle; (b) in the low magnification TEM image, the space between tiny particle is mesopore size; (c) high magnification TEM images of some particles; (d) SAED image of multicrystal ZrO2.

Fig. 3(c) is the high magnification TEM image of some particles. As we can see in the picture, the pore wall is multicrystal and the lattice space of 0.3 nm assigned to the interplanar distance of the (101) planes of the sample. The corresponding Selected Area Electron Diffraction (SAED) pattern (Fig. 3(d)) of the spherical aggregates of ZrO2 nanoparticles is indicative of high nanocrystallinity of the formed product and can be assigned to the tetragonal phase, the concentric Debye–Scherrer rings which can be indexed to the (011), (110), (020) and (121) planes. The d-spacing corresponding to the diffraction rings of the SAED pattern are in good agreement with the tetragonal phases of ZrO2 nanocrystal.

Surface area and porosity

After calcinated at 500 °C, the spherical ZrO2 nanoparticle scaffold exhibits a mesoporous channel system, displaying high surface areas and narrow pore size distribution. Fig. 4 shows N2 adsorption–desorption isotherm of the sample calcinated at 500 °C, in which pore structure is confirmed clearly. The isotherm displays the typical type IV curve, which is usually attributed to the predominance of mesopores. The presence of a pronounced hysteresis loop in the isotherm curve is indicative for a 3D intersection network of the pores, which also goes well with the TEM observation. Moreover, the isotherms possess evident hysteresis loop with an evident increase in adsorbed N2 volume in the relative pressure range of 0.45–0.90. This indicates the capillary condensation of N2 molecules inside the sufficiently pores of small sizes. The average size of the mesopore is calculated to be about 5.0 nm.
image file: c5ra23782c-f4.tif
Fig. 4 N2 adsorption–desorption isotherm of ZrO2 calcinated at 500 °C.

The spherical ZrO2 nanoparticle calcinated at 500 °C exhibits 113 m2 g−1 of surface area by a nitrogen Brunauer–Emmett–Teller (BET) measurement, which is rather high comparing with previous result. Qibing Chang20 synthesized mesoporous ZrO2 with the surface area of 43 m2 g−1. After calcinated at 700 °C, the surface area of ZrO2 nanoparticle reduced to 26 m2 g−1. In bulk zirconia, phase transformation from tetragonal to monoclinic is accompanied by a volume expansion of 3–5%. This volume expansion will result in the collapse and disappear of mesopores.

To explain the special morphology of mesoporous, in Fig. 5, we suppose a model for the forming of mesoporous spherical ZrO2 particles. When ZrOCl2·8H2O is dissolved in water [Zr4(OH)8(H2O)16]8+ complexation is formed, and carbamide is hydrolyzed to NH4+ and OH, then Zr(OH)4−x(OOH)x, is precipitated by the action of OH, finally ZrO2 is produced during the subsequent heating. The whole reaction formula can be expressed as:

 
4ZrOCl2·8H2O → [Zr4(OH)8(H2O)16]8+ + 8Cl + 8H+ (1)
 
CO(NH2)2 + 3H2O → 2NH4+ + 2OH + CO2 (2)
 
[Zr4(OH)8(H2O)16]8+ + 8xOH → 4Zr(OH)4−x(OOH)x−(2+2x) + (24 + 8x)OH (3)
 
Zr(OH)4−x(OOH)x → ZrO2 (amorphous) → t-ZrO2 or m-ZrO2 (4)


image file: c5ra23782c-f5.tif
Fig. 5 Mechanism for the forming of mesoporous spherical ZrO2 particles.

[Zr4(OH)8(H2O)16]8+ in aqueous solution generates Zr(OH)4−x(OOH)x nanoparticles and grows slowly because of the slow introduction of OH from the release of carbamide, and these nanoparticles are adhere to the surface of SDS surfactant. During drying of the solvent, the surfactant induces cooperative assembly of functionalized nanoparticles to attain packing, results in the formation of large spherical particles. When the SDS template is removed from the particles, the mesopores are formed.

Adsorption of cesium ions on ZrO2

It is known that pH is important factor for the adsorption of metal ions on adsorbents, because it affects the solution chemistry of the solute as well as the functional groups present in the sorbent. According to ref. 34, zirconia contains hydroxyl groups which can act role in ion-exchange reaction through the substitution of its protons by cesium ion, the reactions is:
 
nCs+ + Zr(–OH)m ↔ Zr(–O–Cs)mn + nH+ (5)
where –OH is hydroxyl group, nH+ is number of protons released, and Zr refers to the zirconia surface. The adsorption process is influenced by pH, contact time and temperature. The highest removal efficiency of zirconia for cesium ion was obtained at pH 7.0.35 In this paper we fix the experimental parameters as: pH = 7, temperature = 25°, the purpose is to compare the adsorption capacity of several kinds of powder on Cs ion. The adsorption equilibrium is reached within 2 hours. Table 1 shows the adsorption capacity of Cs ion on ZrO2, where Z5 means ZrO2 calcinated at 500 °C, Z7 means ZrO2 calcinated at 700 °C, and R is the data from ref. 35.
Table 1 The adsorption capacity of Cs ion
Sample Surface area (m2 g−1) qe (mg g−1)
Z5 113 357
Z7 26 188
R 130


Our result indicates that the mesoporous ZrO2 has a higher adsorption for Cs ion. Future work includes: adding Y to stable ZrO2 phase, improving the specific surface area, studying the effect of monoclinic and tetragonal phase on the adsorption behaviour, surface modification to improve the adsorption or selective adsorption capacity, and the adsorption behaviour of other radionuclides, etc.

Conclusions

In this work, we produce mesoporous sphere of zirconia from a simple sol–gel processing. Carbamide will release OH when heated to 70 °C in acid solution and OH is the essential group of ZrO2 precursor. After calcinated at the temperature of 500 °C under air condition, the sample exhibit regular nanospherical which consists of tiny particles. The space between these tiny particles is mesopore size and the surface area is as higher as 113 m2 g−1. The adsorption for Cs ion on this kind of mesoporous spherical ZrO2 is 357 mg g−1. When calcinating at 700 °C, tetragonal phase transfers to monoclinic zirconia and the surface area is reduced to 26 m2 g−1, the adsorption for Cs ion is only 188 mg g−1.

Acknowledgements

This work is supported by the National Natural Science Foundation of China (Grand No. 21271114 and No. 91326203); Tsinghua University independent research and development fund (20111080982) and Program for Changjiang Scholars and Innovative Research Team in University (IRT13026).

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