X. Fan et al. / Materials Research Bulletin 46 (2011) 1315–1319
1317
Fig. 3. XRD patterns of ZrO2 hollow microspheres calcinated at different
temperature (a) 300 8C and (b) 500 8C.
the same diameters as original yeast size. Obviously, hydrolysis of
zirconium chloride occurred on the surface of the yeast cells and
the yeast cells played a role of templates in the process of preparing
ZrO2 hollow microspheres. The morphology of ZrO2 hollow
microspheres change little but the size changed slightly when
the dried particles were calcined at different temperature, as
shown in Fig. 2(b) and (c). The size of ZrO2 hollow microspheres is
Fig. 4. Nitrogen adsorption–desorption isotherms and the corresponding pore size
distribution (inset) for the ZrO2 hollow microspheres.
pore structure shows benefits not only to the delivery of
macromolecules, but also to the shape selectivity of micro-
molecules.
about 2.0–3.0
mm. The shrinkage of the particles is attributed to
the removing of organic molecules during heat treatment. The
cracked spheres and apparent cavities show the hollow nature of
the products. The thickness of ZrO2 hollow microspheres shell is
estimated to be about 100 nm. In addition, it was found that the
thickness of the shells of ZrO2 hollow microspheres can be tuned
by the concentration of zirconium chloride rather than reaction
time at 30 8C. Careful observation shows that the surfaces of these
microspheres are constructed by nanoparticles as shown in
Fig. 2(d).
3.1.4. The infrared spectrogram analysis of hollow microspheres
Fig. 5 shows the FT-IR spectrum of ZrO2 hybrid microsphere
and original yeast templates. On the curve of the original yeast
templates, the bands at 1652.9 cmÀ1 could be attributed to the
C55O stretching vibration of the amide I band of proteins. The bands
at 3419.6 could be ascribed to the O–H, C–H, N–H stretching
vibration of the groups which possess hydrogen. On the basis of FT-
IR spectrum of original yeast, shows that active components of
yeast contain these groups. Compared Fig. 5(b) with (a), we found
that the shoulder peak at 1652.9 cmÀ1 in Fig. 5(b) corresponding to
the C55O stretching vibration splits to 1593.1 cmÀ1and
1529.4 cmÀ1 in Fig. 5(a) that belong to Zr–O–C deformation
vibration. The spectrum of original yeast exhibited clear shifts from
3.1.2. The structure of ZrO2 hollow microspheres
The XRD patterns of ZrO2 hollow microspheres synthesized via
the yeast bio-template route are shown in Fig. 3.
As shown here, the crystallization of zirconia has been achieved
almost perfect at 300 8C (Fig. 3(a)). The crystallization is
intensified with the increase of calcinations temperature as shown
in Fig. 3(b). Lower crystallization temperature may be confirmed
that the yeast cells not only are used templates but also the active
bio-molecules of yeast cells take part in the nucleation, growth and
crystallization of ZrO2. All the diffraction peaks can be indexed to
the tetragonal phase structure of ZrO2 (JCPDS 79-1769), and no
peaks of other materials or phases are observed, which indicates
the high purity of the products. The crystallite sizes, as estimated
by Scherrer formula, corresponding to (0 1 1) crystal plane are
6.9 nm (in Fig. 3(a)) and 11.4 nm (in Fig. 3(b)).
3419.6 cmÀ1
,
2927.7 cmÀ1
,
1456.2 cmÀ1 and 1130.2 cmÀ1in
2925.8 cmÀ1 1425.3 cmÀ1 and
Fig. 5(b) to 3415.7 cmÀ1
,
,
1132.1 cmÀ1 in Fig. 5(a) due to the interaction between reactive
functional groups such as carbonyls, hydroxyls, acid amides
andZr2+ by electrostatic force, hydrogen bond and covalent bond.
3.1.3. The pore structure of ZrO2 hollow microspheres
The ZrO2 hollow microspheres are further characterized by
nitrogen adsorption and desorption isotherms at 77 K, as shown in
Fig. 4.
Fig. 4 shows a type III-like isotherm with H3-hysteresis,
indicating the presence of slit-like type porosity in the micro-
spheres. The Barrett–Joyner–Halenda (BJH) method was used to
calculate the pore size distribution (as shown in Fig. 4 inset). The
result indicates that the specific surface area is 70.322 m2/g and
the pore volume is 0.077 cm3/g. However, for the solid micro-
spheres, the specific surface area is 57.708 m2/g and the pore
volume is 0.013 cm3/g. The hollow microspheres have a bimodal
pore structure: the smaller pores with a diameter of 18 nm and the
bigger pores of approximately 35 nm in diameter. This bimodal
Fig. 5. FT-IR spectrum of (a) ZrO2 hollow spheres without the calcined and (b)
original yeast templates.