1374
A.A. Ashkarran et al. / Polyhedron 29 (2010) 1370–1374
of K. The calculated reaction rate constant for the samples prepared
at 10, 15 and 20 A arc currents were 16 ꢁ 10ꢀ3, 14 ꢁ 10ꢀ3 and
5 ꢁ 10ꢀ3 minꢀ1, respectively. Furthermore, compared with com-
mercial TiO2 photocatalyst (Degussa P25) in an equal situation,
our 10 A sample shows near two times more photocatalytic activity.
4. Conclusion
We have prepared ZrO2 nanoparticles in a one-step synthesis
process by a high current electrical arc discharge of Zr electrodes
in DI water. XRD results indicated formation of a mixture of nano-
crystalline ZrO2 monoclinic and tetragonal phase and 26.5 nm sin-
gle crystalline domain size. Surface chemical composition of the
nanoparticles determined by XPS shows formation of ZrO2. TEM
images revealed spherical nanoparticles with 21 and 42 nm mean
particle size at 10 and 20 A arc currents, respectively. The particle
size was found to increase with an increase in the arc current. Sur-
face area of the sample prepared at 10 A arc current, measured by
BET analysis, was 44 m2/g. Further, the photocatalytic activity of
ZrO2 nanoparticles demonstrated that by increasing UV illumina-
tion time, the maximum absorption peak and concentration of
Rh. B decreases in the presence of ZrO2 nanoparticles. In fact, de-
crease of concentration of the sample prepared at 10 A was found
to be more pronounced than the sample prepared at 15 and 20 A
arc current which was due to increased surface to volume ratio.
Fig. 6. Changes of rhodamine
samples prepared at 10, 15 and 20 A arc currents and the blank sample.
B concentration under UV illumination for the
6
S ¼
qd
which
q is the solid density, S is the specific surface area and d is the
References
particle size. The average size of the nanoparticles calculated by this
model is 24 nm which is in close agreement with TEM results.
[1] B. Zhu, C.R. Xia, X.G. Luo, Thin Solid Films 385 (2001) 209.
[2] N.G. Petrik, D.P. Taylor, T.M. Orlando, J. Appl. Phys. 85 (1999) 6770.
[3] A. Bastianini, G.A. Battiston, R. Gerbasi, M. Porchia, S. Daolio, J. Phys. 4 (5)
(1995) 525.
3.5. Photocatalytic activity measurements
[4] A. Corma, Chem. Rev. 95 (1995) 559.
Changes in the absorption spectrum of Rh. B under UV illumina-
tion at different irradiation times for the samples made with 10, 15
and 20 A arc currents and one Rh. B sample as reference are illus-
trated in Fig. 5. No remarkable changes in the concentration of the
Rh. B solution were observed in the absence of ZrO2 nanoparticles
(Fig. 5a). Therefore, decomposition of Rhodamine B only depends
on the photoexcitation of ZrO2 nanoparticles. The concentration
and volume of all ZrO2 samples were chosen at 10 mM and
30 mL, respectively, with 1:1 ratio of ZrO2 to Rh. B for all measure-
ments. We have measured yield and average production rate of
ZrO2 nanoparticles by measuring weight loss of the electrodes
and duration of the arc process. To achieve same ZrO2 concentra-
tion in all samples we have chosen 5, 3 and 2 s arc durations for
10, 15 and 20 A, respectively. It was observed that by increasing
the irradiation time the maximum absorption peak decreases. This
indicates that the concentration of Rh. B is decreasing at the pres-
ence of ZrO2 nanoparticles and UV illumination, Fig. 5(b–d).
Though all kinetic curves behave similarly, for the case of the larger
particles photodegradation rate is less, as illustrated in Fig. 6. This
can be due to higher surface area in samples with smaller size.
Photocatalytic reactions on ZrO2 surface can be expressed by
the Langmuir–Hinshelwood model [25]. The reaction rate after
the adsorption equilibrium can be expressed as
[5] G. Tian, K. Pan, H. Fu, L. Jing, W. Zhou, J. Hazard. Mater. 166 (2009) 939.
[6] M.N. Tahir, L. Gorgishvili, J. Li, T. Gorelik, U. Kolb, L. Nasdala, W. Tremel, Solid
State Sci. 9 (2007) 1105.
[7] G. Ehrhart, B. Capoen, O. Robbe, P. Boy, S. Turrell, M. Bouazaoui, Thin Solid
Films 496 (2006) 227.
[8] A.M. Torres-Huerta, M.A. Dominguez-Crespo, E. Ramirez-Meneses, J.R. Vargas-
Garcia, Appl. Surf. Sci. 255 (2009) 4792.
[9] C. Rozo, D. Jaque, L.F. Fonseca, J.G. Sole, J. Lumin. 128 (2008) 1197.
[10] H. Lange, M. Sioda, A. Huczko, Y.Q. Zhu, H.W. Kroto, D.R.M. Walton, Carbon 41
(2003) 1617.
[11] N. Sano, J. Nakano, T. Kanki, Carbon 42 (2004) 667.
[12] N. Sano, H. Wang, I. Alexandrou, M. Chhowalla, K.B.K. Teo, G.A.J. Amaratunga, J.
Appl. Phys. 92 (2002) 2783.
[13] N. Sano, H. Wang, M. Chhowalla, I. Alexandrou, G.A.J. Amaratunga, Nature 414
(2001) 506.
[14] I. Alexandrou, N. Sano, A. Burrows, R.R. Meyer, H. Wang, A. Ikirkland, C.J. Kiely,
G.A.J. Amaratunga, Nanotechnology 14 (2003) 913.
[15] W.T. Yao, S.H. Yu, Y. Zhou, J. Jiang, Q.S. Wu, L. Zhang, J. Jiang, J. Phys. Chem. B
109 (2005) 14011.
[16] C.H. Loa, T.T. Tsung, H.M. Lin, J. Alloys Compd. 434–435 (2007) 659.
[17] A. A Ashkarran, A. Iraji zad, M. M Ahadian, M.R. Hormozi Nezhadi, Eur. Phys. J.
Appl. Phys. 48 (2009) 10601.
[18] J.K. Lung, J.C. Huang, D.C. Tien, C.Y. Liao, K.H. Tseng, T.T. Tsung, W.S. Kao, T.H.
Tsai, C.S. Jwo, H.M. Lin, L. Stobinski, J. Alloys Compd. 434–435 (2007) 655.
[19] A.A. Ashkarran, A. Iraji zad, S.M. Mahdavi, M.M. Ahadian, M.R. Hormozi
Nezhad, Appl. Phys. A 96 (2009) 423.
[20] A.A. Ashkarran, A. Iraji zad, M.M. Ahadian, S.A. Mahdavi Ardakani,
Nanotechnology 19 (2008) 195709.
[21] A.A. Ashkarran, A. Iraji zad, S.M. Mahdavi, M.M. Ahadian, Mater. Chem. Phys.
118 (2009) 6.
[22] Y.W. Zhang, X. Sun, G. Xu, C.H. Yan, Solid State Sci. 6 (2004) 523.
[23] J. Liang, X. Jiang, G. Liu, Z. Deng, J. Zhuang, F. Li, Y. Li, Mater. Res. Bull. 38 (2003)
161.
[24] S.J. Gregg, K.S.W. Sing, Adsorption Surface Area and Porosity, Academic Press,
1982.
ꢀ lnðC=C0Þ ¼ Kt
where C and C0 are the reactant concentration at time t = t and t = 0,
respectively, K and t are the apparent reaction rate constant and
time, respectively. A plot of ꢀ lnðC=C0Þ versus t will yield a slope
[25] D.L. Liao, C.A. Badour, B.Q. Liao, J. Photochem. Photobiol. A 194 (2008) 11.