10496 J. Phys. Chem. A, Vol. 108, No. 47, 2004
Shiraishi and Kawanishi
(linear velocity) in the photocatalytic reaction using a batch
recirculation reactor to elucidate the effect of film formed in
the neighborhood of the photocatalyst on the photocatalytic
reaction. As a result, we obtained the following conclu-
sions.
(1) The rate of formation of H2O2 in the photocatalytic
reaction apparently increases with the increase of the linear
velocity.
(2) This is probably because the thickness of the film becomes
thin with the increase of the linear velocity and the H2O2 formed
on the photocatalyst surface can easily move through the film
to the bulk liquid.
(3) This phenomenon can successfully be explained by using
a mathematical model for the overall photocatalytic reaction
that takes into consideration the diffusion of H2O2 through the
film.
(4) One of the reasons other researchers could not detect H2O2
in the photocatalytic reaction is that the reaction experiments
were performed under the conditions where H2O2 formed on
the photocatalyst was so quickly decomposed in the film that
the H2O2 concentration in the bulk liquid did not become
high.
(5) As a result, it is concluded that a diffusion film formed
in the neighborhood of the photocatalyst surface is responsible
for a reduction in the H2O2 concentration.
Figure 8. Comparison between initial rates of formation of hydrogen
peroxide from water and an aqueous solution of formic acid (light
source: black light blue fluorescent lamp).
according to the subsequent reactions described as e- + O2 f
-•
O2 f ‚‚‚‚ f H2O2.
References and Notes
Interestingly, the initial rate of formation of H2O2 for the
germicidal lamp is lower than that for the black light blue
fluorescent lamp in the region of low linear velocity, rapidly
increasing with the increase of linear velocity and finally
becoming higher. Considering the fact that the germicidal lamp
emits more powerful UV light than does the black light blue
fluorescent lamp, the experimental result is evidently contradic-
tory. This can be explained as follows. When the linear velocity
is low and the film is relatively thick, the H2O2 produced on
the photocatalyst surface must move slowly by diffusion through
the film to the bulk liquid. As a result, H2O2 is exposed for a
longer time to a highly reactive circumstance in the film,
crowded by a larger amount of radicals produced under
irradiation with the UV light from the germicidal lamp, and
the majority of H2O2 is quickly decomposed in the film. In the
region of high linear velocity, however, the thickness of the
film is thin and the H2O2 produced can quickly move out of
the film or is withdrawn from the film into the bulk liquid by
the recirculation flow passing through the neighborhood of the
photocatalyst surface, thereby increasing the H2O2 concentration
in the bulk liquid. Even when the film becomes very thin due
to a higher linear liquid velocity and the system is reaction-
controlled, H2O2 is decomposed by the radicals that are
continuously produced on the photocatalyst surface and by the
UV light in the bulk liquid. Consequently, the H2O2 concentra-
tion in the bulk liquid takes a constant value at a point where
the rate of formation of H2O2 is equal to the rate of decomposi-
tion of H2O2.
(1) Hoffmann, M. T.; Martin, S. T.; Choi, W.; Bahnemann, D. W.
Chem. ReV. 1995, 95, 69.
(2) Jaeger, C. D.; Bard, A. J. J. Phys. Chem. 1979, 83, 3146.
(3) Wang, C.; Rabani, J.; Bahnemann, D. W.; Dohrmann, J. K. J.
Photochem. Photobiol. A:; Chem. Eng. J. 2002, 148, 169.
(4) Matthews, R. W. J. Catal. 1988, 111, 264.
(5) Sabate, J.; Anderson, M. A.; Kikkawa, H.; Edwards, M.; Hill, C.
G. J. Catal. 1991, 127, 167.
(6) Cho, S.; Choi, W. J. Photochem. Photobiol. A. Chem. 2001, 143,
221.
(7) Augugliaro, V.; Coluccia, S.; Loddo, V.; Marches, L.; Marta, G.;
Palmisano, L.; Schiavello, M. Appl. Catal., B 1999, 20, 15.
(8) Rao, M. V.; Rajeshwar, K.; Pai Verneker, V. R.; DuBow, J. J.
Phys. Chem. 1980, 84, 1987.
(9) Hong, A. P.; Bahnemann, D. W.; Hoffmann, M. R. J. Phys. Chem.
1987, 91, 2109.
(10) Fukinbara, S.; Shiraishi, F.; Nagasue, H. CELSS J. 2000, 12, 9.
(11) Sha, J.; Shiraishi, F. Chem. Eng. J. 2004, 97, 203.
(12) Matthews, R. W. J. Phys. Chem. 1987, 91, 3328.
(13) Turchi, C. S.; Ollis, D. F. J. Phys. Chem. 1988, 92, 6853.
(14) Shiraishi, F. Computational methods for analysis of immobilized
enzyme reactions: from reaction kinetics to reactor-design methods;
Corona: Tokyo, 1997.
(15) Wang, S.; Shiraishi, F.; Nakano, K. J. Chem. Technol. Biotechnol.
2002, 77, 805.
(16) Shiraishi, F.; Hiromitsu, M.; Hasegawa, T.; Kasai, S. J. Chem.
Technol. Biotechnol. 1996, 66, 405.
(17) Wang, S.; Shiraishi, F. Eco-Engineering 2002, 14, 9.
(18) Fukinbara, S.; Shiraishi, F.; Nakano, K. CELSS J. 2001, 13, 1.
(19) Fukinbara, S.; Shiraishi, F. CELSS J. 2001, 13, 11.
(20) Matsuo, K.; Takeshita, T.; Nakano, K. J. Cryst. Growth 1990, 99,
621.
(21) Shiraishi, F.; Nakasako, T.; Hua, Z. J. Phys. Chem. A 2003, 107,
11072.
(22) Shiraishi, F.; Toyoda, K.; Fukinbara, S.; Obuchi, E.; Nakano, K.
Chem. Eng. Sci. 1999, 54, 1547.
(23) Wang, S.; Shiraishi, F.; Nakano, K. Chem. Eng. J. 2002, 87,
261.
5. Conclusion
In the present work, we investigated the relationship between
the rate of formation of H2O2 and the recirculation flow rate
(24) Bird, R. B.; Stewart, W. E.; Lightfoot, E. N. Transport phenomena;
John Wiley & Sons: New York, 1960.