ISSN 1203-8407 © 2010 Science & Technology Network, Inc. J. Adv. Oxid. Technol. Vol. 13, No. 3, 2010 262
Considerations of Particle Size in Aqueous Phase Photocatalysis kinetics
with TiO
2
Catherine Almquist*
Paper and Chemical Engineering Department, Miami University, Oxford, Ohio 45056, USA
Abstract:
There are inconsistencies in the literature regarding the optimum particle size for TiO
2
in photocatalytic oxidation
reactions in aqueous slurries. The apparent optimum particle size has been reported as low as 3 nm and ranges to
greater than 30 nm. It was hypothesized that the inconsistencies reported in the literature stem from differences
in the photocatalyst, the reactor system and the operating parameters used, among other factors. In this study, a
mathematical model was developed to elucidate the effects of selected operating parameters on the apparent
optimum particle size in aqueous-phase TiO
2
photocatalysis. The model utilizes five parameters, which were
varied to best fit one set of experimental data: the photocatalytic oxidation of dimethyl methylphosphonate
(DMMP) in water. For this set of experimental data, the apparent optimum particle size was approximately 25 nm,
and the model parameters were set to fit this set of data. The sensitivity of the model to the model parameters
and operating conditions were assessed, and the theoretical trends based upon model calculations were supported
by observed trends of experimental data reported in the literature. It was found that the apparent optimum
particle size can change significantly with TiO
2
concentration and depth of slurry perpendicular to the incident
light. This supports that the light scattering model parameter, k
scat
, is the most significant model parameter that
determines the apparent optimum particle size.
Introduction
There have been many published manuscripts
reporting on the role of particle size in photocatalysis
over the past 25 years (1-12). In brief, authors state that
competing effects of increasing surface area, decreasing
light absorption efficiencies, and increasing rates of
electron-hole recombination as particle size decreases
results in an optimum particle size for aqueous-phase
TiO
2
photocatalysis. However, the reported “optimum”
particle sizes in the literature vary widely for TiO
2
photocatalysis, from < 5 nm to over 30 nm. Table 1
provides a partial list of authors that have investigated
the role of particle size in TiO
2
photocatalysis and their
key findings.
Noted is that the role of particle size in TiO
2
photocatalytic slurry reactors cannot be isolated easily
in theory or in practice. Subtle differences in surface
sites, defects, and structural properties of the photo-
catalysts result from differences in synthesis methods
and can affect the efficiency at which electron-hole
pairs are formed and recombined upon absorption of
light energy. In addition, differences in reactor design
and experimental operating parameters can affect the
apparent optimum particle size by altering secondary
(agglomerate) particle formation, adsorption coeffi-
*E-mail address: almquic@muohio.edu ; Tel.: 513-529-0767;
Fax: 513-529-0761
cients, and the light propagation into the reaction
slurry. Therefore, the isolation of the effect of particle
size is difficult, at best. However, in this paper, a
model was developed to consider the role of particle
size in the observed kinetics of photocatalytic oxidation
reactions in aqueous slurry reactors.
Theory
Although several reactions occur in photocatalysis,
as presented in the published literature (13-17), the
reactions used in the development of this model, and a
list of assumptions used to formulate this model are
provided in Tables 2 and 3, respectively.
As shown in Reaction 1 of Table 2, the absorption
of light by TiO
2
generates electron-hole (e
-
-h
+
) pairs
in the reaction slurry. The rate at which electron-hole
pairs are generated per unit volume of reaction slurry
at depth z into the reactor is represented as follows:
) ( ) (
1
z I k z g (1)
where g(z) represents the rate of electron-hole
generation on the surface of the TiO
2
particles (moles
s
-1
m
-3
) in the slurry reactor at a distance z into the
reaction slurry, is the light absorption coefficient (m
-1
)
(Eq 2), I(z) is the light intensity (W/m
2
) at a depth z
(m) into the reactor, and k
1
is the rate constant (moles
e
-
-h
+
at surface of the TiO
2
particles W
-1
s
-1
).
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