dynamic simulation of batch photocatalytic reactor (bpr) for wastewater treatment
TRANSCRIPT
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ORIGINAL CONTRIBUTION
Dynamic Simulation of Batch Photocatalytic Reactor (BPR)for Wastewater Treatment
Suman Dutta
Received: 6 March 2012 / Accepted: 21 September 2012 / Published online: 8 December 2012
� The Institution of Engineers (India) 2012
Abstract Reactive dyes discharged from dyehouse causes
a serious environmental problem. UV/TiO2 photocatalysis
has been employed effectively for these organic dyes
removal from dye-house effluent. This process produces less
amount of non-toxic final product. In this paper a photocat-
alytic reactor has been designed for Reactive red 198
(RR198) removal from aqueous solution. The reactor is
operating in batch mode. After each batch, TiO2 catalyst has
been separated and recycled in the next batch. Mathematical
model equation of this batch photocatalytic reactor (BPR)
has been developed considering Langmuir–Hinshelwood
kinetics. Simulation of BPR has been carried out using fourth
order Runge–Kutta (RK) method and fifth order RK method
(Butcher method). This simulation results can be used to
develop an automatic photocatlytic reactor for industrial
wastewater treatment. Catalyst activity decay and its effect
on each batch have been incorporated in this model.
Keywords Reactive red 198 �Batch photocatalytic reactor � Catalyst deactivation �Dynamic simulation � Fifth order R–K method
List of Symbols
a Catalyst activity (-)
a0 Initial catalyst activity (-)
b Langmuir isotherm constant (Lm g-1)
cA; ½Dye� Dye concentration in the reactor (mg L-1)
cA0 Initial dye concentration in reactor (mg L-1)
Cper Permissible limit of dye concentration (mg L-1)
½Dye�ads Dye concentration in the solid (adsorbent)
phase (mg g-1)
h Time step during simulation (min)
k0
Reaction rate constant with fixed TiO2
concentration (g L-1 min-1)
kad Catalyst deactivation kinetic constant (min-1)
KL Langmuir isotherm constant (L g-1)
kr Apparent kinetic constant (L mg-1 g-1)
rdecol Rate of dye decolorization in the reactor
(mg g-1 min-1)
t Time (min)
½TiO2� TiO2 concentration in the reactor (g L-1)
t0 Initial/starting time (min)
tn Time after nth step (min)
V Reactor volume (L)
W Catalyst weight (g)
Introduction
Textile industry is one of the highest water consuming
sectors. Water pollution due to organic dyes is a major
problem for textile industries. After dying, more than 15 %
of the dyes are lost in wastewater streams [1]. These dyes
impart color to water and thus lower its aesthetic value [2].
Dyes are difficult to remove since many of them are bio-
logically non-degradable. Conventional methods for color
removal, using a primary and a secondary treatment are
unsuitable. A tertiary treatment is often needed to remove
color for discharge into a municipal sewer or into a natural
stream [3]. Unless properly treated, the dyestuffs present in
wastewaters can significantly affect photosynthesis activity
due to reduced light penetration and may also be toxic
to certain forms of aquatic life due to the presence of
substituent metals and chlorine [4].
S. Dutta (&)
Department of Chemical and Polymer Engineering,
Birla Institute of Technology Mesra, Ranchi, India
e-mail: [email protected]
123
J. Inst. Eng. India Ser. E (March–August 2012) 93(1):25–30
DOI 10.1007/s40034-012-0003-4
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Azo dyes are widely used by the textile industry, and
due to their complex structure and synthetic origin, are
difficult to decolorize by conventional processes. So, the
wastewater generated is considered as the most polluting
among all industrial sectors [5]. Azo dyes are defined as
compounds that have one –N=N– bond or more in their
structure. These bonds are known as dye chromophore
structure and can provide color through radiant energy
absorption [6]. Reduction of the polluted water coloration
is observed by the –C:C– and –N=N– bond breakage or
by the breakage of the aromatic and heterocyclic rings [7].
UV/TiO2 advanced oxidation process is a promising
technology for removing reactive dyes. TiO2 mediated
photocatalysis have been widely used to destroy organic
pollutants including pharmaceutical compounds and pesti-
cides [8, 9]. Heterogeneous photocatalysis takes advantage
of semiconducting metal oxides that can be used on photo-
assisted reactions either suspended in the water effluent to
be treated, or immobilized on various types of supports.
TiO2-based photocatalysis appears as the most emerging
destructive technology. The key advantage of this method
is that it can be carried out under ambient conditions and
may lead to complete mineralization of organic carbon into
CO2. Moreover, TiO2 photocatalyst is largely available,
inexpensive, non-toxic and shows relatively high chemical
stability. Finally, the TiO2 photocatalytic process, is
receiving increasing attention because of its low cost when
using sunlight as the source of irradiation [10].
Reactor modeling is essential for the application of
heterogeneous photocatalysis on an industrial scale [11].
Modeling and simulation of photocatalytic process is
essential to develop an automated wastewater treatment
plant. In this present study a mathematical model of pho-
tocatalytic reactor have been developed considering L–H
reaction kinetics. The reactor is operating in batch mode;
after each batch TiO2 catalyst was separated and recycled.
Simulation of this BPR was also carried using fourth order
Runge–Kutta and Butcher method (fifth order Runge–Kutta).
Algorithms of these methods are given and C programming
language was used for simulation purpose.
Experimental Methods
The substances that are adsorbed strongly degrade faster
[12], so adsorption was studied to ensure the dye degradation
by photocatalytic reaction on TiO2 surface. Experiments
were conducted with different pH to find the optimum pH for
adsorption. Dark adsorption test of dye on TiO2 surface was
carried out in the Jar Tester manufactured by Phipps and
Bird, Virginia, USA. All of these experiments were con-
ducted in presence of infrared light to prevent any degrada-
tion of dyes by photocatalytic reaction. This test was
conducted at three different pH values (3, 5.5, and 7) with an
initial dye concentration 350 mg L-1. The pH of the solution
(mixture of dye solution and TiO2 adsorbent) was controlled
using 10 M HCl and 10 M NaOH solution. After starting the
experimental run, samples were collected from the Jar Tester
at several times. Then the collected samples were filtered
using 0.45 lm polyethersulfone microfiltration membranes
(Pall, Gelman Laboratory, Michigan) to separate the TiO2
particles. After filtration, the concentration of dye was
measured using a spectrophotometer (Jenway 6505 UV/Vis
spectrophotometer; Dunmow, Essex, UK) at a wavelength
kmax = 516 nm. After completing adsorption test, decolor-
ization test of dyes was carried out in presence of UV ray
illumination. A UV light illuminating bulb (100 W) was
used for this purpose. The experiment was carried out in
batch mode, the schematic of experimental set up is shown in
Figure 1. Samples were collected and filtered as earlier and
concentrations of dyes were measured using an UV–Vis
spectrophotometer. A five cycles experiment was performed
with 350 mg L-1 catalyst concentration and 5 g L-1 initial
dye concentration. Viability of TiO2 recycling was tested
after both adsorption and decolorization test. TiO2 was fil-
tered by 0.45 lm microfiltration membrane after each cycle
and reused to the next cycle.
Results and Discussion
This present study shows that the adsorption and photo-
catalysis depend on many factors viz. pH, TiO2 concen-
tration and time. The details of the effects of all these
parameters are described below.
Fig. 1 Schematic of experimental setup
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Effect of pH on Adsorption
Experimental results show that the dye adsorption strongly
depends on pH. Adsorption is a surface phenomenon and it
depends on adsorbent surface properties. The point of zero
charge of TiO2 (pHpzc) is 6.8; so TiO2 surface becomes
positively charged at pH lower than 6.8 and negatively
charged at pH higher than 6.8 [13]. The reactive dye
RR198 (Figure 2) contains negatively charged sulfonate
groups thus at acidic condition interaction between posi-
tively charged catalyst surface and negatively charged dyes
favour the adsorption. At pH 7 (higher than pHpzc), the
adsorption capacity is very low whereas adsorption
capacity is high at pHs (3 and 5.5) lower than pHpzc; as
shown in Figure 3. This result corroborates that pH 3 is
suitable for industrial application.
Adsorption Isotherm Study
Adsorption isotherms were formed from dark adsorption
experiment data at pH 3. Figure 4 shows that the RR198
adsorption follows Langmuir isotherm (R2 = 0.988)
better than Freundlich isotherm (R2 = 0.957). Values of
Langmuir and Freundlich isotherm constants have been
calculated from the Figure 4.
BPR Model Development
Modeling of a reactor allows obtaining mathematical
expressions for studying the different effects that take place
in it [14]. This paper elucidates a batch reactor within
which a photocatalytic reaction takes place. Experimental
results show that the dye concentration decreases with
time. In a previous paper the authors developed the kinetic
model equation for both photocatalytic reaction and cata-
lyst activity decay. In presence of constant light intensity
the rate of dye decolourization by photocatalytic reaction is
given by [13].
rdecol ¼ k½TiO2�n½Dye�ads ð1Þ
Catalyst activity decreases with increasing time, con-
sidering catalyst activity decay
rdecol ¼ ka½TiO2�n½Dye�ads ð2Þ
Equation (1) is similar to an empirical equation given by
Galindo, et al. [15] and at constant TiO2 concentration:
rdecol ¼ k0a½Dye�ads ð3Þ
It is observed from the isotherm data (Figure 4) that the
Langmuir isotherm fits better than the Freundlich one, and
hence we get:
rdecol ¼ ak0KL½Dye�
1þ b½Dye� ð4Þ
Equation (4) represents the Langmuir–Hinshelwood (L–H)
model equation combined with catalyst activity (a). When
equilibrium dye concentration in liquid phase reaches
almost zero (½Dye� ! 0) then it is assumed that
1 � b[Dye] and Equation (4) becomes:
rdecol ¼ ak0KL½Dye� ð5Þ
The previous study shows that the catalyst decay follows
1st order kinetic.
a ¼ a0e�kadt ð6Þ
Fig. 2 Molecular structure of
RR198
Fig. 3 Dye adsorption at different pH
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Fresh catalyst was used for the study, so the initial
catalyst activity a0 = 1.0. Catalyst deactivation co-efficient
kad was determined from experimental data [13].
Material balance over the batch reactor gives the
following equation:
Rate of accumulation of dye = rate of loss of
dye due to reaction ð7Þ
dcA
dt¼ �W
VkrcAa0e�kadt ð8Þ
Developed final problem is an initial value problem
which can be solved by fourth and fifth order Runge–Kutta
method.
Simulation of BPR
Equation (8) represents the mathematical model of the
BPR. Many parameters are required for simulation pur-
pose. Values of those parameters are given in Table 1. The
apparent kinetic constants are taken from the previous
study [13] where catalyst concentration in the BPR was
5 g L-1. The apparent kinetic constant has a dependence
on catalyst concentration which is described by an
adsorption model [16]. C programming language was used
for computer simulation.
Algorithm of RK4 Method
Simulation of the BPR by fourth order Runge–Kutta
requires the following steps:
Step 1: Define the function f t; cAð ÞStep 2: Enter the initial condition cA0; t0
Step 3: Enter the values of the parameter kr; kad; a0; V ; W
Step 4: Enter the value of tn; h
Step 5: Calculate K1; K2; K3; K4 and KRK4 according to
following formula
K1 ¼ f t0; cA0ð Þ
K2 ¼ f t0 þh
2; cA0 þ
K1
2
� �
K3 ¼ f t0 þh
2; cA0 þ
K2
2
� �
K4 ¼ f t0 þ h; cA0 þ K3ð Þ
and
KRK4 ¼ K1 þ 2K2 þ 2K3 þ K4ð Þ=6
Step 6: Calculate cA1 ¼ cA0 þ KRK4 � h
Step 7: Calculate t1 ¼ t0 þ h
Fig. 4 Adsorption isotherm at
pH 3
Table 1 Parameters used for BPR simulation
Name of the parameter Value of the parameter
Apparent kinetic constant (kr) 0.35
Catalyst deactivation co-efficient (kad) 0.1034
Initial catalyst activity (a0) 1.0
Volume of the reactor (V) 1.0
Weight of catalyst (W) 5.0
Permissible limit of dye concentration (Cper) As low as possible
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Step 8:cA0 ¼ cA1
t0 ¼ t1
Algorithm of RK5 (Butcher) Method
Fifth order Runge–Kutta method (Butcher method) can be
used to simulate the BPR. Required steps are same as the
RK4 method except Step 5, given below:
Step 5: Calculate K1; K2; K3; K4; K5; K6 and KRK5
according to following formula
K1 ¼ f t0; cA0ð Þ
K2 ¼ f t0 þh
4; cA0 þ h
K1
4
� �
K3 ¼ f t0 þh
4; cA0 þ h
K1
8þ h
K2
8
� �
K4 ¼ f t0 þh
2; cA0 � h
K2
2þ hK3
� �
K5 ¼ f t0 þ3h
4; cA0 þ h
3K1
16þ h
9K4
16
� �
K6 ¼ f t0 þ h; cA0 � h3K1
7þ h
2K2
7þ h
12K3
7� h
12K4
7
�
þh8K5
7
�
and
KRK5 ¼ 7K1 þ 32K3 þ 12K4 þ 32K5 þ 7K6ð Þ=90
Effect of Step Size
Step size h has an effect on real time simulation; increasing
h increases accuracy but takes more time for simulation.
For real time simulation, simulation time should be less
than process time. Sometimes stability of the solution
depends on the step size. In this present paper three
different step sizes (0.1, 0.5 and 1) were considered.
Figures 5 and 6 giving an idea about the simulated
results with different step size using RK4 and RK5 method
simultaneously. This result shows that simulation with step
size 0.5 is considerable for real time simulation, because
accuracy and simulation time both are good. Figure 7
shows a comparison between RK4 and RK5 method with
0.5 step size. It is clear from this comparison that RK5
(Butcher) method is more suitable than RK4 method.
Calculation of Batch Time
Determination of batch time is a vital job for economic
plant operation. Calculation of proper batch time optimizes
the throughput of the process. Algorithm for batch time
determination is given below:
Step 1: Define the function f t; cAð ÞStep 2: Enter the initial condition cA0; t0
Step 3: Enter the values of the parameter kr; kad; a0;
V; W
Step 4: Enter the value of permissible limit Cper and step
size h
Step 5: Calculate K by RK5 method
Step 6: Calculate cA1 ¼ cA0 þ K � h
Step 7: If cA�Cper, stop
Since RK5 method shows better results, it is used in
‘Step 5’ during batch time calculation.
Fig. 5 Experimental result versus simulation results for RK4 method
Fig. 6 Experimental result versus simulation results for RK5 method
Dynamic Simulation of BPR for Wastewater Treatment 29
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Conclusion
The present study depicts the way of developing an auto-
mated wastewater treatment plant by advanced oxidation
process (TiO2/UV). The results show that within 30 min,
almost 100 % RR198 dye removal is possible using BPR.
This study also shows that simple RK4 and RK5 method
can be used for simulation of this BPR. Simulated results
show RK5 method follows experimental data better com-
pared to RK4. Optimum step size 0.5 gives good result and
taking less simulation time.
Acknowledgments A part of this study was carried out at Centre for
Water Science (Formerly School of Water Sciences), Cranfield
University, Cranfield, Bedfordshire, MK43 OAL, UK under British
Council Higher Education Link Programme. The authors would like
to express thanks to the British Council for financial support.
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Fig. 7 Fourth Runge–Kutta against fifth order Runge–Kutta
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