5.2
Impact Factor
Generic selectors
Exact matches only
Search in title
Search in content
Post Type Selectors
Search in posts
Search in pages
Filter by Categories
Corrigendum
Current Issue
Editorial
Erratum
Full Length Article
Full lenth article
Letter to Editor
Original Article
Research article
Retraction notice
Review
Review Article
SPECIAL ISSUE: ENVIRONMENTAL CHEMISTRY
5.3
Impact Factor
Generic selectors
Exact matches only
Search in title
Search in content
Post Type Selectors
Search in posts
Search in pages
Filter by Categories
Corrigendum
Current Issue
Editorial
Erratum
Full Length Article
Full lenth article
Letter to Editor
Original Article
Research article
Retraction notice
Review
Review Article
SPECIAL ISSUE: ENVIRONMENTAL CHEMISTRY
View/Download PDF

Translate this page into:

ORIGINAL ARTICLE
12 (
8
); 3054-3063
doi:
10.1016/j.arabjc.2015.07.004

Implementation of a venturi photocatalytic reactor: Optimization of photodecolorization of an industrial azo dye

Laboratoire de l'ingénierie et des procédés de l'environnement LIPE, Faculty of pharmaceutical process engineering, Constantine 3 university, 25000 Constantine, Algeria

⁎Corresponding author. Tel.: +213 551680294. chem.engd@gmail.com (Mohammed Berkani),

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.
Tel.: +213 667441013.

Abstract

The photocatalytic decolorization of the textile azo dye C.I. Basic Red 46 was studied in a semi-pilot photocatalytic reactor combined with an emulsion venturi. The venturi has two principal roles, bring dissolved oxygen necessary for the photocatalytic reaction, and ensure a good homogenization, within its divergent, of the mixture dye solution-air-TiO2 particles. This study shows that this proposed photoreactor can be easily applied and extrapolated in photocatalysis reactions with a significant performance.

The optimization of UV/TiO2 process in the photoreactor was carried out using the response surface methodology (RSM), based on the central composite design (CCD), to assess individual and interactive effects of the four main independent parameters (initial dye concentration, concentration of TiO2, flow rate (QL) and initial (pH) on the decolorization Efficiency Y (%) of (BR46)). Experimental results found from RSM was in good agreement with the model prediction (R2 = 0.96 and Adj-R2 = 0.92) and the presence of venturi has increased the discoloration rate of 20%. The optimization results showed that maximum decolorization efficiency was achieved at the optimum conditions: pH 8.68, TiO2 = 0.97 g/L, QL 1324 L h−1, [RB46] 5 mg L−1.

Keywords

Photocatalysis
Photoreactor
Venturi
Response surface methodology (RSM)
Basic Red 46
Central composite design (CCD)
1

1 Introduction

A successful implementation of photocatalysis requires very efficient catalysts, illumination sources, a strong oxidizing agent in most cases oxygen and adapted reactors at the process (Orozco et al., 2009; De Lasa et al., 2005), thus the design of photocatalytic reactors is a new interesting research area (Li Puma and Lock Yue, 2003). Indeed, since the emergence, these last thirty years of photocatalysis, new semi-pilot reactor for the treatment of water and air has been widely developed (Salaices et al., 2004; Zhang et al., 2011; Buechler et al., 1999; McCullagh et al., 2010; Ibrahim and de lasa, 2002). Recently, airlift reactors were used as photobioreactors (Acién et al., 2001; Loubière et al., 2009; Arbib et al., 2013; Yuan et al., 2011; Degen et al., 2001). In photocatalysis process dissolved oxygen reduces the risk of recombination hole/electron as electron scavenger; hence, providing continuous oxygen to the system ensures that the reaction limiting step is not the lack of oxygen (Chong et al., 2010). However, the amount of dissolved oxygen required is not very high, so to limit the costs, processes giving a great transfer gas–liquid must be avoided and air should be used instead pure oxygen. In the present work we show the performances of new developed semi-pilot photoreactor equipped by an emulsion venturi. The air is self-aspired in the venturi throat by kinetic energy action of liquid recirculation with a low gas flow (QG/QL < 1), that is suitable for the photocatalytic process which does not require large quantities of oxygen. The liquid gas dispersion formed in the divergent part of the venturi causes a good oxygen transfer and a good homogenization of the liquid- solid–gas mixture (dye solution-TiO2-air). The bioreactors equipped with emulsion venturi have many potential applications and tend more and more to replace the mechanically stirred reactors, especially in bioconversion processes (Gourich et al., 2005; Khellaf et al., 2014; Bouhelassa and Zoulalian, 1995a,b). The organic compound degradation by photocatalysis is highly dependent on a number of the operation parameters (pH, temperature, amount of catalyst, UV irradiation time, light intensity, initial pollutants concentration) and reactor technology (implementation of photocatalyst, oxygen transfer, agitation, flow of gas and liquid). The high number of influential variables makes the use of suitable experimental design attractive, in order to optimize the influence of this parameters, the application of factorial experimental design can be used as a powerful tool in the development of any photocatalytic process, among these experimental designs, we can find the central composite design CCD which is a widely used form of response surface methodology (RSM), this efficient technique applied to optimize the response surface influenced by various process parameters and to quantify the relationship between the controllable input parameters and the obtained response surfaces (Khataee et al., 2010; Kwak, 2005; Merabet et al., 2009). Moreover, the main advantage of RSM is the reduced number of experimental trials needed to evaluate multiple parameters and their interactions with a large number of factors and levels (Karacan et al., 2007).

To evaluate the performance of our photoreactor, we studied the photocatalytic degradation of an azo dye known as Basic Red 46 (BR46), by TiO2 P25 powder. Also we developed a simulation model using factorial design methodology based on the central composite design (CCD) in order to optimize four independent parameters: the concentration of TiO2, initial pH, initial dye concentration and the flow rate in the photocatalytic degradation process of an aqueous solutions containing an azo dye Basic Red 46 (BR46).

2

2 Photocatalytic process

In the photocatalytic UV/TiO2 process system, the photonic excitation of a semiconductor such as TiO2 produces electron–hole pairs in the surface of semiconductors. The highly oxidative h VB + can react with surface bound H2O to produce hydroxyl radicals OH° or can directly react with the organic molecules (Da Silva and Faria, 2003): TiO 2 + h υ e CB - + h VB + Dye + OH ° degradation product Dye + TiO 2 ( h VB + ) oxidation product Dye + TiO 2 ( e CB - ) reduction product

3

3 Materials and methods

3.1

3.1 Chemicals and materials

The textile dye, Basic Red 46 (BR46, commercial name Astrazon Red FBL) was obtained from Aurassienne Spinning and Blankets (SAFILCO) Company, Algeria (molecular formula = C18N6H21, color index number = 110,825, λmax = 531 nm, Mw = 357.5 g/mol, azo group one, type cationic). Titanium dioxide powder used is TiO2 Degussa P25 with greater than 99.5% purity (average primary particle size: 21 nm, BET surface area: 50 ± 15 m2/g). Initial pH of the aqueous solutions was adjusted by both sulfuric acid and sodium hydroxide.

3.2

3.2 The photocatalytic reactor

The first objective was to highlight the device ability for the implementation of photocatalytic reactions. The photocatalytic reactor is combined to an emulsion venturi operating in self-aspiration, on a recirculated boucle shown in Fig. 1 which consists of four main parts:

  • An emulsion venturi, consisting of a convergent and divergent separated by a throat diameter of 11 mm (Fig. 1). The diameters of the convergent and the divergent are similar and equal to 58 mm at the inlet and the outlet of the venturi. The device operates according to the Bernoulli energy conservation of a fluid, principle: In the constricted portion at the collar, the kinetic energy of fluid increases and the static pressure decreases. When the flow reaches a given value (between 400 and 500 L/h in our case see Fig. 2), the static pressure decreases below the atmospheric pressure. The external air is then self-aspired at the venturi throat through four symmetrically radial orifices. The liquid gas dispersion formed in the divergent causes a good oxygen transfer and a good homogenization of the liquid- solid–gas mixture (dye solution-TiO2-air). Indeed, it is well known that the role of dissolved oxygen in photocatalytic process is to prevent the recombination of holes/electron pair formed in the semiconductor surface.

  • Such a venturi is characterized by a ratio QG/QL < 1, this is suitable for the photocatalytic field, which does not require large quantities of oxygen. Such a device has been applied in aerobic biological processes. (Khellaf et al., 2014; Bouhelassa and Zoulalian, 1995a,b).

  • A cylindrical Pyrex Glass reactor (length: 700 mm, external diameter: 58 mm, thickness: 1.4 mm) made in Germany (Schott–Rohrglas GmbH Company) and delivered by SOMIVER (E.N.A.V.A) Company Algeria, The volume effectively irradiated was 1.584 L and the volume of colored water to be treated was 10 L. The reactor is irradiated by four UV-light lamps NARVA UV 010 (λ = 365 nm UV-A) to achieve a higher efficiency of photon, the distance between the lamps and the reactor wall was fixed at 35 mm The photoreactor and lamps were completely covered with an UV opaque cylinder in which the temperature is maintained constant by a controlled cooling air using adapted ventilators.

  • A recirculation loop includes a 25 l tank and a centrifuge pump fitted. The liquid recirculation flow rate can be controlled using a calibrated rotameter (CITEC DFM 200) placed between the pump outlet and the reactor inlet.

  • An air circuit mounted around of the venturi throat, perforated with four orifices through which, air is aspired, its flow rate is measured by a gas flowmeter (Rhone Duisburg GERMANY 07/96).

Schematic representation of Emulsair photocatalytic reactor.
Figure 1
Schematic representation of Emulsair photocatalytic reactor.
Variation of the flow rate ratio QG as a function of QL for different concentrations of BR46.
Figure 2
Variation of the flow rate ratio QG as a function of QL for different concentrations of BR46.

3.3

3.3 Experimental design

The second main objective was to determine the optimum operating conditions for a given system that satisfies the specific operating conditions, the application of statistical experimental design reduced process variability combined with the requirement of less resources (time, reagents and experimental work), Response surface methodology (RSM) allows to solve multivariable equations and evaluate simultaneously the relative significance of several affecting factors even in the presence of complex interaction (Wu et al., 2010). RSM based on central composite design (CCD) was applied for optimization of photocatalytic decolorization process, consisting of 29 experiments for four variables (n = 4) and two levels low (−) and high (+). The total number of experiments was 29 determined by the expression: 2n (24 = 16: factor points) + 2n (2 × 4 = 8: axial points) + 5 (center points: five replications), as shown in Table 3. The parameters in the design were studied at five different levels (−2, −1, 0, 1, 2), also the test factors were coded according to following Eq. (A.1):

(A.1)
x i = X i - X i 0 Δ X where xi is the coded value of the ith independent variable, Xi the natural value of the ith independent variable, Xio the natural value of the ith independent variable at the center point, and ΔX is the step change value (Cho and Kyung, 2007).

The central composite design is based on a mathematical model which related the response Y to factors X1, X2, …, Xi, …, Xn, was employed for optimization of this process and the second-order polynomial response equation to correlate the dependent and independent variables: Eq. (A.2)

(A.2)
Y ( Decolorization efficiency ) = a 0 + a 1 X 1 + a 2 X 2 + a 3 X 3 + a 4 X 4 + a 12 X 1 X 2 + a 13 X 1 X 3 + a 23 X 2 X 3 + a 14 X 1 X 4 + a 24 X 2 X 4 + a 34 X 3 X 4 + a 11 X 1 2 + a 22 X 2 2 + a 33 X 3 2 + a 44 X 4 2

The statistical software MINITAB (16 Minitab Institute, USA) was used to fit the experimental data to the second-order polynomial equation.

3.4

3.4 Analysis

All the collected samples from the experiments were centrifuged at 4000 rpm for 25 min using a centrifuge (sigma 2–16) to remove the TiO2 and color removal of the dye BR 46 was determined by UV absorption at λmax = 365 nm using a UV–vis spectrophotometer (Shimadzu UV-160A) and calibration curve. The yield of decolorization (Y (%)) was expressed as the percentage ratio of decolorized dye concentration to that of the initial one.

The mineralization monitoring is carried out by the TOC measurement using a total carbon analyzer (V-CPH SHIMADZU).

4

4 Results and discussions

4.1

4.1 Self-aspiration capacity

The influence of liquid flow on self-aspiration capacity of venturi was studied by varying the liquid flow (QL) between 500 and 1500 L/h. According to Bernoulli’s principle, when the liquid is pumped, at a high velocity, a low pressure is created in the venturi throat.

For the selected values of QL, the air was self-aspired in the venturi throat when the liquid pressure was lower than the atmospheric pressure (Table 1).

Table 1 Pressure and velocity at the venturi throat according to the recirculation liquid flow QL.
QL (L/h) 500 700 800 900 1000 1100 1200 1300 1400
P (Pa) 92,337 90,114 88,514 87,315 86,115 84,116 82,516 80,651 78,918
UC (m/s) 1.46 2.04 2.34 2.63 2.92 3.22 3.51 3.80 4.09

The effect of QL on self-aspiration capacity of the reactor was studied by representing in (Fig. 2) the variation of QG with respect to QL, in both clear water and charged with BR46 dye. The self-aspired air increased by increasing QL. Additionally, Experimental results presented show that the increase in air flow (QG) is more marked in the case when the recirculation liquid is charged with BR46 (15–45 mg/L). This phenomenon is probably due to the decrease in surface tension of the solution (Fig. 3) whose consequence is the decrease in bubble size due to the inhibition of the coalescence, which corresponds to the increase in the exchange surface-to-volume liquid ratio (Khellaf et al., 2014; Bouhelassa and Zoulalian, 1995a).

Variation of the surface tension of solution with BR46 concentration (mg L−1).
Figure 3
Variation of the surface tension of solution with BR46 concentration (mg L−1).

The measurement of the surface tension (σ) of the solution for different concentrations of BR46 shown in (Fig. 3) has been performed using a tensiometer (KRUSS K8).

The variation of the surface tension (σ) as a function of dye concentration reveals that textile dyes reduce the surface tension of water, and this facilitates the formation of bubbles by reducing the energy required to create air–water contact surfaces, the obtained results are similar to those found by (Mazet et al., 1990) during a study concerning the removal of an industry textile dyes by wood sawdust.

On the other hand, it can be assumed that the friction loss created in contactor throat becomes lower in the presence of colored liquid and this effect leads to high flows of self-aspired air.

4.2

4.2 Photolysis and photocatalysis

To make a clear comparison in the efficiency of the photolysis under UV irradiation only and photocatalytic process (Fig. 4), two tests were carried out in the same operating conditions: pH (original) = 6.8, C0 = 16 mg L−1, [TiO2]0 = 0.5 g L−1, QL = 1200 L h−1, QG (self-aspired) = 365 L h−1.

Photodecolorization of BR46 as a function of time (pH (natural) = 6.8, C0 = 15 mg L−1, [TiO2]0 = 0.5 g L−1, QL = 1200 L h−1, QG (self-aspired) = 378 L h−1, QG/QL = 0.315).
Figure 4
Photodecolorization of BR46 as a function of time (pH (natural) = 6.8, C0 = 15 mg L−1, [TiO2]0 = 0.5 g L−1, QL = 1200 L h−1, QG (self-aspired) = 378 L h−1, QG/QL = 0.315).

It was observed that only 10% of decolorization was achieved after 150 min in the absence of the catalyst (photolysis). However, in the presence of TiO2 Degussa P25 (0.5 g L−1), it can be seen that 86% of BR46 is degraded after 150 min of irradiation. Note that for the experience of photocatalysis, the UV lamps were kept off during 30 min to achieve the adsorption equilibrium and then they were turned on.

4.3

4.3 Photocatalytic mineralization of BR46

Photocatalytic mineralization of the dye in UV/TiO2 process was studied and monitored by TOC loss at the end of the photocatalytic process of BR46 solution (Fig. 5). TOC removal indicating the ultimate oxidation of BR46 was much slower than decolorization. The complete decolorization of BR46 occurred in 150 min, and thus it requires more than 400 min to reach the complete mineralization. This might be due to the formation of intermediates in BR46 solution with main dye molecules. TOC removal efficiency (Fig. 8) was determined as 93% at initial dye concentration of 15 mg/L, pH = 6.8, [TiO2]0 = 0.5 g L−1, QL = 1200 L h−1.

TOC removal efficiency of BR46.
Figure 5
TOC removal efficiency of BR46.

4.4

4.4 Effect of emulsion venturi flow rate ratio

The oxygen resulting from the self-aspirated air by emulsion-venturi and the gas–liquid dispersion created in its divergent improve the photocatalysis process (Fig. 5); thus, the suspension homogenization (liquid–air–TiO2) is favored and the transfer of oxygen is enhanced by the bubbles generated in the divergent section by the kinetic energy increase in the venturi throat. The recombination phenomenon of electron/hole pair is thus reduced. Otherwise oxygen captured by conduction band electron serves to form radicals such as O°2 to give added photocatalytical effect. It has been shown that the degradation and mineralization rate constants increased with the dissolved oxygen concentration (Tseng et al., 2012). Several experiments also have shown that when all the oxygen in the system has been consumed, the process stops. However, their reinjection into medium has allowed restarting again the reaction (Piscopo et al., 2001).

The self-aspired gas flow rate is strongly influenced by the liquid flow rate; also it is more logical to consider the ratio (QG/QL). To evaluate the influence of this ratio on the rate of BR46 decolorization, several experiments were carried out at the same conditions of typical data for BR46 decolorization with initial concentration of [TiO2]0 = 0.5 g L−1 at pH 6.8. The obtained results are summarized in Table 2.

Table 2 Values of flow rate ratio (QG/QL) and yield of decolorization (Y %) on 150 min of irradiation.
[BR46]0 (mg L−1) QL (L h−1) QG/QL Y (%)
15 735 0.215 66.70
1200 0.315 86.05
35 735 0.231 49.21
1200 0.317 65.78

Experimental results have proved that decolorization yield Y (%) of BR46 rises progressively as the flow rate ratio (QG/QL) increases at the same conditions and, could attain a yield of Y = 86.04% at high flow rate ratio.

4.5

4.5 Experimental design methodology and analysis of variance (ANOVA)

In this work, RSM was applied to assess individual and interactive effects of the four main independent parameters (initial dye concentration, concentration of TiO2, flow rate and initial pH) on the decolorization efficiency Y (%) of BR46, the experimental ranges and the levels of the independent variables for BR46 removal are given in Table 3.

Table 3 Range and levels of experimental parameters.
Variables Ranges and levels
−2 −1 0 +1 +2
pH (X1) 2 4.5 7 9.5 12
Initial dye concentration (mg L−1) (X2) 5 15 25 35 45
Concentration of TiO2 (g L−1) (X3) 0.2 0.325 0.55 0.775 1
Flow rate (L h−1) (X4) 500 735 970 1205 1440

The four-level CCD design matrix and the experimental results obtained in the photocatalytic decolorization are presented in Table 4, which shows the statistical combinations of independent variables pH (X1) Initial dye concentration (mg L−1) (X2) concentration of TiO2 (g L−1) (X3) flow rate (L h−1) (X4) with the yield Y (%) (measured) was predicted over a period of 150 min. These predicted values are very close to the observed ones in all set of experiments.

Table 4 CCD design matrix for four test variables in coded units along with the observed and predicted responses.
Run PH C (mg L−1) [TiO2] (g L−1) QL (L h−1) Decolorization efficiency Y (%)
Experimental Predicted
1 −1 −1 −1 −1 57.33 55.46
2 +1 −1 −1 −1 49.80 53.30
3 −1 +1 −1 −1 46.89 51.83
4 +1 +1 −1 −1 50.11 47.67
5 −1 −1 +1 −1 66.70 70.39
6 +1 −1 +1 −1 81.64 80.71
7 −1 +1 +1 −1 44.62 43.61
8 +1 +1 +1 −1 50.32 51.92
9 −1 −1 −1 +1 52.80 57.34
10 +1 −1 −1 +1 55.94 56.87
11 −1 +1 −1 +1 61.97 62.82
12 +1 +1 −1 +1 57.90 60.35
13 −1 −1 +1 +1 72.89 75.26
14 1 −1 +1 +1 86.05 87.26
15 −1 +1 +1 +1 54.94 57.58
16 +1 +1 +1 +1 65.78 67.58
17 −2 0 0 0 87.67 82.61
18 +2 0 0 0 91.49 90.45
19 0 −2 0 0 54.10 52.40
20 0 +2 0 0 31.48 29.09
21 0 0 −2 0 53.60 50.17
22 0 0 +2 −2 75.00 72.34
23 0 0 0 +2 48.40 47.68
24 0 0 0 0 70.60 65.23
25 0 0 0 0 55.70 52.73
26 0 0 0 0 53.96 52.73
27 0 0 0 0 52.60 52.73
28 0 0 0 0 51.33 52.73
29 0 0 0 0 50.10 52.73

Based on these results, an empirical relationship between the response and independent variables was attained and expressed by the following second–order polynomial equation (Eq. (C)):

(C)
Y = 52.738 + 1.96 X 1 - 5.8275 X 2 + 5.5416 X 3 + 4.3858 X 4 - 0.5012 X 1 X 2 + 3.1175 X 1 X 3 - 5.78876 X 2 X 3 + 0.4212 X 1 X 4 + 2.2775 X 2 X 4 + 0.7437 X 3 X 4 + 8.45 X 1 2 - 2.9974 X 2 2 + 2.13 X 3 2 + 0.93 X 4 2

Analysis of variance (ANOVA) study (Table 5) shows the results of the quadratic response surface model. ANOVA is required to test the significance and adequacy of the model. The ratio between the mean square of the model and the residual error is presented by the Fisher variation ratio F-value which is a statistically valid measure of how well the factors describe the variation in the data about its mean (Liu and Chiou, 2005). If the model is a good predictor of the experimental results, F-value should be greater than the tabulated value of F-distribution for a certain number of degrees of freedom in the model at a level of significance α. The high significant of the model is performed by (F-value = 24.02) which is much greater than the tabular F-value (F tabular = 3.48), indicating that the treatment differences are highly significant, F-value also indicates the variation from the model is significant or not when compared with the ones associated with residual error (Khataee et al., 2010). The quality of fitting the second-order equation was expressed by the coefficient of determination R2. The R2-values provide a measure of how much variability in the observed response values can be explained by the experimental factors and their interactions. The R2-value is always between 0 and 1. The closer the R2-value is to 1, the better the model predicts the response (Liu and Chiou, 2005). It was found that the predicted values matched the experimental values reasonably well with R2 = 0.96 and this implies that 96% of the variations for percent color removal are explained by the independent variables (Table 5). Adjusted R2 (Adj-R2) is also a measure of goodness of a fit and corrects the determination coefficient R2-value for the sample size and the number of terms in the model. In this study the value of Adj-R2 (0.9202) is very close to the corresponding R2 value (Table 5).

Table 5 Analysis of variance (ANOVA) for fit of decolorization efficiency from central composite design.
Source of variations Sum of squares Degree of freedom Adjusted mean square F-value
Regression 5361.71 14 382.98 24.02
Residuals 223.23 14 15.94
Total 5584.94 28

R2 = 96%, Adj-R2 = 0.9202. F-value = 24.02 ≫ F0.05 (14, 14) tabular = 3.48.

Table 6 summarizes the estimates of regression coefficients accompanied with their standard errors, t-statistics and the corresponding p-values.

Table 6 Regression results from the data of central composite design experiments.
Coefficient Parameter estimate Standard error t-Value P-value
Intercept 52.7380 1.7858 29.532 0.000
X1 1.9600 0.8151 2.405 0.031
X2 −5.8275 0.8151 −7.150 0.000
X3 5.5417 0.8151 6.799 0.000
X4 4.3858 0.8151 5.381 0.000
X1X1 8.4501 0.7839 10.779 0.000
X2X2 −2.9974 0.7839 −3.824 0.002
X3X3 2.1301 0.7839 2.717 0.017
X4X4 0.9301 0.7839 1.186 0.255
X1X2 −0.5012 0.9983 −0.502 0.623
X1X3 3.1175 0.9983 3.123 0.007
X1X4 0.4212 0.9983 0.422 0.679
X2X3 −5.7888 0.9983 −5.799 0.000
X2X4 2.2775 0.9983 2.281 0.039
X3X4 0.7438 0.9983 0.745 0.469

P-values were used as a tool to check the significance of each of the coefficients, which in turn, are necessary to understand the pattern of the mutual interactions between the test variables. The larger the magnitude of the Student’s t-test and smaller P-value, the more significant is the corresponding coefficient (Liu and Chiou, 2005).

The probability value (P) of coefficients was greater than 0.05, indicating the term did not have a significant effect on the predicted response (Jiang et al., 2013). Based on obtained results Table 6, P-value is relatively low, indicating the significance of the model, we can affirm that initial dye concentration (mg L−1) (X2), concentration of TiO2 (g L−1) (X3), and flow rate (L h−1) (X4) with P values smaller than 0.0001 for 95% confidence level implied that terms were significant. Also pH (X1) had a slightly negative effect with (p-value < 0.031). Moreover quadratic effects, shows that dye concentration presents a negligible P-value (p-value 0.002), indeed the mutual between dye concentration and TiO2 loading (p-value < 0.0001) and pH solution with TiO2 concentration (p-value < 0.007) are significant comparing to others factors.

The major diagnostic plots (Fig. 6) are used also to evaluate the residual analysis (difference between the observed and the predicted response value) of the response surface design, ensuring that the statistical assumptions fit the analysis data. Normal probability plots of the residuals are a suitable graphical method to verify whether the standard deviations between the actual and the predicted response values follow a normal distribution. The results illustrated in (Fig. 6) convey the general impression of a normal distribution of underlying errors, since the residuals fall near to a straight line; thus, there is no clear indication of non-normality of experimental results. Based on this plot, the residuals appear to be randomly scattered; thus, the model proposed is adequate and the constant variance assumption is confirmed.

Variation of RB46 concentration as a function of time in photocatalysis with and without Venturi (PH = 6.8, C0 = 15 mg L−1, [TiO2]0 = 0.5 g L−1, QL = 1440 L h−1, QG self-aspired = 385 L h−1, QG/QL = 0.267).
Figure 6
Variation of RB46 concentration as a function of time in photocatalysis with and without Venturi (PH = 6.8, C0 = 15 mg L−1, [TiO2]0 = 0.5 g L−1, QL = 1440 L h−1, QG self-aspired = 385 L h−1, QG/QL = 0.267).

4.6

4.6 Effect of variables as response surface

The main objective of the optimization is to determine the optimum values of variables for photocatalytic decolorization process, from the model obtained using experimental data.

Response surfaces shown in (Fig. 7) provide the results of the interaction between factors which are more significant.

Residual plots for photocatalytic decolorization efficiency of BR46.
Figure 7
Residual plots for photocatalytic decolorization efficiency of BR46.

Fig. 8(1) shows the effects of catalyst concentration and initial dye concentration for flow rate of 970 L h−1 and initial pH = 7 at high levels of dye concentration in parallel with TiO2 loading, the decolorization efficiency of the dye decreases as the concentrations increases in this case the photons got intercepted before they could reach the catalyst surface which decreases the color removal of BR46, likewise at very low concentrations of dye and catalyst, the response surface does not present any significant photodegradation due to the adherence of catalyst particles to the system walls, including to some non-illuminated sections.

The response surface plots of photocatalytic decolorization efficiency Y (%) by the interaction between, (1) Initial dye concentration BR46 (mg L−1) and TiO2 concentration (g L−1), (2) Initial dye concentration BR46 (mg L−1) and flow rate QL (L h−1) and (3) pH of solution and TiO2 concentration (g L−1).
Figure 8
The response surface plots of photocatalytic decolorization efficiency Y (%) by the interaction between, (1) Initial dye concentration BR46 (mg L−1) and TiO2 concentration (g L−1), (2) Initial dye concentration BR46 (mg L−1) and flow rate QL (L h−1) and (3) pH of solution and TiO2 concentration (g L−1).

Additionally, the optimum catalyst loading for photodegradation is varied, and mainly depends on the dimension of the photoreactor (De Lasa et al., 2005).

In contrast, it should be noted that with decreasing the initial concentration of dye, the photocatalytic decolorization efficiency provides very significance results.

Fig. 8(2) represents the photocatalytic decolorization efficiency as a function of flow rate and initial dye concentration at catalyst concentration of 0.55 g L−1 and initial pH of 7. The figure shows that the increase in decolorization efficiency Y (%) of BR46 was caused by an increase in flow rate at the higher values of the initial dye concentration and by a decrease in recirculated liquid flow at the lower values of the initial dye concentration. The presumed reason is that when the recirculated liquid flow is increased, the turbulence in the system is enhanced which ensures better dispersion of particles (BR46 and TiO2) in the solution inside the reactor. It may lead to decompose more and more adsorbed dye molecules on the surface of TiO2 and thus photocatalytic decolorization efficiency increases. The higher decolorization efficiencies at higher flow rates were also attributed to the increase in the mass transfer coefficient. (Dijkstraa et al., 2002) In the case of low flow the solution is more exposed to lamp irradiation which improves the formation of hydroxyl radicals (OH) and this leads to increasing in degradation efficiency.

The degradation efficiencies of dyes were observed in high levels at acidic solution, and it was also effective under alkaline condition as a function of increasing on TiO2 loading (Fig. 8(3). BR46 is a cationic dye thus, in acidic medium the repulse force inhibiting the adsorption of dye molecule in the catalyst surface. But the formation of hydroxyl radicals remains possible which react with dye molecule, in basic medium, hydroxyl radicals were also produced on the catalyst surface by the following reaction (Eq. (D)) (Gozmen et al., 2009):

(D)
TiO 2 ( h VB + ) + OH ( ads ) - OH High pH favors adsorption on the catalyst surface which results in high decolorization efficiency (Jiang et al., 2008).

5

5 Optimal conditions for decolorization of BR46

From analysis of our model Eq. (C) with a statistical technique within Minitab 16 software, the process optimum values for the maximum decolorization efficiency were 0.97 g/L, 5 mg L−1, 1324 L h−1 and 8.68 for catalyst concentration (X1), initial dye concentration (X2), flow rate (X3) and initial pH (X4), respectively. At these optimum values, the predicted and observed Y (%) was 100% and 98.5%, respectively. After verifying by a further experimental test with the predicted values, the result indicates that the maximal decolorization efficiency was obtained when the values of each parameter were set as the optimum values, which is in good agreement with the predicted value from the regression model. It implies that the strategy to optimize the decolorization conditions and to obtain the maximal decolorization efficiency by RSM for the photocatalytic degradation of the dye Basic Red 46 in this study is successful. Furthermore, this study is a way to optimize such a photoreactor and will enable to apply in this device, a specific treatment for a real water obtained from Aurassienne Spinning and Blankets (SAFILCO) Company, Algeria, charged by the dye, C.I. Basic Red 46 by imposing the optimization results.

6

6 Conclusions

The photocatalytic decolorization of the textile dye C.I. Basic Red 46 was studied in the photocatalytic reactor combined with a venturi, the emulsion venturi provides low amounts of air which are suitable and sufficient in the photocatalytic decolorization of BR46. The photodecolorization of BR46 was performed successfully in the photoreactor, and it was found that at high flow rate ratio (QG/QL) the BR46 photodecolorization presents a significant performance. The optimization and the modeling of photocatalytic degradation were performed by using a composite experimental design, the experimental values agreed with the predicted ones, indicating suitability of the model employed and the success of RSM in optimizing the conditions of photocatalysis. Based on analysis of variance (ANOVA) indicating a high coefficient of determination (R2 = 96%, Adj-R2 = 0.9202), the predicted values of decolorization efficiency were found to be in good agreement with experimental values.

The presented device enables all the technological aspects required for the photocatalytic process indeed:

  • The necessary dissolved oxygen is provided by the air self-aspired in the venturi throat by the increase in kinetic energy and decrease in static pressure of liquid recirculation.

  • The liquid gas dispersion formed in the divergent part of the venturi causes a good oxygen transfer and a good homogenization of the liquid-solid–gas mixture (pollutant-solution-TiO2–air).

  • The UV lamps and the implementation of photocatalyst (fixed or slurry) can be adapted easily on the recirculation loop.

  • The flow of gas and liquid can be perfectly optimized.

Also, we think that such a device is perfectly integrated for a photocatalysis operation and can be easily extrapolated for a specific treatment of water containing recalcitrant pollutants to conventional treatment. (Water discharges from textile plants, detergents, pharmaceutical products, …).

Acknowledgments

This work was supported by Professor Mohammed Bouhelassa and the experimental setup mounted by Mohammed Mokhtar Bouchareb (Plumbing and Central Heating Company. Algeria). The authors gratefully acknowledge financial support from the Constantine University 3.

References

  1. , , , , . Airlift-driven external-loop tubular photobioreactors for outdoor production of microalgae: assessment of design and performance. Chem. Eng. Sci.. 2001;56:2721-2732.
    [Google Scholar]
  2. , , , , , , . Long term outdoor operation of a tubular airlift pilot photobioreactor and a high rate algal pond as tertiary treatment of urban wastewater. Ecol. Eng.. 2013;52:143-153.
    [Google Scholar]
  3. , , . Dimensionnement d’un bioréacteur «Emulsair». Entropy. 1995;188(189):47-53.
    [Google Scholar]
  4. , , . Hydrodynamics and gas-liquid transfer in a bioreactor of type «Emulsair» operating in self suction. Entropy. 1995;188(189):39-45.
    [Google Scholar]
  5. , , , , , . Design and evaluation of a novel controlled periodic illumination reactor to study photocatalysis. Ind. Eng. Chem. Res.. 1999;38:1258-1263.
    [Google Scholar]
  6. , , . Photocatalytic degradation of azo dye (Reactive Red 120) in TiO2/UV system: optimization and modeling using a response surface methodology (RSM) based on the central composite design. Dyes Pigm.. 2007;75:533-543.
    [Google Scholar]
  7. , , , , . Recent developments in photocatalytic water treatment technology: a review. Water Res.. 2010;44:2997-3027.
    [Google Scholar]
  8. , , . Photochemical and photocatalytic degradation of an azo dye in aqueous solution by UV irradiation. J. Photochem. Photobiol. A Chem.. 2003;155:133-143.
    [Google Scholar]
  9. , , , . Photocatalytic Reaction Engineering. Western Ontario: Springer; .
  10. , , , , , . A novel airlift photobioreactor with baffles for improved light utilization through the flashing light effect. J. Biotechnol.. 2001;92:89-94.
    [Google Scholar]
  11. , , , , , . Modeling the photocatalytic degradation of formic acid in a reactor with immobilized catalyst. Chem. Eng. Sci.. 2002;57:4895-4907.
    [Google Scholar]
  12. , , , , . Simultaneous measurement of gas hold-up and mass transfer coefficient by tracer dynamic technique in “Emulsair” reactor with an emulsion-venturi distributor. Chem. Eng. Sci.. 2005;60:6414-6421.
    [Google Scholar]
  13. , , , . Photocatalytic degradation of Basic Red 46 and Basic Yellow 28 in single and binary mixture by UV/TiO2/periodate system. J. Hazard. Mater.. 2009;164:1487-1495.
    [Google Scholar]
  14. , , . Photo-catalytic conversion of air borne pollutants. Effect of catalyst type andcatalyst loading in a novel photo-CREC-air unit. Appl. Catal., B. 2002;38:201-213.
    [Google Scholar]
  15. , , , , , . Solar photocatalytic decolorization of C.I. Basic Blue 41 in an aqueous suspension of TiO2–ZnO. Dyes Pigm.. 2008;78:77-83.
    [Google Scholar]
  16. , , , , . Optimization of photocatalytic performance of TiO2 coated glass microspheres using response surface methodology and the application for degradation of dimethyl phthalate. J. Photochem. Photobiol., A. 2013;262:7-13.
    [Google Scholar]
  17. , , , . Optimization of manufacturing conditions for activated carbon from Turkish lignite by chemical activation using response surface methodology. Appl. Therm. Eng.. 2007;27:1212-1218.
    [Google Scholar]
  18. , , , , . Optimization of photocatalytic treatment of dye solution on supported TiO2 nanoparticles by central composite design: intermediates identification. J. Hazard. Mater.. 2010;181:886-897.
    [Google Scholar]
  19. , , , . Surfactant recovery by foam fractionation using the gas–liquid contactor, emulsion venturi. Separ. Sci. Technol.. 2014;49:311-316.
    [Google Scholar]
  20. , . Application of Taguchi and response surface methodologies for geometric error in surface grinding process. Int. J. Mach. Tool Manuf.. 2005;45:327-334.
    [Google Scholar]
  21. , , . Modelling and design of thin-film slurry photocatalytic reactors for water purification. Chem. Eng. Sci.. 2003;58:2269-2281.
    [Google Scholar]
  22. , , . Optimal decolorization efficiency of Reactive Red 239 by UV/TiO2 photocatalytic process coupled with response surface methodology. Chem. Eng. J.. 2005;112:173-179.
    [Google Scholar]
  23. , , , , , , . A new photobioreactor for continuous microalgal production in hatcheries based on external-loop airlift and swirling flow. Biotechnol. Bioeng.. 2009;102:132-147.
    [Google Scholar]
  24. , , , , . Removal of industry textile dyes by wood sawdust. J. Water Sci.. 1990;3:129-149.
    [Google Scholar]
  25. , , , , , . Development of a slurry continuous flow reactor for photocatalytic treatment of industrial waste water. J. Photochem. Photobiol., A. 2010;211:42-46.
    [Google Scholar]
  26. , , , , . Photocatalytic degradation of indole in UV/TiO2: optimisation and modelling using the response surface methodology (RSM) Environ. Chem. Lett.. 2009;7:45-49.
    [Google Scholar]
  27. , , , . Radiation absorption and degradation of an azo dye in a hybrid photocatalytic reactor. Chem. Eng. Sci.. 2009;64:2173-2185.
    [Google Scholar]
  28. , , , . Comparison between the reactivity of commercial and synthetic TiO2 photocatalysts. J. Photochem. Photobiol., A. 2001;139:253-256.
    [Google Scholar]
  29. , , , . Photocatalytic conversion of phenolic compounds in slurry reactors. Chem. Eng. Sci.. 2004;59:3-15.
    [Google Scholar]
  30. , , , . Effect of oxygen and hydrogen peroxide on the photocatalytic degradation of monochlorobenzene in TiO2 aqueous suspension. Int. J. Photoenergy 2012
    [CrossRef] [Google Scholar]
  31. , , , , , . Modeling physical and oxidative removal properties of Fenton process for treatment of landfill leachate using response surface methodology (RSM) J. Hazard. Mater.. 2010;180:456-465.
    [Google Scholar]
  32. , , , , . Impact of ammonia concentration on Spirulina platensis growth in an airlift photobioreactor. Bioresour. Technol.. 2011;102:3234-3239.
    [Google Scholar]
  33. , , , , , . Development of a novel capillary array photocatalytic reactor and application for degradation of azo dye. Chem. Eng. J.. 2011;7809:1-2.
    [Google Scholar]
Show Sections