American Journal of Chemistry

p-ISSN: 2165-8749    e-ISSN: 2165-8781

2016;  6(2): 47-54

doi:10.5923/j.chemistry.20160602.04

 

Adsorption of Methylene Blue on the Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5, 1) Lyonsite Phases

Khadija Gourai 1, Abdeslam El Bouari 1, Bouchra Belhorma 2, Lahcen Bih 3

1Department of Chemistry, Laboratory of Physical Chemistry of Applied Materials, Faculty of Sciences Ben M’Sik, University Hassan II Casablanca, Casablanca, Morocco

2National Center for Energy, Nuclear Science and Technology, Rabat, Morocco

3Team Physical Chemistry of Condensed Matter, Faculty of Sciences Meknes, University Moulay Ismail, Meknes, Morocco

Correspondence to: Khadija Gourai , Department of Chemistry, Laboratory of Physical Chemistry of Applied Materials, Faculty of Sciences Ben M’Sik, University Hassan II Casablanca, Casablanca, Morocco.

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Copyright © 2016 Scientific & Academic Publishing. All Rights Reserved.

This work is licensed under the Creative Commons Attribution International License (CC BY).
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Abstract

This work focuses on the study of the adsorption of methylene blue (MB) onto the mixed transition metal oxide compounds Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) of Lyonsite structure. The studies are carried out in batch methods, and they allowed determining several parameters that govern this adsorption. The influence of pH, temperature, contact time and mass of the adsorbent on the MB adsorption were determined. The adsorption kinetics was analyzed using the Langmuir and Freundlich models. The obtained results show that the adsorption of methylene blue onto these mixed oxides is well described by the model of Langmuir and its kinetic corresponds to the second order.

Keywords: Adsorption, Methylene blue, Kinetic, Isotherm, Lyonsite structure

Cite this paper: Khadija Gourai , Abdeslam El Bouari , Bouchra Belhorma , Lahcen Bih , Adsorption of Methylene Blue on the Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5, 1) Lyonsite Phases, American Journal of Chemistry, Vol. 6 No. 2, 2016, pp. 47-54. doi: 10.5923/j.chemistry.20160602.04.

1. Introduction

The treatment of brackish water by reverse osmosis is a membrane filtration technique which allows production of good quality water for different applications (drinking water, agriculture, industries...) [1, 2]. This treatment requires a series of meadows-treatments such as the filtration with activated carbon, which is based on the phenomenon of adsorption, and is relatively easy to implement. The activated carbon is the most widely used adsorbent because of its high adsorption capacity [3]; but it has the disadvantage of a high cost and difficulty to regenerate after each adsorption cycle which limits its commercial application [4]. Hence, several investigations looking for new adsorbents with high efficiency and low cost are performed [5-7]. In order to evaluate how these adsorbents are more effective, the studies considered the investigation of the mechanism of attachment of dye molecules on the surface of the adsorbents.
According to the literature [8, 9], several new adsorbents based on transition metal oxide were proposed. In the framework of looking for new adsorbent materials, our interest is focused on oxide compounds based on molybdate Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) containing transition metals like iron and chromium. In fact, the presence of these transition metals in the structure of these molybdates could facilitate the adsorption and therefore the elimination of impurities from water. The first molybdate material which has the lyonsite structure is the compound NaCo2.31(MoO4)3 [10]. In general, oxides of lyonsite structure can be expressed as A16B12O48 and are composed of an assembly of octahedra AO6 and tetrahedrons BO4. The octahedral sites AO6 are occupied by heavily loaded cations of electrical-charge +5 and +6 and the tetrahedral sites BO4 are occupied by the cations of charges +1, +2 and +3 such as (Li+, K+, Na+, Zn2+, Ca2+… ) [11].
In this work, we present first the method of preparation of the molybdates Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) and then the studies of adsorption of methylene blue onto these compounds. The influence of pH, temperature, contact time and mass of the adsorbent on the adsorption capacity is studied. The adsorption kinetic is determined using the models of Langmuir and Freundlich.

2. Materials and Methods

2.1. Adsorbent

The adsorbents used in this study are the molybdates Lyonsite type of the formulae Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1). The powders of Li3Fe1-xCrx(MoO4)3 are prepared by the soft combustion method which consists to dissolve in a minimum volume of water a mixture of glycine (C2H5NO2)2 and stoichiometric reagents nitrates (LiNO3), Fe(NO3)3.9H2O, Cr(NO3)3.9H2O and (NH4)6Mo7O24.4H2O). These solutions provide highly viscous liquids after dehydration at a temperature of 80°C. Then a heat treatment between 150°C and 200°C allows to obtain powders of porous molybdates Li3Fe1-xCrx(MoO4)3. Finally, these powders were submitted to a final heat treatment at 700°C.
The structural analysis of these samples was carried out by X-ray diffraction (XRD) technique using a Bruker D8 Advance apparatus. The UV-Visible spectra of the solutions are measured by a UV-3100PC spectrophotometer VWR. A pH-meter PHSJ-5 was used for the pH measurements.

2.2. Adsorbate

The adsorbate considered in this work is the 3.7-bis-(dimethylamino) phenazathionium known as the methylene blue which is a cationic dye, and it was synthesized the first time by Heinrich Caro in 1876. Its molecular formula is C16H18CIN3S, with a molar mass equal to 319.852 g/mol and a pH equal to 6.5. The Fig.1 shows the chemical structure of methylene blue.
Figure 1. Chemical Structure of methylene blue

2.3. Adsorption Experiments

The adsorption was made in batch method and the concentration of the solution was determined by using UV–visible spectrophotometer (VWR, V 3100). The calculation of the adsorption capacity is carried out from the following equation:
(1)
where, Qe: Adsorption capacity of the adsorbent (mg/g), C0: Initial concentration of dye (mg/l), Ce: Concentration of dye (mg/l) at equilibrium, m: Mass of the adsorbent (g), V: Volume of the solution.

3. Results and Discussion

3.1. X-Ray Diffraction Analysis

X-ray patterns of Li3Fe1-xCrx(MoO4)3 (x= 0, 0.5 and 1) samples are shown in Fig.2. The replacement of iron (Fe3+) by chromium (Cr3+) gives X-ray patterns with the same shapes but with a small displacement of X-ray peaks. It is demonstrated that the substitution of iron by chromium form a continuous solid solution because Cr3+ (r = 0.615 Å) and Fe3+ (r = 0.645 Å) [12] have similar sizes. The results show that these materials crystalize in the orthorhombic pattern, with a space group Pnma. The experimental XRD data for all the samples are successfully indexed by DICVOL software and the linear cell parameters are gathered in Table 1. It is noticed that the substitution of iron by chromium induces the decrease of these parameters owing to the fact that the ionic radius of chromium Cr3+ is slightly smaller compared to that of Fe3+.
Figure 2. XRD patterns of Li3Fe1-xCrx(MoO4)3 : (a) x = 0, (b) x = 0.5 and (c) x = 1
Table 1. Cell parameters of Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) materials
     

3.2. Influence of Some Parameters on the Adsorption

3.2.1. Effect of Contact time
The effect of contact time on adsorption of MB onto the Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) samples is studied. The experiments were realized at room temperature by keeping the pH of the solution constant at 6.5 and using 20 mg/l MB. Fig.3 showed the obtained results. The uptake of MB onto the different adsorbents is nearly the same. The adsorption equilibrium is reached in 5 min (28 mg/g), and the adsorption capacity becomes nearly constant without changes after this equilibrium time. The short equilibrium time (5 min) could indicate that the adsorption reaction between MB and lyonsite samples is very fast [13].
Figure 3. Influence of the contact time on the adsorption of the MB on Li3Fe1-xCrx(MoO4)3
The substitution of iron by the chromium seems to have a positive effect on the adsorption of MB on the Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) adsorbents. The adsorption capacity increases with the increase of the amount of chromium in the samples. By moving from x = 0 to x = 1 the adsorption capacity increases by a little bit from 27 mg/g to 32 mg/g.
3.2.2. Effect of Temperature
In general, the adsorption depends on the structure of the adsorbent and on the temperature. To get an idea of this dependency, we studied the effect of temperature on the adsorption of MB onto the prepared molybdate adsorbents.
The experiments were performed by adding 20 mg of Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) to a solution of 100 ml of methylene blue at different temperature. The temperatures were set at 25°C, 45°C, 65°C and 75°C using a thermostat bath. Fig.4 shows the dependence of the adsorption content of MB on the temperature.
Figure 4. The temperature dependence of the MB adsorption
From Fig.4, one can note that the adsorption capacity increases with the temperature. Actually, from 25°C to 75°C the adsorption capacity of the Li3Fe(MoO4)3 increases from 28.944 mg/g to 74.403 mg/g; that of Li3Fe0.5Cr0.5(MoO4)3 increases from 28.925 mg/g to 49.726 mg/g; and that of Li3Cr(MoO4)3 goes up from 32.184 mg/g to 90.452 mg/g. This induces that the temperature has a positive effect on the adsorption; In fact, the increase of temperature increases the diffusion rate of the adsorbed molecules through particles of the external layer of adsorbent [14]. Moreover, it is showed from the adsorption-temperature dependency that the chromium based compound is more effective for the MB adsorption.
The adsorption process of MB onto the Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) induces some energy changes of the adsorbate-adsorbent system. This energy can be reflected by the thermodynamic parameters such as free energy change (∆G°, kJmol-1), entropy change (∆S°, Jmol-1K-1) and enthalpy change (∆H°, kJmol-1). They can be determined by the following equations:
(2)
(3)
where K is the equilibrium constant.
By plotting LnK as a function of 1/T (Fig.5), we obtained a straight line of slope ∆H/R and the intercept ∆S/R.
Figure 5. Variation of the equilibrium constant Ln K as a function of temperature for MB adsorption on Li3Fe1-xCrx(MoO4)3
By determining these thermodynamic parameters one can get more insight to the effect of temperature on the adsorption and investigate the possible mechanism involved in the adsorption process. The calculated values of thermodynamic parameters were gathered in Table 2. It is observed that the free energy values are negative and ascertaining that the adsorption of MB on lyonsite adsorbent is spontaneous and thermodynamically favorable [15]. The mechanism of the adsorption could be understood from the values of the free energy [16]. For instance, it is reported [16] that the change in free energy for physisorption was between -20 and 0 kJ/mol, while chemisorption mechanism was in the range -80 to -400 kJ/mol. According to data of Table 2, the values of (∆G°) are within the range -20 to 0 kJ/mol. This result suggests the main adsorption of MB onto lyonsite adsorbents could be performed by the physisorption mechanism.
Table 2. Thermodynamic parameters of the MB adsorption onto lyonsite Li3Fe1-xCrx(MoO4)3 adsorbents (x = 0, 0.5 and 1) at various temperatures
     
Furthermore, the positive value of ∆H indicated that the adsorption is an endothermic process. In other words, the positive values of the enthalpy energy suggest that the MB adsorption onto the molybdate sorbents is more favorable at high temperatures, in agreement with the dependence of the adsorption with the temperature given in Fig.4. In addition, the positive value of ∆S do indicate the increase randomness at the solid-solution interface during the adsorption process of MB on the molybdate adsorbents [17]. One can also remark that the given values of the entropy energy are relatively low suggesting that the interactions between MB and the molybdate adsorbents are physical in nature. The same result is proposed elsewhere [18].
3.2.3. Effect of pH
The pH is an important factor in any study of adsorption because it can influence at the same time the adsorbent structure and the mechanism of the adsorption [19]. The effect of the pH on the adsorption is studied by adjusting the initial pH of the methylene blue, by adding NaOH and HCl, to adjust the pH to 2, 4, 6, 8, and 10. The experiments were performed by adding 20 mg of Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) to 100 ml of the methylene blue solution (20 mg/l) at different pH values under the temperature of 25°C.
The effect of the pH of the aqueous solution in the MB adsorption onto the Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) can be attributed to the variation in the degree of ionization of MB and the surface properties of the molybdates. The influence of pH on the adsorption is demonstrated in Fig.6. This latter indicates that an increase in solution pH from 2 to 10 induces an increase in the MB adsorption capacity on molybdate adsorbents. It is observed that the MB adsorption is pH-dependent and the uptake of the MB onto the molybdate adsorbents is favorable at higher pH value. For instance, at low pH values (from 2 to 4), the adsorbed quantity is about 26 mg/g; by increasing pH value up to 6 the uptake quantity becomes 34 mg/g. At high pH values the adsorbed quantity attains 93.8 mg/g [20].
Figure 6. Influence of pH on the adsorption of MB on Li3Fe1-xCrx(MoO4)3
3.2.4. Effect of Adsorbent Mass
The effect of mass is studied by adding 100 ml of 20 mg/l MB to different masses of the lyonsite adsorbent 20, 40, 60, 80 and 100 mg. The experiment is done at room temperature at pH = 6.5. Fig.7 shows the effect of adsorbent mass on MB adsorption by molybdate lyonsite adsorbent.
Figure 7. Effect of adsorbent mass on MB adsorption onto Li3Fe1-xCrx(MoO4)3 phases
The effect of adsorbent mass shown in Fig.7 shows that the increase in adsorbent mass increases the removal rate of MB in the solution. The reason for such behavior could be due to large number of vacant adsorption sites allowing more interactions between MB and molybdate species. This increase of the MB adsorption could also be in favor of the discoloring phenomenon of some aqueous solutions [21]. Furthermore, for the same adsorbent mass, the adsorbent based on chromium molybdate shows high adsorptive reaction of MB in comparison to the other molybdates.
According to the experimental results, it seems that the statistical distributions of chromium and iron in the structure of Li3Fe1-xCrx(MoO4)3 have an important effect on the MB adsorption. Indeed, in the compounds relatives to pure chromium (x=1) and in its homologous iron molybdate (x=0) in which the distribution of cationic ions is ordered one can observe that the removal rate of MB is high. However, when there is a mixture of cations in the structure (x=0.5) the removal of MB decreases.

3.3. Adsorption Kinetics

The adsorption kinetic is an essential issue in the adsorption studies since it reveals some aspects of the adsorption process. The study of adsorption kinetics of MB onto Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) molybdates is considered in the framework of the first-order and the second-order models. The conformity between the experimental data obtained from the kinetic experiments and the model prediction are based on the values of the correlation coefficients (R2); the value of R2 nearest to the unit indicates the proper model to describe correctly the adsorption kinetics.
The linear forms of these models are given by the following equations:
(4)
(5)
where Qe: Quantity of MB at equilibrium (mg/g), Qt: Quantity of MB adsorbed at any time t, k1 (min-1) and k2 (g.mg-1.min-1): the pseudo-first-order and pseudo-order model rate constants, respectively.
The plot of log (Qe-Qt) versus time as experimental data is represented in Fig.8. They are fitted by the kinetic model of the pseudo-first order. The correlation coefficient (R2), k1 and calculated Qe are gathered in Table 3. The experimental results fitted by the pseudo-second order model are shown in Fig.9. The amount adsorbed at equilibrium Qe and the constant of the pseudo-second order k2 can be determined from the slope and intercept of t/Qt as function of t. Table 4 summarizes the obtained parameters.
Figure 8. The plots of log (Qe-Qt) versus time relative to MB adsorption onto Li3Fe1-xCrx(MoO4)3
Table 3. The first-order model parameters for MB adsorption on molybdate adsorbents Li3Fe1-xCrx(MoO4)3
     
Figure 9. The second order model fits to the experimental data for the adsorption of the MB on Li3Fe1-xCrx(MoO4)3
Table 4. Parameters of the second order kinetic model for MB adsorption on molybdate adsorbents Li3Fe1-xCrx(MoO4)3
     
The calculated (Qe) of the pseudo-first order model is within the range from 2 to 9 mg/g and the coefficient correlation (R2) varies from 0.83 to 0.89. On the contrary, the calculated (Qe) of the pseudo-second order varies according to the chemical composition of the molybdate compounds from 28.73 to 33.11 (mg/g); and the correlation coefficient (R2) is 0.99. One can note that the correlation coefficient R2 is very close to the unit while the adsorbed quantity at equilibrium is close to that calculated by employing the pseudo-second order model. This result shows that the second order model fits well the experimental data. According to this kinetic model, the adsorption process under study depends on MB and Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) and the mechanism of the adsorption involves both the chemisorption and/or the physisorption process [22].

3.4. Adsorption Isotherms

Adsorption isotherm describes the relationship between the adsorbed content of one substance and its amount in the equilibrium solution at fixed temperature. It facilitates the description of the interaction between the adsorbate and the adsorbent. Adsorption isotherm represents the amount of the adsorbate bounded to the surface (Qe) as a function of the material present in the solution (Ce). Fig.10 reproduces the adsorption isotherms relatives to the molybdates Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1).
Figure 10. Adsorption isotherm of MB onto Li3Fe1-xCrx(MoO4)3
According to Giles et al [23], the obtained adsorption equilibrium for MB onto Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) adsorbents belongs to class L curve. It reveals that the MB adsorption process could occur in monolayer form.
In this study two isotherm models namely Langmuir and Freundlich were used to determine the adsorption mechanism of MB onto Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) and the surface properties of the adsorbent.
The Langmuir equation is adapted to describe the behavior of adsorption of homogeneous surfaces. The linear transformation of this model gives the following equation:
(6)
where Qe: is the adsorption capacity at equilibrium (mg/g), Qm: is the maximum adsorption capacity (mg/g), Kl : is the Langmuir equilibrium constant (l/mg) and Ce: is the equilibrium concentration of MB in solution (mg/L).
An essential parameter of the Langmuir isotherm is the parameter RL; it’s defined by the following equation:
(7)
where Kl is the Langmuir constant and C0 is the highest adsorbate concentration. When RL is greater than 1, the adsorption is unfavorable, and when RL is equal to 1 it indicates that the adsorption is linear, whereas when RL is between 0 and 1, the adsorption is favorable [24].
On the other hand, the Freundlich model is an empirical expression which assumed that a multilayer adsorption occurs on the heterogeneous surface or surface supporting sites of various affinities. The isotherm is given by the following equation:
(8)
where Qe: is the equilibrium MB concentration on the adsorbent (mg/g), Ce: is the equilibrium concentration of MB in the solution (mg/l), Kf: is the empirical constant of Freundlich isotherm, nf: is the empirical parameter related to the favorability of the adsorption process. For instance, when the ratio (1/nf) takes values below 1, the adsorption is favorable. The linear form of the equation (8) is the following equation:
(9)
Fig.11 and Fig.12 give the adsorption isotherms of MB onto Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) according to Langmuir and Freundlich models, respectively. Table 5 gathers all the extracted parameters from the used models.
Figure 11. Langmuir isotherm of the MB adsorption onto Li3Fe1-xCrx(MoO4)3
Figure 12. Freundlich isotherm of the MB adsorption onto Li3Fe1-xCrx(MoO4)3
Table 5. Isotherm parameters and correlation coefficients for the MB adsorption onto Li3Fe1-xCrx(MoO4)3
     
The inspection of the data from Table 5 shows that the obtained values for the Langmuir RL parameter are comprised between 0 and 1, suggesting that the adsorption is favorable. Indeed, the correlation coefficient (R2) for Langmuir model is high and indicates that the Langmuir model fits well the adsorption of the MB on Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) samples with Qm= 48.07 for the composition (x=1). This indicates that the adsorption of MB occurs on localized sites with no interaction between MB molecules and that the maximum adsorption occurs when the surface is covered by a monolayer of adsorbate [25]. On the other hand, according to the data of Table 5 and specially the values of the correlation coefficient (R2) extracted from the fits of the experimental adsorptions by the Freundlich model, one can also consider that the later model could describe the MB adsorption. However, this assumption is rejected since the values of (1/nf) parameter are higher than 1 which makes the adsorption unfavorable.

4. Conclusions

The molybdates Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) have been successfully synthesized by the soft combustion method and proved to belong to the Lyonsite type structure. The adsorption studies showed that these materials can interact with the MB dyes. The results showed that the MB adsorption depended on pH of solution, temperature, adsorbent amount and contact time. The adsorption was found to be favorable with the increasing of pH of solution and it was indicated that the adsorption is more favorable at high temperature. The adsorption of MB onto Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) was best described by the pseudo-second order model. The thermodynamic parameters of the adsorption showed that the adsorption of MB onto Li3Fe1-xCrx(MoO4)3 (x = 0, 0.5 and 1) is an endothermic process and the interaction between MB and the molybdate adsorbents are physical in nature. The maximum value of the adsorption capacity calculated according to the Langmuir model for the composition (x=1) is 48.07 mg/g. It is also shown that the adsorption is very fast and the substitution of iron by the chromium has a positive effect on the adsorption.

ACKNOWLEDGEMENTS

The authors acknowledge the Institute for Research in Solar Energy and New Energies (IRESEN) for the financial support.

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