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Thilagavathy, P., and Santhi, T. (2013). "Sorption of toxic Cr(VI) from aqueous solutions by using treated Acacia nilotica leaf as adsorbent: Single and binary system," BioRes. 8(2), 1813-1830.

Abstract

The use of cheap and eco-friendly adsorbents prepared from freely and abundantly available Acacia nilotica leaves for the removal of highly toxic Cr(VI) from aqueous solutions in single and binary ion solutions as well as from a mixture of it with Co(II) & Cu(II) was investigated by batch methods. The effects of pH, contact time, and initial metal ion concentration of Cr(VI) onto H2SO4-treated Acacia nilotica leaves (HAN) was investigated. The linear form of the Freundlich model achieved high coefficients of determination R2 = 0.9808 for Cr(VI) adsorption. The R2 values for fitting the adsorption rate data were greater than 0.983 for Cr(VI) ion, which indicates the applicability of pseudo-second-order kinetic model. The desorption and recycling ability of Cr(VI) and HAN were found to be good. The studies showed that this low-cost adsorbent could be used as an efficient adsorbent material for the removal of Cr(VI) from aqueous solutions.


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Sorption of Toxic Cr(VI) From Aqueous Solutions by Using Treated Acacia nilotica Leaf as Adsorbent: Single and Binary System

Palanisamy Thilagavathyand Thirumalisamy Santhib,*

The use of cheap and eco-friendly adsorbents prepared from freely and abundantly available Acacia nilotica leaves for the removal of highly toxic Cr(VI) from aqueous solutions in single and binary ion solutions as well as from a mixture of it with Co(II) & Cu(II) was investigated by batch methods. The effects of pH, contact time, and initial metal ion concentration of Cr(VI) onto H2SO4-treated Acacia nilotica leaves (HAN) was investigated. The linear form of the Freundlich model achieved high coefficients of determination R2 = 0.9808 for Cr(VI) adsorption. The Rvalues for fitting the adsorption rate data were greater than 0.983 for Cr(VI) ion, which indicates the applicability of pseudo-second-order kinetic model. The desorption and recycling ability of Cr(VI) and HAN were found to be good. The studies showed that this low-cost adsorbent could be used as an efficient adsorbent material for the removal of Cr(VI) from aqueous solutions.

Keywords: Adsorption; Cr(VI); Acacia nilotica leaves; Isotherms; Kinetics; Desorption

Contact information: a: Department of Chemistry, Professional Group of Institutions, Palladam641 662 India; b: Department of Chemistry, Karpagam University, Coimbatore India;

* Corresponding author: ssnilasri@yahoo.co.in

INTRODUCTION

The presence of heavy metals in the environment can be detrimental to a variety of living species including human. Heavy metals can be distinguished from other toxic pollutants, since they are non-biodegradable and can accumulate in living tissues, thus becoming concentrated throughout the food chain. Compared to other heavy metal ions, chromium (VI) is abundant in nature and also highly toxic and carcinogenic (Goyer and Mehlman1977; Carson et al. 1986). Chromium exists in +3 and +6 oxidation states, as all other oxidation states are not stable in aqueous solutions. Both valences of chromium are potentially harmful (Dakiky et al. 2002). Hexavalent chromium, which is primarily present in the form of chromate (CrO42−) and dichromate (Cr2O72−) ions, poses significantly higher levels of toxicity than the other valency states (Ahalya et al. 2010).The permissible limit of chromium ion for drinking water is 0.1 mgL-1 (as total chromium). Electroplating and tannery industry effluents are the major sources for the Cr(VI) production in wastewater streams. Eye irritation has been reported by factory workers exposed to chromium dust. Hence it is essential to remove chromium from industrial wastewater before discharging to natural water sources, in order to meet National Regulatory Standards as well as to protect public health. The treatment method for metal-bearing effluents commonly includes chemical precipitation (hydroxides, sulphides, etc.), membrane filtration (reverse osmosis, nano filtration, etc.), electrolytic reduction, solvent extraction, ion exchange, and adsorption (Rousseau 1987). These methods are non-economical and have many disadvantages such as incomplete metal removal, high reagent and energy requirements, and generation of toxic sludge or other waste products that require disposal or treatment. The adsorption process is the most useful method to remove Cr(VI); this approach takes advantage of the availability of different kinds of adsorbents associated with convenient procedures for obtaining high efficiency (Harland 1994; Cooney 1999). A large number of different adsorbent materials containing a variety of attached chemical functional groups have been reported for this purpose. For instance, activated carbon is the most popular material; however its high cost restricts its large-scale use (Bable and Kurniawan 2003; Bailey et al.1999). This problem has led many researchers to search for cheaper adsorption substitutes including fly ash, lignin, peat, natural material, (chitosan, alginate, biomass, etc.), clays (clinoptilolite, montmorillonite, kaolinite, etc.) (El-Geundi 1997), and cellulose-based hydrogels (Zhou et al. 2012). The present study evaluates the possibility of using Acacia nilotica leaf carbon as a low-cost adsorbent for the removal of Cr(VI) ions from dilute solutions. Acacia nilotica is native to Africa and the Indian subcontinent. Acacia nilotica leaves are used as an agricultural waste for the depollution of water effluents contaminated by heavy metals from industrial effluents (Santhi et al. 2011).

EXPERIMENTAL

Materials

Preparation of chemically treated adsorbent (HAN)

The leaves of Acacia nilotica used in this work were collected locally (Palladam, India). Leaves were shade-dried and powdered in a grinder. Then the mixture was impregnated with conc. H2SOfor 20 h and washed thoroughly with distilled water until it attained neutral pH. It was soaked in 2% NaHCO3 overnight in order to remove any excess of acid and kept in a hot air oven at 300°C for carbonization. Then the material was named as HAN and preserved in an air-tight container for further use.

Adsorbate

All the chemicals used were of analytical grade. A stock solution of 1000 mgL-1Cr(VI) was prepared by dissolving 2.8287g of 99.9% potassium dichromate (K2Cr2O7) in 1000 mL of distilled water. This solution was diluted as required to obtain standard solutions containing 50 to 200 mgL-1 of Cr(VI). Adjustment of pH was carried out by using 0.5N HCl and 0.5N NaOH solutions.

Methods

Batch adsorption experiments were carried to evaluate the effects of pH, contact time, initial concentration, and adsorbent dosage on the adsorbed amounts. Tests were carried out to evaluate adsorption kinetics, adsorption isotherms, and desorption of Cr (VI) on HAN. In all sets of experiments a fixed volume of single metal ion solutions (SMS) (50 mL) of various concentrations (50,100,150, and 200 mgL-1) and for Binary Metal System (BMS) 50 mL volume of BMS solution with 25 mL of 50 mgL-1 concentration of working metal and 25 mL of Co2+ and Cu2+ of various concentrations (10, 20, 30, 40, and 50 mgL-1) were taken in a conical flask. For TMS, 50 mL volume of TMS solution with 25 mL of 50 mgL-1 concentration of working metal and 12.5 mL of both Co2+ and Cu2+ of various concentrations (10, 20, 30, 40, and 50 mgL-1) were taken in conical flasks, which were thoroughly mixed with 0.2 g of biosorbent dose at room temperature at 160 rpm (revolutions per minute) shaking speed for 2 h. Two hours of equilibrium period for sorption experiment was used to ensure equilibrium. The pH values were adjusted from 2 to 10 using 0.1 N HCl and 0.1 N NaOH solutions and were measured using a digital pH meter (ELICO L1120). The initial Cr (VI) concentration was measured spectrophotometrically by developing a purple-violet color with 1,5-diphenyl carbazide in acidic solution as a complexing agent (APHA 1985), and the absorbance was measured at λmax of 540nm. The flasks were kept on a rotating shaker with constant shaking. At the end of the experiment, the flasks were removed and the solution was separated from the adsorbent by filtration through filter paper. The filtrate was analyzed to find out the amount of metal left after sorption. The amount of equilibrium uptake of metal (qe) and the percentage removal were calculated using the following equations,

where Co and Ce are the initial and final equilibrium concentration, Vis the volume (L) of the solution, and w is the weight (g) of the adsorbent.

RESULTS AND DISCUSSION

Characterization of HAN

Determination of Zero Point Charge (pHzpc) was carried out to investigate the surface charge behavior of both adsorbents. For the determination of pHzpc, 0.2 g of the sample suspension was prepared in 50 mL of NaNOelectrolyte of concentration approximately 10-2M. Aliquots of suspensions were adjusted to various pH values with 0.5 N NaOH and 0.5 N HNO3. After 60 min of equilibrium, initial pH was measured. Then 0.1 g of NaNOwas added to each aliquot to bring the final electrolytic concentration to about 0.45 M. After an additional 60 min of agitation, the final pH was measured. The results were plotted with initial pH (final pH – initial pH) against final pH.

Fig. 1a. SEM image of HAN before Cr(VI) loading

Fig. 1b. SEM image of HAN after Cr(VI) loading

The surface morphology was studied using scanning electron microscopy (SEM) (Fig. 1a.) An SEM image of HAN before Cr(VI) loading at a magnification of 1000X shows that the surface of material was porous, and Fig.1b shows the Cr(VI) loaded sites at magnification of 2000X. It is clear from the SEM image that the external surface of the sample was rough and contained abundant porous structures of different size and shapes. The inner cavities in porous structures provide new structures for the accommodation of Cr(VI) ions.

Effect of pH Cr(VI) Adsorption onto HAN

The pH of the solution is an important factor that controls the uptake of Cr(VI). The experimental results revealed that the percentage adsorption increased as the pH was decreased and reached 97% for 50 mgL-1 of Cr(VI) concentrations. When the pH increased above 3, the percent removal decreased (Fig. 2). Similar results have been reported (Donmez and Aksu 2002; Dakiky et al. 2002; Selvaraj et al. 2003; Yu et al. 2003; Ucun et al. 2002; Hu et al. 2003; Gupta et al. 2001). The high adsorption of Cr(VI) can be explained by the species of chromium and the adsorbent surface. At acidic pH, the predominant species of Cr(VI) are Cr2O72-, HCrO4-, and CrO42-. Under acidic conditions, the surface of the adsorbent becomes protonated and attracts anionic species of Cr(VI). The reduction of Cr(VI) to Cr(III) has been found to proceed under highly acidic conditions (i.e. pH between 1 and 3). Researchers have observed that oxidation of surface groups of a cellulose-based sorbent material takes place when reductively adsorbing the Cr(VI) ion. Studies involving the blocking of specific sites have shown that both carboxyl groups and amino groups can participate in the reductive adsorption process of Cr(VI) and that the oxidation of the surface often increases the number of carboxylate groups, which are well suited to the bonding of the positively charged Cr(III) ions that result from the process (Hubbe et al. 2012). The effects of pH of Cr(VI) adsorption on various adsorbents are shown in Table 1.

Fig. 2. Effect of pH onto HAN

Effect of Contact Time and Initial Concentration

The uptake of Cr(VI) onto HAN increased with increase in contact time. The adsorption equilibrium was achieved at 2 h. The nature of adsorbent and available adsorption sites affected the rate of adsorption of Cr(VI). The mechanism of solute transfer to the solid includes diffusion through the fluid film around the adsorbent particle, and diffusion through the pores to the internal adsorption sites occurs at pH 3. In the initial stage of adsorption of Cr(VI), the concentration gradient between the film and the available pore sites are large, and hence the rate of adsorption of Cr(VI) is faster. The rate of adsorption decreases in later stage is probably due to the slow pore diffusion of the solute ion into the bulk of the adsorbent.

The uptake of Cr(VI) onto HAN as a function of contact time is shown in Fig. 3. It can be seen that with the increase in the Cr(VI) concentration from 50 to 200 mg g-1, the percentage removal decreased from 97% to 58% and the adsorption capacity increased from 12.13 to 36.29 mg g-1. The decrease in percentage can be explained by the fact that all the adsorbents had a limited number of active sites, which would have become saturated above a certain concentration. The increase in adsorption capacity with increase in Cr(VI) concentration may be due to the higher adsorption rate and utilization of all the available sites for the adsorption at higher concentration.

Fig. 3. Effect of contact time and initial concentration

Adsorption Isotherm

The Langmuir Isotherm

The Langmuir isotherm model assumes monolayer coverage of adsorbate over a homogeneous adsorbent surface (Langmuir 1918). There is an assumption that sorption takes place at specific homogeneous sites within the adsorbent. Once a metal molecule occupies a site, no further adsorption can take place at that site. It is commonly expressed as:

 (3)

The equation (3) can be linearized into the following form (Kinniburgh 1986; Longhinotti et al. 1998),

 (4)

where q(mg/g) and Ce(mg/L) are defined before in Eq(2). Qis a constant and reflects a complete monolayer (mg/g); Ka is the adsorption equilibrium constant (mg/L) that is related to the apparent energy of adsorption and is found to be 0.0846 mg/L. A plot of Ce/qeversus Ce should indicate a straight line of slope 1/Qand an intercept of 1/(KaQm), which is shown in the Fig. 4. The result obtained from the Langmuir model for the removal of Cr(VI) onto HAN is shown in Table 2.

Fig. 4. Langmuir Isotherm for adsorption of Cr(VI) onto HAN

The Freundlich isotherm

The well-known Freundlich isotherm is often used to describe adsorption on heterogeneous surface energy systems (Schneider et al. 2007; Cooney 1999; Ozacar 2003; Agyei et al. 2000). The Freundlich isotherm can be derived by assuming a logarithmic decrease in enthalpy of adsorption with the increase in the fraction of occupied sites. The isotherm model is commonly expressed by the following non-linear equation:

(5)

A linear form of this expression is,

 (6)

where Kf is the Freundlich constant and is the Freundlich exponent. Kf and n can be determined from the linear plot of log qe versus log Ce, which is given in Fig. 5. The values of the Freundlich constants together with a high coefficient of determination Rvalue of 0.9808 are presented in Table 2, which represents the best fit of experimental data compared to Langmuir isotherm equations. This trend is due to the high surface area of the adsorbent and multilayer of adsorption on the HAN. Freundlich constants Kf and were found to be 1.0278 mg/g and 3.9793, respectively. It has been shown by McKay et al. (1982) that values between 1 and 10 indicate beneficial adsorption. This trend was investigated also by Schneider et al. (2007), who observed that the Freundlich isotherm gave the best fit.

Fig. 5. Freundlich Isotherm for adsorption of Cr(VI) onto HAN

The Temkin Isotherm

Temkin and Pyzkey (1940) considered the effects of some indirect adsorbate or adsorbate interactions on adsorption isotherms and suggested that because of these interactions, the heat of adsorption of all the molecules in the layer would decrease linearly with coverage. The Temkin isotherms (Ozacar 2003; Choy et al. 1999) have been used in the following form:

 (7)

A linear form of the Temkin isotherm can be expressed as,

 (8)

where

 (9)

The constant β is related to heat of adsorption (Akkaya and Ozer 2005; Pearce et al. 2003). The adsorption data can be analyzed according to Equation (8). Therefore, a plot of qe versus lnCe enables one to determine the constants A and b. A plot of this type is shown in Fig. 6, and the values of the Temkin constants Ab, and coefficient of determination are listed in Table 2.

Fig. 6. Temkin Isotherm for adsorption of Cr(VI) onto HAN

The coefficient of determination obtained from the Temkin model was lower compared to those obtained for Langmuir, Freundlich, and D-R models, which indicates a poorer fit for adsorption of Cr(VI) onto HAN.

The Dubinin-Radushkevich isotherm

The Dubinin-Radushkevich isotherm and the Langmuir isotherm equations have been used for the adsorption of metal ions on surfactant-modified montmorillonite and adsorption of acid dyes on activated carbon (Choy et al. 1999; Lin and Juang2002) or adsorption of phosphorus on calcined alunite (Ozer 2005). It can be used to describe adsorption on both homogeneous and heterogeneous surfaces (Shahwan and Erten 2004). The Dubinin-Radushkevich equation has the following form (Dubinin and Radushkevich 1947; Gregg and Sing 1982),

 (10)

where Qm is the theoretical saturation capacity (mg/g), is a constant related to adsorp-tion energy, and ε is the Polanyi potential calculated from (Eq.11),

 (11)

where is the gas constant (8.314 J mol-1K-1), is the absolute temperature, and Cis the equilibrium constant. By plotting qversus ε2, it is possible to determine slope K and the value of Qm(mg g-1), which is the intercept and plot and is shown in Fig 7. The mean free energy E (KJ mol-1) of adsorption can be estimated by using the Kvalue obtained from the following equation:

 (12)

Fig. 7. D-R Isotherm for adsorption of Cr(VI) onto HAN

The calculated Dubinin-Radushkevich constants are given in Table 2. The satura-tion adsorption capacity Qobtained using D-R isotherm model for adsorption of Cr(VI) onto HAN was 18.386 mg g-1. The value of mean total error was determined, and the value was higher than both Freundlich and Temkin values but lower than Langmuir value. Therefore, the Dubinin-Radushkevich equation represents a better fit of experi-mental data than the Langmuir, Freundlich, and Temkin models.

Table 1. Maximum Adsorption Capacity of Various Low Cost Adsorbents and Agricultural Waste (Gupta and Babu 2009)

Table 2. Isotherm Constants for Cr(VI) Adsorption onto HAN

Kinetic Studies

Figure 3 shows that the amount of Cr(VI) adsorption increased with time and that it remained constant after a contact time of about 2 h. (i.e. equilibrium time). The equilibrium time was independent of initial Cr(VI) concentration. The time profile of chromium uptake could be represented by a single, smooth, and continuous curve leading to saturation, suggesting the possible multilayer coverage of chromium on the surface of the adsorbent. In order to investigate the mechanism of adsorption and potential rate controlling steps such as chemical reaction, diffusion control, and mass transport process, kinetic data were analyzed using pseudo-first order (Lagergren 1898), pseudo-second order (Ho et al. 2000), Elovich, and intra-particle diffusion (Weber and Morris 1963) equations. Many models such as the homogeneous surface diffusion model and the heterogeneous diffusion model (also known as pore and diffusion model) have been extensively applied in batch reactors to describe the transport of adsorbate inside the adsorbent particles (Fadali et al. 2005; Wu 2001; Raven et al. 1998). The conformity between experimental data and the model predicted values was expressed by the coefficient of determination (R2, values close or equal to 1). A relatively high R2value indicates that the model successfully describes the kinetics of Cr(VI) adsorption.

Pseudo first-order model

The sorption kinetics may be described by a pseudo first-order equation (Hossain et al. 2005). The pseudo-first-order equation of Lagergren is,

 (13)

where qe and qare the amounts of chromium that are adsorbed at equilibrium and at time (mg g-1), respectively, and k1 is the equilibrium rate constant of pseudo first-order adsorption (min-1). A plot of linear form of pseudo first-order model at all concentrations studied. The slopes and intercepts of plots of log (qeqt) versus t are used to determine the pseudo first-order constant k1 and equilibrium adsorption density qe, which is shown in the Fig. 8. A comparison of the results with the correlation coefficients is shown in Table 3. The correlation coefficients for the pseudo first order kinetic model obtained at all the studies concentrations were low. This suggests that this adsorption system is not a pseudo-first-order reaction and hence not a diffusion-controlled phenomenon.

Fig. 8. Pseudo-First-order kinetics for adsorption of Cr(VI) onto HAN

Pseudo second-order model

The adsorption kinetics may also be described by a pseudo-second-order equation (Ho et al. 1999).

 (14)

The pseudo second-order rate constants were used to calculate the initial adsorption rate, which is given by the following equation,

 (15)

where Kand qe values from the slopes and intercepts of plots t/qtversus t were used to calculate the pseudo second-order rate constants k2 and qe, and the plot is shown in the Fig 9. Table 3 lists the computed results obtained from the pseudo-second-order kinetic model. The coefficients of determination for the pseudo-second-order kinetic model obtained were greater than 0.983 for all concentrations, indicating the applicability of the pseudo-second-order kinetic model. Similar phenomena also have been observed in adsorption of dye RR189 on cross-linked chitosan beads (Chiouand Li 2002), in adsorption of dye BB69 and DR227 on activated clay (Wu 2001), in adsorption of AB9 on mixed sorbents (activated clay and activated carbon) (Ho et al. 1999), and in adsorption of Chromium hexavalent on used black tea leaves (Hossain et al. 2002).

Fig. 9. Pseudo-second-order kinetics for adsorption of Cr(VI) onto HAN

Elovich equation

The Elovich model of the adsorption capacity generally is expressed as the following equation (Chienand Clayton 1980; Sparks 1986),

 (16)

where Bis the initial adsorption rate (mg g-1min-1), and Ais the desorption constant (g/mg) during any experiment. It is simplified by assuming AB>>t. By applying the boundary conditions qt = 0 at t= 0 and qt = qt at t = t, equation (16) becomes:

 (17)

If Cr(VI) adsorption fits the Elovich model, a plot of qt versus ln (t) should yield a linear relationship with a slope of 1/AE and an intercept of (1/AE) ln (AEBE). Figure 10 shows a plot of linearization form of Elovich model at all concentrations studied. The initial adsorption rate BE increased from 15.8154. However, data deviated considerably from the theoretical data. A comparison of the results with the correlation coefficients is shown in Table 3. The correlation coefficients for the Elovich kinetic model obtained at all the studied concentrations were low. This suggests that this adsorption system is not an acceptable one for this system.

Fig. 10. Elovich equation for adsorption of Cr(VI) onto HAN

Intra-particle diffusion model

When diffusion (internal surface and pore diffusion) of metal ion inside the adsorbent is the rate-limiting step, then adsorption data can be expressed by the following equation (Srivastava et al. 1989),

 (18)

where, (mg g-1) is the intercept and Kdif is the intra-particle diffusion rate constant (in mg g-1 min-1/2). The values of qt were linearly correlated with values of √t, and the rate constant Kdif was directly evaluated from the slope of the regression line. Such plots may present a multi-linearity (Wu et al. 2001; Annadurai et al. 2002), indicating that two or more steps take place. The first, sharper portion represents the external surface adsorption or instantaneous adsorption stage. The second portion is the gradual adsorption stage, where intra-particle diffusion is rate-controlling. The third portion is the final equilibrium stage where intra-particle diffusion starts to slow down due to extremely low adsorbate concentrations in the solution. Figure 11 shows a plot of the linearized form of the intra-particle diffusion model at all concentrations studied. The values of intercept C provides information about the thickness of the boundary layer; the resistant to the external mass transfer increases as the intercept increases. The constant C was found to increase from with increase in initial concentration from 50 to 200 mg L-1 onto HAN, indicating the increase of the thickness of the boundary layer and decrease of the external mass transfer and hence increase in the chance of internal mass transfer. The R2 values are close to unity indicating the applicability of this model. This may confirm that the intra-particle diffusion is the rate-limiting step.

As can be seen from Table 3, the pseudo second-order kinetic model provided the best correlation for all of the adsorption process, whereas the intra-particle diffusion model fit the experimental data well for an initial period of the adsorption process only. Hence, it was concluded that the pseudo second-order kinetic model represented the rate-limiting step in adsorption, followed by the intra-particle diffusion model. Similar phenomena have also been observed in adsorption of chrome dye (OCRME) on mixed adsorbents-fly ash and coal (Gupta et al. 1990), in adsorption of phenols on fly ash (Singh and Rawat1994), in adsorption of lead (II) on cypress leaves (Salim et al. 1994), and in adsorption of chromium (VI) on the activated carbon prepared from agricultural wastes (Demirbas et al. 2002).

Fig. 11. Intraparticle diffusion for adsorption of Cr(VI) onto HAN

Table 3. Kinetic Parameter for the Adsorption of Cr(VI) onto HAN

Batch Studies of Binary and Ternary Metal System (BMS & TMS)

In the BMS system, one metal ion (Cr(VI) was used as the main metal, the initial concentration of which was made to remain unaltered while the other two metal ion (Co2+ and Cu2+) concentrations were varied from 10 to 50 mg L-1 to determine the maximum adsorption. The proposed binary mixtures were in the following combinations: Cr-Co and Cr-Cu, whereas a grouping of Cr-Co-Cu was taken as a ternary aqueous phase. The adsorption experiment was carried out in the similar fashion as was performed for SMS. Figure 12 shows that there was a considerable reduction in metal sequestering ability of the adsorbents in binary and tertiary metal systems in comparison with single metal systems. Thus, in the case of binary metal system, the HAN exhibits the highest decline of 47% in adsorption efficiency for Cr-Cu than Cr-Co – 60% compared to 97% percentage removal of Cr(VI) in SMS which is shown in Fig. 12. It was observed that there was a reduction of 68% in Cr(VI) uptake efficiency of HAN in TMS in contrast to metal confiscating potential in SMS (97%). In other words, the percentage adsorption of Cr(VI) in TMS was only 29%.

The results for binary and ternary systems showed clearly that the combined action of multiple ions was antagonistic. Thus, the metal removal efficiency was greater in the single component system in comparison with multiple component one. This is probably due to the absence of competitive processes between metal and adsorbent in a single component system (Kovacevic et al. 2000). The most likely reason for the antagonistic effect is the competition for adsorption sites on the cell surfaces and /or the screening effect by the competing metal ions (Sheng et al. 2007). Results of the present research shows that Cr(VI) adsorption is affected by Cu followed by Co. A similar phenomenon had been observed in the binary adsorption of Pb(II), Cu(II), Cd(II), and Ni(II) with the heterogeneous adsorbents (Papini et al. 2004; AmnaShoaib et al. 2011).

Fig. 12. Adsorption of Cr(VI) onto HAN in binary system

Desorption

The regeneration of the adsorbent and/or disposal of the adsorbate-loaded adsorbent (or spent adsorbent) is very important. It has potential to make the treatment more economical and feasible. Desorption helps to elucidate the mechanism of metal adsorption and recycling of the spent adsorbent and the metal. In the present study, HAN was regenerated and is used for the removal of Cr(VI) at different pH range (1 to10). Cr(VI) adsorption is an example of physical adsorption, and it is possible to regenerate the HAN, which can be considered for reuse.

Fig. 13. Desorption of Cr(VI) onto HAN

The adsorption of Cr(VI) onto HAN was found to be dependent on pH, such that increased desorption of Cr(VI) was accomplished by increasing the solution pH. The maximum desorption of Cr(VI) onto HAN is obtained at pH 8 (Fig. 13), which is consistent with electrostatic repulsion between negatively charged Cr(VI) ions and the negatively charged cellulosic surface expected under such conditions. In addition, the fact that no more than 50% of the chromium could be desorbed throughout the pH range studied supports a hypothesis that at least some of the Cr(VI) had been converted to Cr(III) during the process of adsorption. Desorption of metal ions by aqueous solutions reveals that the metal ions were adsorbed onto the adsorbent through an ion-exchange mechanism.

CONCLUSIONS

  1. It was shown that Acacia nilotica leaves (HAN) can serve as an effective adsorbent for the removal of Cr(VI) metal ion from aqueous solutions. The equilibrium adsorption was achieved in 120 min for adsorption of Cr(VI) onto HAN at pH 3.
  2. The removal efficiency increased with an increase in agitation time and with initial concentrations.
  3. Freundlich isotherm model fit well with the adsorption data, and the adsorption kinetics could be successfully fitted to the pseudo-second-order kinetic model with intra-particle diffusion as one of the rate-limiting steps.
  4. Desorption and recycling ability of HAN was observed to be good. Therefore, the eco-friendly adsorbent HAN is expected to be environmentally and economically feasible for the removal of Cr(VI) from aqueous solutions.

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Article submitted: May 26, 2012; Peer review completed: August 2, 2012; Revised version received and accepted: January 25, 2013; Published: February 20, 2013.