3.1. Characterization of the resin
An energy-dispersive X-ray spectroscopy (EDX), scanning electron microscopy, and Fourier transform infrared (FTIR) spectroscopy were used to evaluate the resin's chemical and physical characteristics.
3.1.1. Fourier transformed infrared (FTIR) spectroscopy
FT-IR analysis was performed to display the structure of Amberlite (IRA 400) resin both prior to and during the sorption of Se(IV). The resulting spectrums have been recorded and presented in Fig. 1(a, b). Styrene-divinylbenzene polymeric matrix,s spectra exhibit a prominent peak at 3426 cm−1, which may be ascribed to –OH, as illustrated in Fig. 1a. The asymmetric C−H stretching vibrations of CH2 and CH3 in CH3−N are responsible for the band at 2923 cm−1 [28]. Furthermore, many peaks are seen at 1637, 1513, 1380, 1262, 1030, and 520 cm-1. These could be related to the C–X and –C–C– functional groups, as well as the C=O, S=O, and C−N stretching vibrations of benzene rings. The peaks at 1030 and 890 cm−1, respectively, are caused by the C–O and C–H bonds. Upon comparing the spectra, the FT-IR spectrum of Amberlite (IRA 400) following Se(IV) adsorption is displayed in Fig. 1b, exhibiting several discernible alterations. These modifications (at 1625, 1262, and 1024 cm-1) could therefore be the result of Se(IV) binding to adsorbent.
Figure 1
3.1.2 Scanning electron microscopy (SEM)
SEM at 50X magnification is used to examine the surface appearance of Amberlite (IR 400), as shown in Fig. 2(a, b) prior to and following the adsorption of Se(IV). It is evident that the particles in Amberlite (IR 400) have smooth, spherically-shaped surfaces. However, the surface structure following the adsorption of Se(IV) revealed a few small surface fissures rather than changes in the particle's shape, which roughly demonstrates the resin's durability.
Figure 2
3.1.3 Energy Dispersive X-ray spectroscope (EDX)
Figure 3(a, b) displays the Amberlite (IR 400) EDX spectrum both before and after the adsorption of Se(IV). Based on the EDX examination, the main components of Amberlite (IR 400) (Fig. 3a) include C (78.35%), N (7.39%), O (3.19%), and Cl (11.07%).Additionally, components C (74.29%), N (5.37%), O (3.79%), Cl (15.26%), and Se (1.29%) were detected in the Amberlite (IR 400) EDX spectrum following Se(IV) adsorption (Fig. 3b). The presence of Se elements in the loaded resin was verified by the EDX characterization.
Figure 3
3.2. Batch Sorption Studies
3.2.1. Effect of pH
Ionization characteristics of adsorbent's active sites are highly impacted by the adsorption media's pH [29]. The results of an examination into pH impact on the sorption percentage of Se(IV) from aqueous solution in the range of 1.0 to 8.0 are displayed in Fig. 4a.Upon increasing the pH from 1.0 to 3.0, it was observed that the sorption effectiveness improved from 14.92% to 80.25%. The sorption % then dropped as the pH increased.The Se(IV)speciation diagrams are displayed in Fig. 4b by the Hydra/Medusa chemical equilibrium software. Selenious acid (H2SeO3) is the main species of Se(IV) at low pH values, as this figure clearly illustrates. This explained the low values for the sorption percent at pH≤ 2. Furthermore, the dominating species biselenite (HSeO3-) emerged as the pH rose to 3.5. According to the data, the anionic resin employed in the experiment had positive charges (more H+ ions) at low pH values, which caused an electrostatic reaction to occur between the (HSeO3–) species and the resin surface's positive charge. Thus, pH 3.0 was used for the sorption process of selenium ions in the next study.
Moreover, the sorption process is accelerated at pH 3 due to the resin's chemical makeup, which includes amino functionalities in its –R3N+Cl- structure. As shown in Fig. 4c, an ion exchange reaction may be used to carry out this procedure [30, 31]. As zero-point charge verified it. At pH 3, the resin's zero-point charge (pHzpc) was determined (Fig. 4d).The sorbent surface holds positive charges at pH less than pHzpc, which increases the electrostatic attraction force with biselenite (HSeO3-). The proposed mechanism is clarified in Fig. 4c.
Figure 4
3.2.2. Effect of Shaking time
One of the most crucial factors to consider when developing a batch sorption experiment is the rate of sorption. It affects removal efficiency, contributes to contact time optimization, supports kinetics modeling, and contributes to establishing suitable experimental conditions. In each experiment, contact duration influence on selenium sorption were investigated at pH 3.0, starting concentration of 100.0 mg/L, and adsorbent mass of 10 mg. Figure 5a shows the evaluation of Se(VI) sorption as a function of shaking time, with 1.0–60.0 min, on the Amberlite IR 400 resin. Upon increasing the shaking period from 1.0 to 10.0 min, we find that the sorption percentage of Se(IV) rises from 69.62 to 82.10%. Following that, the sorption percentage held steady for 60 minutes.
The selenium adsorption process onto Amberlite IR 400 resin has been explained by two primary linear kinetic models: the pseudo-first-order model and the pseudo-second-order model (see Fig. 5b,c). Table 3 summarizes the correlation coefficient (R2) and several parameters of these kinetic models. Based on R2 = 0.999, the correlation index for pseudo-second-order is seen to be close to the unit. Furthermore, the experimental result, qe EXP = 4.11 mg/g, and the calculated qeCAL = 4.12 mg/g values match quite well. These results demonstrated that the Se(VI) adsorption on Amberlite IR 400 is adequately explained by the pseudo-second-order model.
Figure 5
Table 3
3.2.3. Effect of initial selenium ion concentration
Figure 6a illustrates how the initial concentrations of selenium affect the sorption %. With an increase in Se(VI) starting concentration from 100.0 to 200.0 mg/L, we observed a decrease in Se(VI) sorption percentage from 81.27 to 67.0%. These outcomes can be explained by the fact that, at low starting concentrations of Se(VI), there are comparatively less Se(VI) species in the solution than there are binding sites available overall on the adsorbent's surface. A high sorption efficiency results from the fact that there When more Se(VI) is introduced to the system at higher initial concentrations, the number of Se(VI) species in the solution increases but the number of binding sites remains constant. The sorption efficiency will consequently directly decline.
3.2.4. Sorption isotherm and modeling
In order to estimate Se(IV) ions interactions on adsorbent surface, adsorption isotherms at equilibrium are crucial.The experiment's outcomes were assessed using a variety of linear isotherm models.Table 4 displays the values calculated using the Se(VI) sorption slopes and intercepts obtained from Fig. 6b, c. Selenium species prefer to adsorb as a monolayer onto Amberlite IR 400 active sites, as evidenced by Langmuir model's maximum correlation coefficient of 0.999.
Figure 6
Table 4
3.2.5. Effect of adsorbent dose
Figure 7 illustrates the impact of Amberlite IRA 400 resin on Se(VI) sorption efficiency in the range of 0.10-0.20 g. After increasing adsorbent dosage from 0.10 to 0.20 g, the experiment's results showed that Se(VI)'s sorption performance increased from 81.44% to 86.62%. The higher dosage of adsorbent will result in larger active sites being accessible for selenium sorption, which is why there was a reported increase in sorption.
Figure 7
3.2.6. Effect of solution Temperature
Figure 8a shows how temperature changes between 25 and 65 °C affect the percentage of selenium that is soluble in aqueous solutions. It is demonstrated that as the temperature increases, the adsorption percentage increases gradually. It is well known that increasing the temperature increases the rate at which the sorbent molecules diffuse through the sorbent particle's interior pores and outside the boundary layer. The Ln Kd vs T-1 linear plot shown in Figure 8b's slope and intercept indicate the values of ΔHo and ΔSo, as well as the thermodynamic parameter (ΔGo), were computed. The parameters' respective values are listed in Table 5. This table shows that selenium adsorption occurs readily and spontaneously on Amberlite IRA 400 resin, as demonstrated by the negative ΔGo values. As suggested by negative ∆H° value, the adsorption process is exothermic in nature. Furthermore, positive ΔS° indicated an increase in the system's randomness.
Figure 8
Table 5
3.2.7. Desorption studies
The desorption of Se(IV) from loaded Amberlite IRA 400 resin was also performed with several desorbing agents of different concentrations. The desorbing agents used included sodium acetate, nitric acid, and hydrochloric acid. According to Table 6's data and findings, 1.0 mol/L of nitric acid, 1.0 mol/L of HCl, and 1.0 mol/L of sodium acetate were all necessary to produce a maximum Se(IV) desorping of 96.40%.