Characterization
SEM analysis
The surface morphology of the magnetic composite gel spheres was dense and slightly rough, as shown in Fig. 1(a), which facilitates contact with Zn(II), mainly due to the cross-linking of the carboxyl group on SA with Ca2+ in the solution. As shown in Fig. 1(b), the internal mesh structure of SML with more folds provides a channel for Zn(II) to enter the gel sphere and expand the contact area between the target ions and adsorption sites. Figs. 1(c) and 1(d) show that Fe and N were evenly distributed on the surface, indicating that Fe3O4 and L-met were uniformly distributed on the adsorbent.
FTIR analysis
The structure of the SML is shown in Fig. 2(a). The vibrational peak at 3430 cm−1 is caused by the stretching of the -OH group vibration (Lin et al. 2012), indicating the presence of water crystallization in the magnetic composite gel spheres. The C-H group adsorption peak was observed at 2930 cm−1. The vibration bands at 1421 cm−1 and 1510 cm−1 represent the bending vibration peaks of the -COO and N-H bonds, respectively, indicating the presence of L-methionine in the composite material. The stretching bond, appearing near 580 cm−1, belongs to the peak of Fe-O, and it shows that Fe3O4 loaded successfully in the composite material (Jiang et al. 2013).
Thermogravimetric analysis
As shown in Fig. 2(b), the entire pyrolysis process of SML exhibited four weightlessness stages, and peaks appeared at 190, 290, 520, and 750°C. First, the weightlessness stages observed from room temperature to 190°C were mainly due to the reduction of free water, and the corresponding percentage of weightlessness was approximately 15.96%. Second, the relative weight loss of the magnetic adsorbent was approximately 29.45% for temperatures ranging from 190 to 290°C, which is related to the skeleton breakage of calcium alginate and the removal of the adjacent hydroxyl groups. Next, decomposition and carbonization of some carboxyl functional groups from 290 to 500°C caused a weight loss of approximately 11.15%. Finally, near 11.45% of weightlessness occurs under 520 to 750°C, which indicates further oxidation and decomposition of calcium alginate.
Magnetic property analysis
Hysteresis lines of Fe3O4 and SML were measured using a magnetometer to determine whether the resulting magnetic composite gel spheres could be separated quickly from water under an applied magnetic field.
In Fig. 2(c), both samples appear superparamagnetic and do not show hysteresis; the saturation magnetizations of SML and Fe3O4 are 72.92 emuˑg−1 and 4.84 emuˑg−1, respectively. Although the surface of the material is covered by SA, which degrades the magnet response performance, it maintains good performance and does not affect the magnetic separation effect. Under the condition of an applied magnetic field (0.4 T), a solid–liquid can be separated rapidly, facilitating recycling after adsorption and reducing the risk of secondary contamination.
Adsorption
Effect of pH on the adsorption of Zn(Ⅱ)
Figure 3(a) shows the effect of pH on the adsorption ability of SML in simulated wastewater. In the beginning, the adsorption capacity increases as the pH increases; at pH=5, maximum adsorption ability is 89.9 mgˑg−1; when pH=2, the adsorption effect of the adsorbent is poor. This is because the competitive adsorption between H+ and Zn2+ causes the carboxyl group, and the reduction of amino groups seriously affects the effect of SML. Because the functional group is protonated, the effect of electrostatic repulsion is increased, which interferes with Zn(II) adsorption. As pH increases, H+ decreases to a large extent, the amino and carboxyl groups are rapidly deprotonated, and the electrostatic repulsion is gradually reduced, which increases the adsorption capacity of the gel spheres. When pH=6, the solution produced white precipitate Zn(OH)2, which is not conducive to adsorption with the gel ball; therefore, the adsorption capacity decreased.
Effect of SML dosage on the adsorption of Zn(II)
Figure 3(b) presents the effects of SML dosage on target metal ion adsorption capacity. In this section, the removal rate increased as the SML dosage increased. The removal rate was nearly 70% when the dosage was 0.7 g·L−1, and the adsorption capacity remained at a high level with a slight decrease. A reasonable conclusion is that increasing the gel ball improved the adsorption properties and contact area with heavy metal ions. When the dosage of magnetic adsorbent reached 2 g·L−1, the removal efficiency was 90.14%, and the removal rate increased, whereas the adsorption capacity decreased. This finding can be explained as follows: excess adsorption sites on the gel ball lead to a decrease in the unit adsorption capacity. Thus, 0.7 g·L−1 is the optimal dosage of SML based on the adsorption capacity and removal rate.
Effects of initial concentration on adsorption of Zn(Ⅱ) on different materials
The adsorption performance improved with the increase in the initial concentration of Zn(II), as shown in Fig. 3(c), because the electrostatic gravitational force also gradually increases, and the adsorption sites of the gel spheres are easily occupied (Hongyu et al. 2015). The increase in adsorption gradually decreased at 200 mgˑL−1 to 500 mgˑL−1 and tended to reach equilibrium. Moreover, adsorption with gel spheres on metal ions encapsulated with L-met at initial concentrations of 20 mgˑL−1 to 500 mgˑL−1 is significantly higher than that of SA and SA@Fe3O4. This result demonstrates that the loading of L-met increases the effective functional groups of the gel spheres for heavy metal adsorption, which increases the quantity of adsorption spots of the material, improving the adsorption efficiency. The reason for the greater adsorption of SA than SA@Fe3O4 is that the nanoscale Fe3O4 in the gel spheres limits the contact of metal ions in solution with the sites, reducing the adsorption capacity of the material(Zhang et al. 2013).
Effect of time on adsorption of Zn(II) by SML at various starting concentrations
As shown in Fig. 3(d), the effect of SML on Zn(II) exhibited a rapid increase with the increase of adsorption time over 30 min. The leading cause of this situation is that the gel sphere has sufficient adsorption sites occupied by heavy metal ions, and there is a large concentration difference between the inside and outside of the gel sphere during the early period of adsorption. Metal ions diffuse rapidly to the surface of the gel sphere; some target heavy metals enter the gel sphere through ion exchange; and the higher the concentration gradient of the solution, the greater the driver will be at the beginning. Thus, the greater the original concentration of the metal, the faster the adsorption rate of the material. The amount of Zn(II) adsorbed by SML reached 302.12 mg-L−1 at 60 min, close to the adsorption equilibrium amount. After 60 min, the adsorption sites of Zn(II) gradually saturated, and the concentration difference between the heavy metal inside and outside the adsorbent decreased, which reduced the adsorption driver and led to gradual degradation in the adsorption rate. Additionally, the number of available adsorption sites on the material also slowly decreased, and this did not facilitate the adsorption process; thus, the adsorption capacity increased slowly and tended to dynamic equilibrium.
Adsorption kinetics analysis
Saturated adsorption of SML was 29.82, 51.2, 83.92, 86.84 mg·L−1 at 20 to 200 mg·L−1, respectively.
Table.1 Calculated kinetic parameters for adsorption of Zn(II) by SML
Co(mg·L−1)
|
Pseudo-first-order kinetic model
|
Pseudo-second-order kinetic model
|
|
Qe(mg·g−1)
|
k1
|
R2
|
Qe(mg·g−1)
|
k2
|
R2
|
20
|
47.74
|
0.0895
|
0.9782
|
42.70
|
0.00348
|
0.993
|
50
|
95.12
|
0.0411
|
0.9753
|
94.61
|
0.00281
|
0.999
|
100
|
161.9
|
0.0237
|
0.9152
|
164.9
|
0.00194
|
0.999
|
200
|
323.1
|
0.0229
|
0.9223
|
328.8
|
0.00129
|
0.999
|
As shown in Table 1, the higher value of the regression coefficient for the pseudo-second-order model than that of the other models confirms this finding. The kinetics of Zn(II) adsorption by SML were governed by chemisorption.
Adsorption isotherms analysis
Table.2 Relevance parameters of SML for Zn(II) adsorption
Temp(℃)
|
Langmuir
|
Freundich
|
Qmax(mg·g-1)
|
kL(L·mg-1)
|
R2
|
RL
|
kL(L·mg-1)
|
n
|
R2
|
25
|
85.13
|
0.0618
|
0.995
|
0.0512
|
16.974
|
3.029
|
0.764
|
35
|
90.83
|
0.0671
|
0.997
|
0.0472
|
19.221
|
3.210
|
0.785
|
45
|
93.15
|
0.0762
|
0.997
|
0.0419
|
20.921
|
3.331
|
0.789
|
55
|
96.01
|
0.0761
|
0.997
|
0.0420
|
21.217
|
3.165
|
0.836
|
The results in Table 2 indicate that the reaction process of SML shows a relatively higher correlation in the Langmuir adsorption isotherm equation than in the Freundlich adsorption isotherm equation. The coefficients of determination R2 were all greater than 0.99, indicating that the monomolecular layer of SML after adsorption formed uniformly adsorbed onto the surface material. The separation constant at different temperatures was in the range of 0 < RL < 1, indicating that the reaction process can proceed easily. Kf in the Freundlich model increased gradually from 25 to 55 °C, indicating that the increase in temperature can promote the adsorption reaction.
Adsorption thermodynamic analysis
Table.3 Fitting parameters for adsorption thermodynamics of Zn(II) by the SML
Temp(℃)
|
kF
|
∆G/(kJ·mol-1)
|
∆H(kJ·mol-1)
|
∆S/(J·mol-1)
|
25
|
115.329
|
-11.762
|
|
55.804
|
35
|
121.857
|
-12.299
|
4.8667
|
55.732
|
45
|
129.423
|
-12.857
|
55.702
|
55
|
138.027
|
-13.437
|
|
55.654
|
Table 3 shows that ΔG is -7.019,-7.573,-8.043, and -8.334 kJ·mol-1 at 25–55 °C, indicating that the gel sphere adsorption process is spontaneous. The entropy characteristics (ΔS) listed in Table 3 indicate that the adsorption reaction is a process of entropy increase. The enthalpy change(ΔH) is 4.866 kJ·mol-1, indicating that the sorption of Zn(II) belongs to the heat absorption process.
Cycle performance
Figure 4 shows the cycle performance of the magnetic composite gel spheres. In this section, SML was used to conduct five adsorption-desorption experiments in 0.1 mol·L−1 HNO3.
As shown in Fig. 4, some of the adsorption sites occupied by H+ are released and exposed again, and the adsorption capacity of the magnetic adsorbent on Zn(II) reaches 58.65 mgˑL−1 after five adsorption-desorption experiments. The concentration of Fe in the experiment’s solution is 0.24 ± 0.02 mg·L−1, and the leaching rate is 0.0629%. This phenomenon indicates that SML can still maintain good adsorption capacity after times adsorption-desorption experiments, with a low waste rate of Fe. Additionally, the stability of SML does not cause the threat of the instant release of heavy metals.
Effect of coexisting ions
Effect of increasing total amount of Pb(Ⅱ) on adsorption of material to Zn(Ⅱ)
Zn(II) concentration in the solution system was limited to 50 mg-L-1; the changes in sorption of two heavy metals by SML were investigated by increasing the concentration of Pb(II); and the Zn(II):Pb(II) concentration ratios were set to four concentration ratio gradients: 50:10, 50:25, 50:50, and 50:100.
As shown in Fig. 5(a), the adsorption of Pb(II) showed an increasing trend when the Pb(II) concentration in the solution system gradually increased from 10 to 100 mg. The adsorption amount of Zn(II) decreased from 30.26 to 18.73 mg, which indicated that interfering Pb(II) influenced the adsorption of magnetic composite gel spheres on Zn(II), and SML has preferential adsorption on Pb(II).
Effect of increasing total amount of Pb(Ⅱ) on adsorption of material to Pb(Ⅱ)
The concentration of Pb(II) was limited, and the variation of SML on Pb(II) adsorption was investigated by increasing the concentration of Zn(II) in the system. As shown in Fig. 5b, when the interfering ion concentration was increased from 10 to 100 mg, there was no influence on the sorption of Pb(II) by SML, and the amount of Pb(II) sorption remained at approximately 50 mg. As the concentration of exogenous ion Pb(II) increased, although the amounts of Zn(II) adsorbed steadily increased to 37.81 mg, they were still much lower than those of Pb(II) adsorption. This difference might be mainly because the ionic radius of Pb(II) is 119 pm, which is greater than that of Zn(II) (83 pm); therefore, the polarization force is smaller for Pb(II) ions than for Zn(II), which facilitates complexation with functional groups and thus preferential adsorption on Pb(II). Zhu et al.(2012) prepared modified chitosan magnetic gel spheres and found that the order of competing order was Pb(II) > Zn(II), and our experimental findings are in agreement with this conclusion.
Adsorption mechanism
BET analysis
The results of the pore size distribution and adsorption-desorption isotherms are presented in Figure 6. Fig. 6(a) shows that the relative surface area of the SML is 10.11 m2/g, average pore size is 20.02 nm, and pore volume is 0.0182 cm3·g−1, indicating that this material is mesoporous. The adsorption-desorption curves of SML were drawn by changing the pressure and using the BJH method in the nitrogen condition, and the appearance of the hysteresis loop at 0.65 P/Po reveals that the magnetic adsorbent has slit-like holes formed by a loose polymer. Additionally, in Fig. 6(b), the curve belongs to the H3 hysteresis loop(Liu et al. 2005), and this conclusion is consistent with the material properties of SA polymer. The absence of adsorption limitation in the relatively high-pressure region indicates that the present material is a mesoporous material with a relatively superior adsorption performance.
XPS analysis
Figure 7 shows the elements change on SML before and after the adsorption of Zn (Ⅱ). As revealed in Figure 7(a), the Zn2p peak appeared, and the strength of Ca2s peak weakens after adsorption, indicating an ion exchange in the adsorption system of the Ca and Zn. The change in N1s peak is shown in Figure 7(b). The binding energy of amino shifted from 400.13 to 399.18 ev, which shows that the nitrogen-containing groups in L-met were involved in the reaction. The spectrum of O1s is presented in Figure 7(c). A shift in the binding energy of C=O-O, C-O, and C=O shifted from 533.9 eV, 532.9 eV, and 531.7 eV to 534.06 eV, 532.77eV, and 531.55 eV, respectively, which indicated that the binding energy of oxygen-containing groups has changed after adsorption. We conclude that oxygen-containing groups coordinated with Zn(Ⅱ)(Sun et al. 2019). Additionally, FTIR analysis results showed the presence of carboxyl and amino groups, confirming that these two groups are participating in the adsorption process of heavy metal ions. The Zn2p spectrum in Figure 7(d) is composed of two peaks, representing the formation of Zn-O and Zn-N. According to the Lewis acids and bases and hard-soft-acid-base theory, the existence of electron-donating groups is the reason for the adsorption of the material and the divalent metal ion. The transfer of O and N lone pairs of electrons during the adsorption process causes changes in binding energy, indicating that the donor atoms (O and N) have a coordination effect with Zn(Ⅱ)(Matlock et al. 2002). Additionally, the adsorption process is affected by the ion exchange effect of Ca(II).
Concentration analysis of Ca(II) after adsorption of SML on Zn(II)
The concentration of Ca(II), shown in Fig. 8, is after the adsorption of SML on Zn(Ⅱ). The sorption ability of SML for Zn(II) was 1.128 mmol·g−1, and the release of Ca(II) in the adsorbent was 0.6258 mmol at a concentration of 100 mg·L−1. At this concentration, the capacity of adsorption and release of Ca(II) in SML tended to balance, and the contribution of ion exchange in adsorption was approximately 48.98%. We conclude that the Ca(II) in the gel spheres underwent ion exchange with heavy metal and separated into solution, whereas the Ca(II) used to cross-link was unable to react with heavy metals.