3.1. Morphology of the adsorbents
The morphology of MgLaFe LDO, MnO2 NW, and MnO2@LDO composite was observed by SEM and TEM. Figure 1a showed that the MgLaFe LDO exhibits lamellar agglomerates produced by stacking 2D nanosheets, as shown in the TEM image, which displays stacked nanosheet aggregates. Figure 1b displayed the uniform length of the α-MnO2 nanowires, also shown as a hollow tubular material in the TEM image. Figure 1c displayed the uniform wrapping around most of the nanowires, exhibiting core-shell material characteristics of MnO2@LDO. Additionally, as seen from the TEM image, many tiny sheet materials were distributed on the surface of the wrapped nanowires.
Figure 1.
SEM and insetted TEM images of (a) MgLaFe LDO, (b) MnO2 NW, and (c) MnO2@LDO.
Figure 1.
SEM and insetted TEM images of (a) MgLaFe LDO, (b) MnO2 NW, and (c) MnO2@LDO.
3.2. Characterization of the adsorbents
The crystal structures of MgLaFe LDO, MnO2 NW, and MnO2@LDO composites were characterized by XRD, as presented in Figure 2. The diffraction peaks of MnO2@LDO were consistent with those of MnO2. Still, the 2θ of all peaks is shifted to the left by about 0.6◦ overall, indicating that the lattice has been stretched by the stress of the interstitial atoms. The intensity of the peaks on the (110) and (131) crystal planes decreased, implying successful immobilisation of LDO on MnO2. The characteristic diffraction peaks of 12.8◦, 18.1◦, 28.7◦, 37.6◦, 42.0◦, 49.9◦, 56.2◦, 60.2◦, 65.5◦, 69.6◦, and 73.1◦ corresponded to the (110), (020), (131), (211), (031), (141), (060), (251), (002), (541), and (132) crystal planes of α-MnO2 (PDF#98-002-0227), respectively. The sharp shape indicated that the sample had good crystallinity. In contrast, the diffraction patterns of MgLaFe LDO exhibited characteristics of amorphous metal (hydro)oxides.
Figure 2.
XRD patterns of MgLaFe LDO, MnO2 NW, and MnO2@LDO.
Figure 2.
XRD patterns of MgLaFe LDO, MnO2 NW, and MnO2@LDO.
Figure 3 showed the FT-IR spectra of MgLaFe LDO, MnO
2 NW, and MnO
2@LDO. The observed bands ranging from 400 to 1000 are attributed to O-M-O, O-M, and M-O-M bonds (M= Mn, Mg, La, and Fe)[
29]. The bands below 1000 were improved in MnO
2@LDO as opposed to MnO
2 NW. Moreover, the absorption peak of MnO
2 NW at 725 cm
-1 showed a shift to 712 cm
-1, perhaps due to surface loading of LDO. The LDO's specific CO
32- absorption peaks were also evident at 1420-1490 cm
-1[
30]. The bending mode of the H-O-H bond on the metal hydroxides and adsorbed water appeared at 1640 and 3450 cm
-1[
31], respectively. By contrast, the MgLaFe LDO demonstrated absorption peaks of CO
32- and adsorbed water, with the vibration of metal oxide M-O also visible in the 700-720 cm
-1 absorption band[
32]. In the comparison, the MnO
2@LDO surface exhibited more metal (hydro)oxides and LDO's typical CO
32- intercalation feature.
Figure 3.
FT-IR spectra of MgLaFe LDO, MnO2 NW, and MnO2@LDO.
Figure 3.
FT-IR spectra of MgLaFe LDO, MnO2 NW, and MnO2@LDO.
As shown in
Figure 4, the adsorption isotherms of IV-type were observed. The hysteresis loops of MnO
2@LDO and MgLaFe LDO belonged to type H3, whereas the MnO
2 NW hysteresis loop was of type H4. Both H3 and H4 had a combination of micropores and mesopores, which arose mainly from irregular pore structures, including cracks and slits. The H3 hysteresis loop, in particular, corresponded to surfaces with more flat plate slit structures and wedge structures, which were typical of LDO structures[
33]. The justification for the presence of the H3 hysteresis loop lay in the numerous irregular voids caused by stacking and the high concentration of loaded MgLaFe LDOs featuring lamellar flat plate slit structures, as evidenced by the SEM images of MnO
2@LDO (
Figure 2c). The surface area had increased from 38.4 m2/g to 114.5 m2/g. This increase in surface area could be due to the reduction in the packing of MnO
2 by LDO, resulting in a further increase in porosity. The larger surface area led to an increased contact reaction area, which was beneficial for adsorption. Although MgLaFe LDO possessed a larger specific surface area, the effect of the specific surface area on the adsorption process would be further analyzed by adsorption performance.
Figure 4.
N2 adsorption-desorption isotherm curves of MgLaFe LDO, MnO2 NW, and MnO2@LDO.
Figure 4.
N2 adsorption-desorption isotherm curves of MgLaFe LDO, MnO2 NW, and MnO2@LDO.
3.3. Evaluation of adsorption performance
The adsorption abilities of As(Ⅲ), As(V), and F- were investigated using samples of MgLaFe LDO, MnO2 NW, and MnO2@LDO as adsorbents. The experimental conditions were: adsorbent amount was settled as 0.5 g/L according to the preliminary experiment, As(Ⅲ) concentration 5 mg/L, As(V) concentration 5 mg/L, F- concentration 100 mg/L, experimental temperature 303K, reaction time 480 min.
Figure 5a indicated that the adsorption of As(Ⅲ) by MnO2 NW had a high oxidation efficiency, resulting in a high As(Ⅲ) removal rate of 15.8% during early adsorption stages. However, this increase was only 14.8% for As(V), implying that As(Ⅲ) was almost entirely oxidized to As(V). The MgLaFe LDO demonstrated improved adsorption for As(V) and F-, while revealing inadequate adsorption for As(Ⅲ). This was because the LDO material, being an anionic adsorbent, cannot effectively adsorb As(V) presented in the molecule. The adsorption performance of MnO2@LDO on As(Ⅲ), As(V), and F- was improved by 18.1%, 7.0%, and 7.3%, respectively, compared to that of MgLaFe LDO after 10 min of reaction.
As Figure 5b shown, the removal rate for As(V) was merely 27% as most of the As(Ⅲ) underwent oxidation to As(V), with limited oxidation of As(Ⅲ) because of the competition for the adsorption sites on the MnO2 NW surface. And MnO2 NW's removal of F- was less efficient. The MgLaFe LDO exhibited additional adsorption of As(V) and F- while the adsorption effect of As(Ⅲ) remained relatively stable, similar to that observed at 10 min. MnO2@LDO demonstrated superior efficacy in eliminating As(Ⅲ), As(V), and F- after a 480 mins reaction. The underlying cause for this higher removal rate could be attributed to the heterogeneous structure of MnO2@LDO, which possessed increased oxidation capabilities and anionic adsorption properties. Therefore, MnO2@LDO was selected as the adsorbent for further study.
Figure 5.
Individual adsorption performance of As(Ⅲ), As(V) and F- in absorbent MgLaFe LDO, MnO2 NW, and MnO2@LDO after (a) 10 mins, (b) 480 mins.
Figure 5.
Individual adsorption performance of As(Ⅲ), As(V) and F- in absorbent MgLaFe LDO, MnO2 NW, and MnO2@LDO after (a) 10 mins, (b) 480 mins.
3.4. Effect of solution pH
Figure 6 displayed the adsorption of As (Ⅲ), As (V), and F- based on the pH of the solution. The pH values were consistently maintained at a range of pH 3 to pH 11 while keeping other parameters constant (initial concentration of As (Ⅲ) 5 mg/L, As (V) 5 mg/L, F- 100 mg/L; contact time 480 mins; adsorbent dosing 500 mg/L). The findings indicated that the highest As (V) intake occurred within a pH range of 5-6, whereas As (Ⅲ) intake displayed a comparable pattern. The reason behind the similar trend of As (Ⅲ) and As (V) could be the conversion of As (Ⅲ) to As(V) by MnO2 in the heterogeneous structure of the adsorbent; simultaneously, As(V) could be absorbed into the interlayers of LDO which anchored growth on the MnO2 surface. Additionally, F- was effectively adsorbed within a pH range of 4-6. A low pH could lead to the conversion of F- to hydrofluoric acid, making it challenging to adsorb. On the other hand, a high pH could result in a large number of hydroxides aggregating on the adsorbent material surface, occupying the adsorption sites containing deprotonated As (Ⅲ), As (V), and F-, causing a significant reduction in adsorption capacity.
Figure 6.
Effect of pH on As(Ⅲ), As(V), and F- adsorption by MnO2@LDO.
Figure 6.
Effect of pH on As(Ⅲ), As(V), and F- adsorption by MnO2@LDO.
3.5. Isotherm study
Isotherm models are commonly employed to describe the equilibrium interaction between adsorbates and adsorbents. The adsorption process occurring on the heterogeneous structure of MnO
2@LDO can be better explored by isotherm model fitting. The Langmuir isotherm model indicates that monolayer adsorption occurs on identical adsorbent sites. In contrast, the Freundlich isotherm model suggests multilayer adsorption occurs due to adsorptive interaction with various sites on the non-homogeneous adsorbent surface. The adsorption capacity for As (Ⅲ), As (V), and F
- under different solution concentrations was displayed in
Figure 7, and the characteristic constants were listed in
Table 1. The Langmuir model demonstrated better fitting for the adsorption process of As (Ⅲ), leading to the inference that As (Ⅲ) might mainly react on the MnO
2 surface within the heterogeneous structure. These findings aligned with the results from our experiments on adsorption performance. The Freundlich model demonstrated a better fit for the equilibrium results for As (V) and F
-. It suggested that multilayer adsorption occurred on the LDO and heterogeneous interface. In addition, since the nF parameter of the Freundlich model followed the order: As (Ⅲ) < F
- < As (V) < 1, which also suggested that the adsorption rate of As (V) was the most rapid and that chemisorption was predominantly present on all adsorbents. The MnO
2@LDO demonstrated excellent adsorption capacity compared to the present adsorbent, as illustrated in
Table 1, manifesting outstanding performance.
Figure 7.
The MnO2@LDO co-adsorption isotherms fitting of (a) arsenic and of (b) fluoride.
Figure 7.
The MnO2@LDO co-adsorption isotherms fitting of (a) arsenic and of (b) fluoride.
3.6. Kinetics study
The adsorption kinetic curves and parameters were presented in
Figure 8 and
Table 2. The adsorption rates of As (Ⅲ), As (V), and F
- were more rapid before 120 min, with removal rates of 63.4%, 78.2%, and 81.0%, respectively. The adsorption rate of As (Ⅲ) was higher than that of As (V) before 40 minutes, potentially due to the oxidation of most of the As (Ⅲ) to As (V) during the initial stage of adsorption, leading to the increment of As (V) concentration in the solution. After 480 minutes, the adsorption process reached stability, and As (Ⅲ), As (V), and F
- removal rates reached 99.1%, 100%, and 93.7%, respectively. Additionally, based on the R2 fitted by the kinetic model, the adsorption of As (Ⅲ) could be better described by pseudo-second-order, indicating that the chemisorption mainly governed the adsorption process. In contrast, the pseudo-first-order kinetic model better fitted for the adsorption of As (V) and F
-, suggesting that electrostatic interaction and ligand exchange also co-existed in the adsorption process.
Figure 8.
(a) Pseudo-first-order model fitting and (b) Pseudo-second-order model fitting with co-adsorption of As(Ⅲ), As(V), and F- on MnO2@LDO.
Figure 8.
(a) Pseudo-first-order model fitting and (b) Pseudo-second-order model fitting with co-adsorption of As(Ⅲ), As(V), and F- on MnO2@LDO.
3.7. Mechanism Study
The XPS measurements can detect the surface elemental composition, metal oxidation states, and adsorbed species of solid materials, providing critical information about binding mechanisms. In the spectrum of MnO
2@LDO (
Figure 9a), two significant new peaks were observed at As2p (1325 eV) and F1s (685 eV). The presence of these peaks indicated that the target ions were immobilized. As shown in
Figure 9b, the C1s spectra of MnO
2@LDO after adsorption were assigned as C=O, C-O, and C-C with binding energies of 288.3, 285.9, and 284.4 eV, respectively. There was a negative shift accompanied by a significant decrease in the intensity of C=O, which belongs to CO
32- between the interlayers of LDO in the heterostructure (
Table 4). It indicated that the interlayer CO
32- is replaced by the anion of As(V)/ F
-, thus assuming a free state. The O1s spectra before and after adsorption are displayed in
Figure 9c and assigned to C=O, C-O, and M-O. Positive shifts of different degrees were observed after adsorption, accompanied by a noteworthy reduction in C=O intensity. These observations indicated that the interlayer CO
32- in MnO
2@LDO was replaced during adsorption. It could contribute to its rapid adsorption of As(V) and F
-.
Figure 9.
MnO2@LDO before and after As(Ⅲ), As(V) and F- co-adsorption of (a) XPS survey spectra, high-resolution spectra of (b) C1s, and (c) O1s.
Figure 9.
MnO2@LDO before and after As(Ⅲ), As(V) and F- co-adsorption of (a) XPS survey spectra, high-resolution spectra of (b) C1s, and (c) O1s.
The XPS spectra for Mn 2p, Mg 1s, La3d 5/2, and Fe 2p before and after adsorption are presented in Figure 10. The Mn 2p 3/2 XPS spectra can be deconvoluted into four components with binding energies (BE) of 646.1, 642.5, 641.3, and 639.9 eV after adsorption (Figure 10a). These components could be attributed to the satellite peaks of the surface Mn 2+ species, and the Mn4+, Mn3+, and Mn2+ species, respectively. The typical satellite peaks produced by the Mn2+ shock effect were observed after adsorption, which indicated that significant redox reactions during the adsorption process accompanied the surface MnO2@LDO. Moreover, the molar ratio of Mn4+/(Mn3++ Mn2+) in MnO2@LDO (0.64) was significantly decreased after adsorption (0.49). It explained the efficient removal of As(Ⅲ) in the adsorption performance as well as the increase in As(V) at the beginning of adsorption. The intensity of the spectra of Mg1s in Figure 10b exhibited negligible alteration, while the binding energy revealed a negative shift of 0.1 eV. For the peaks in Figure 10c of La3d 5/2 and Figure 10d of Fe2p, there was a notable alteration in intensity. These findings implied that La and Fe have a significant chemisorption function in the adsorption of As(Ⅲ), As(V), and F-. It also further explained the results obtained in adsorption performance, isotherm fitting, and kinetic fitting.
Figure 10.
MnO2@LDO before and after As(Ⅲ), As(V) and F- co-adsorption XPS high-resolution spectra of (a) Mn2p; (b) Mg1s; (c) La3d 5/2; (d) Fe2p.
Figure 10.
MnO2@LDO before and after As(Ⅲ), As(V) and F- co-adsorption XPS high-resolution spectra of (a) Mn2p; (b) Mg1s; (c) La3d 5/2; (d) Fe2p.