3.1 Effect of different Fe3O4 loadings on adsorption
The effect of the addition of magnetic Fe3O4 nanoparticles to the structure of MIL-100(Fe) and MIL-101(Fe) was studied. In the synthesis of MIL-100(Fe) 0.05 g, 0.1 g, 0.15 g and 0.3 g of Fe3O4 were added and screened for the best ratio of adsorption efficiency. The adsorbents were tested for uptake of 50 mg L− 1 of Sb(III) from solution at pH = 7 and the results were shown in Table 1. Among all the nanoparticles in the synthesized ratios, the highest adsorption efficiency of 0.15g Fe3O4@MIL-100(Fe) could reach 41%, which was a 5% increase in adsorption as compared to the composite with the addition of 0.05 g Fe3O4.
Table 1
Adsorption efficiency of Fe3O4@MIL-100(Fe) with different ratios.
Adsorbent material | Adsorption rate (%) |
0.05 g Fe3O4@MIL-100(Fe) | 36% |
0.10 g Fe3O4@MIL-100(Fe) | 35% |
0.15 g Fe3O4@MIL-100(Fe) | 41% |
0.30 g Fe3O4@MIL-100(Fe) | 36% |
Similarly, in the synthesis of MIL-101(Fe) similarly 0.05 g, 0.1 g, 0.15 g, 0.3 g of Fe3O4 were added and screened for the best ratio of adsorption efficiency. The results were shown in Table 2. Among all the nanoparticles in the synthesis ratios, the highest adsorption efficiency of 0.15 g Fe3O4@MIL-101(Fe) could reach 73%, which was an 8% increase in adsorption compared to the composite material with 0.05 g Fe3O4 adding. It was experimentally tested that the material with this ratio was more magnetic, and easy to separate from the solution by an external magnetic field.
Table 2
Adsorption efficiency of Fe3O4@MIL-101(Fe) with different ratios.
Adsorbent material | Adsorption rate (%) |
0.05 g Fe3O4@MIL-101(Fe) | 65% |
0.10 g Fe3O4@MIL-101(Fe) | 70% |
0.15 g Fe3O4@MIL-101(Fe) | 73% |
0.30 g Fe3O4@MIL-101(Fe) | 64% |
3.2 Characterization
The XRD spectra of the two MOF samples were shown in Fig. 2(a)(b). The locations of the main diffraction peaks in the MIL-100(Fe) sample located at 2.14°, 4.28°, 4.92°, 6.11°, 10.35°, 11.48°, 12.62°, 17.96°, 18.96°, 19.25°, 20.11° ( Song et al., 2014; Ke et al., 2012). The XRD pattern of MIL-101(Fe) showed characteristic peaks of MIL-101(Fe) at 2θ = 5.18°, 8.78°, 9.36°, 18.98°, 23.7°. It was the same as previously reported (Liu et al., 2021), so it could be inferred that the successful synthesis of MIL-101(Fe) and MIL-100(Fe). The synthesized Fe3O4 comparison with a standard diffraction card (PDF#65-3107) showed matching peaks. The significant peaks of Fe3O4 are located at 2θ = 30°, 35°, 43°, 58° and 62°, corresponding to (220), (311), (400), (511) and (440), respectively. Moreover, the significant peak positions of Fe3O4 observable in Fe3O4@MIL-100(Fe), located at 2θ = 30°, 35°, 43°, 58° and 62°, respectively. The result proved the successful loading of Fe3O4 onto the MOF, which indicated that the sample was successfully prepared and had a good crystallinity (Ozkaya et al., 2009). Finally, the distinctive characteristic peaks of Fe3O4@MIL-101(Fe) were observed in the XRD image of the composite material, confirming the successful synthesis of the composite.
Using the N2 adsorption/desorption method, the specific surface area and pore size of two types of MOF materials were calculated using the isothermal adsorption model. The N2 adsorption/desorption curve of Fe3O4@MIL-100(Fe) rapidly rose in the P/P0 range of 0–0.2 and approached saturation, indicating a Type I adsorption isotherm. In most cases, this type of isotherm could prove that the material is a microporous material with a pore size of less than 2 nm. By using the corresponding formulas, the specific surface area of Fe3O4@MIL-100(Fe) was calculated to be 729.991 m2 g− 1, and the total pore volume was 0.323 cm3 g− 1. Both of the results reflected the high specific surface area and large porosity characteristics of Fe3O4@MIL-100(Fe). As shown in Fig. 2(d), the total pore volume and surface area of immobilized Fe3O4@MIL-101(Fe) were and 0.1 cm3 g− 1 and 141.3 m2 g− 1, respectively. A type IV isotherm with H1 hysteresis loop behavior is seen in the adsorption/desorption curve, which is typical of mesoporous materials. Mesoporous materials possessed a larger specific surface area than macroporous materials. Their larger pore size than microporous materials allowed them to adsorb large molecules without pore blockage, facilitating the transport of reactants or solvents. Therefore, they had greater selectivity for adsorbing antimony in different forms.
Our previous study found that under hydrothermal conditions, MIL-100 (Fe) particles had obvious angles, but their morphology was not regular. It has been shown that the addition of hydrofluoric acid (HF) during preparation could improve its crystallinity, obtain grains with larger morphology and more regularity. In Fig. 2(e), the dispersed particles of MIL-100(Fe) prepared in the experiment had a particle size of about 100–300 nm, and the particles were in a cluster-like morphology. Additionally, Fe3O4 nanoparticles loaded on top of the crystalline MIL-100(Fe) could be observed. The SEM of Fe3O4@MIL-101(Fe) showed that they formed a segregated and uniform octagonal structure. It was clearly visible that Fe3O4 was attached to the surface of MIL-101(Fe), with a crystal diameter of 1.6 ± 0.26 µm for MIL-101(Fe) and 63 ± 35 nm for Fe3O4. In addition, the structure and morphology of Fe3O4@MIL-101(Fe) were further explored using TEM analysis, as can be observed in Fig. 2(g). The individual crystals of MIL-101(Fe) and Fe3O4 were clearly visible, which proved that the magnetic Fe3O4 nanoparticles were successfully immobilized in MIL-101(Fe). Figure 2(h) showed that the synthesis was well done, with individual particles being uniform in size and regular in shape.
Figure 3(a)(b) showed the magnetic adsorption curves of Fe3O4@MIL-101(Fe) and Fe3O4@MIL-100(Fe) before and after adsorbing Sb(III). From the graph, it could be observed that the materials have been endowed with magnetism. Further indicating that the magnetic nanoparticles Fe3O4 have been successfully fixed into the structure of MIL-100(Fe) and MIL-101(Fe). By imparting magnetic properties to the composite material, with an external magnet, it may be effectively and simply removed from the test solution. Furthermore, the study found that the materials used in the adsorption experiment still retained their magnetism, albeit slightly decreased, proving their structural stability. Especially for Fe3O4@MIL-101(Fe), it maintained good magnetism before and after adsorption, making it easy to separate from water. In comparison, the magnetic properties of Fe3O4@MIL-100(Fe) were weaker, as it requires perfect occupation of Fe2+ and Fe3+ in the corresponding sites to exhibit good magnetism. It could be inferred that the effect of loading Fe3O4 on MIL-101(Fe) was superior to that on MIL-100(Fe).
3.3 Effect of pH on adsorption
Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) showed different adsorption effects on Sb(Ⅲ) as shown in Fig. 3(c) and (d). In the pH range of 1 to 2, Fe3O4@MIL-100(Fe) material had a greater capacity to adsorb Sb(Ⅲ), reaching the highest value of 58.9% at pH = 2. The adsorption rate at pH = 1 was slightly lower than at pH = 2. Because for Sb(Ⅲ), at around pH = 2, antimony existed mainly as Sb(OH)2+ and had a negative zeta potential, resulting in electrostatic attraction and increased adsorption capacity at pH = 2. Between pH = 3 and 10, the adsorption rate of Fe3O4@MIL-100(Fe) for Sb(Ⅲ) decreased. With an isoelectric point of approximately 7.1, the zeta potential of Fe3O4@MIL-101(Fe) decreased as the pH value went from 4 to 9. Under extremely acidic conditions, the electrostatic repulsion between positively charged Sb(OH)2+ and Sb(Ⅲ) made it difficult for Sb(Ⅲ) to be efficiently adsorbed. As the pH value increased, the proportion of Sb(OH)3 in water increased, weakening the electrostatic repulsion. Consequently, across the pH range of 3 to 10, the removal rate of Sb(Ⅲ) by Fe3O4@MIL-101(Fe) stayed nearly constant at roughly 72%. The results indicated that unless under strong acidic conditions, changes in pH did not significantly affect the adsorption of MOF materials (Liu et al., 2017). This was due to the fact that in the pH range of 2 to 11.8, Sb(Ⅲ) primarily occurs as neutral Sb(OH)3, so electrostatic attraction had almost no effect on the adsorption rate within this range (Wilson et al., 2010). In conclusion, compared to Fe3O4@MIL-101(Fe), Fe3O4@MIL-100(Fe) had a lower adsorption rate for Sb(Ⅲ) and a narrower optimal pH range. Chemical adsorption predominated the adsorption process at pH = 2, while there was also a physical electrostatic attraction. The adsorption mechanism was nearly totally reliant on chemical adsorption above pH = 2.
3.4 Kinetics of adsorption
Investigated was the impact of the adsorption period on the clearance rate of Sb(III) adsorbed by Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe). In this experiment, experimental data at various time points were fitted using pseudo-first-order model (2) and pseudo-second-order model (3). The relevant calculation formula is as follows (Rahmani et al., 2010):
$$\:{\text{Q}}_{\text{t}}={\text{Q}}_{\text{e}}(1-{\text{e}}^{{-\text{k}}_{1}\text{t}})$$
2
$$\:{\text{Q}}_{\text{t}}=\frac{{\text{k}}_{2}{\text{Q}}_{\text{e}}^{2}\text{t}}{1+{\text{k}}_{2}{\text{Q}}_{\text{e}}\text{t}}$$
3
Parameter k1(h− 1) is the first-order kinetic rate constant, and parameter k2(g mg− 1 h− 1)is the second-order kinetic rate constant. Qt(mg g− 1) is the adsorption amount at each time point, and Qe(mg g− 1) is the adsorption amount when the adsorption reaches equilibrium.
Fe3O4@MIL-100(Fe) reached adsorption equilibrium after approximately 12 hours. In comparison, the adsorption of Sb(III) by Fe3O4@MIL-101(Fe) was much faster, reaching maximum adsorption capacity in just 10 minutes. The kinetic constants shown in Table 3 indicate that both materials exhibit high correlation coefficients for the adsorption of Sb(III). The adsorption behavior was more accurately characterized by the pseudo-second-order model, which also fitted the adsorption capacity to the experimental data with good accuracy. Demonstrating once more that the primary mechanism involved in the adsorption process was chemical adsorption. It was preliminarily suggested that the main adsorption mechanism involves chemical adsorption, where Sb(III) formed Fe-O-Sb bonded with incompletely coordinated Fe ions within the metal clusters (Ho and Mckay, 2000).
Table 3
Kinetic fitting results for the adsorption of Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) on Sb(Ⅲ).
| | Parameter/unit | Sb(Ⅲ) |
Fe3O4@MIL-100(Fe) | Pseudo-first-order model | Qe/mg g− 1 | 29.8909 |
| | K1/h− 1 | 0.0155 |
| | R2 | 0.9085 |
| Pseudo-second-order model | Qe/mg g− 1 | 31.9603 |
| | K2/g mg− 1h− 1 | 7.29×10− 4 |
| | R2 | 0.9747 |
Fe3O4@MIL-101(Fe) | Pseudo-first-order model | Qe/mg g− 1 | 27.2251 |
| | K1/h− 1 | 3.4763 |
| | R2 | 0.9046 |
| Pseudo-second-order model | Qe/mg g− 1 | 28.0464 |
| | K2/g mg− 1h− 1 | 0.2376 |
| | R2 | 0.9847 |
3.5 Thermodynamic study
The relevant experimental data were substituted into Langmuir(Eq. (4)) and Freundlich(Eq. (5)) isotherm models for fitting. The fitting relevant formulas are as follows (Ozdemir et al., 2004):
$$\:\frac{{C}_{e}}{{q}_{e}}=\frac{1}{{\text{q}}_{\text{m}}{\text{K}}_{\text{L}}}+\frac{{\text{C}}_{\text{e}}}{{\text{q}}_{\text{m}}}$$
4
$$\:\text{l}\text{o}\text{g}{\text{q}}_{\text{e}}=\frac{1}{\text{n}}\text{l}\text{o}\text{g}{\text{C}}_{\text{e}}+\text{l}\text{o}\text{g}{\text{K}}_{\text{F}}$$
5
Qe (mg g− 1) is the equilibrium adsorption capacity of Sb; Qmax (mg g− 1) is the maximum adsorption capacity of the material for Sb(Ⅲ) under different concentration conditions; Ce (mg L− 1) is the equilibrium concentration; In the formula of Freundlich isotherm, n represents the adsorption strength and KF represents the adsorption capacity. In the equation of Langmuir isotherm, KL represents the adsorption correlation constant. These two groups of fitting curves represent the isotherm and data fitting results respectively, reflecting the adsorption law of adsorbent on Sb(III). In the designed experiment, the concentration of heavy metals in the solution was used as a variable and was gradually increased from 5 mg L− 1. The amount of adsorption grew progressively as the concentration rose. The maximum adsorption capacity of Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) for Sb(III) was achieved at concentrations of 50 mg L− 1 and 60 mg L− 1 respectively.
In order to gain a better understanding of the adsorption behavior of Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) on antimony, Freundlich and Langmuir isotherm models were used to match the experimental results. The fitting results for the adsorption of Sb(III) by Fe3O4@MIL-100(Fe) were shown in Fig. 4(c), the adsorption capacity data was well-fit by both the Freundlich and Langmuir isotherm models. The relevant fitted parameters showed the Freundlich model yielded a correlation coefficient (R2) of 0.9813, while the Langmuir isotherm model yielded an R2 of 0.9838. For the adsorption of Sb(III) by Fe3O4@MIL-101(Fe), the Freundlich and Langmuir isotherm models resulted in R2 values of 0.9961 and 0.9997, respectively. Both adsorption isotherm models showed good fitting, in contrast, the adsorption of Sb(III) by Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) was more consistent with the Langmuir isotherm model. It indicated that the adsorbent existed as monolayer adsorption on the adsorbent, showed obvious homogeneity in the adsorption sites, and was generally dominated by chemisorption.
According to the principles associated with the Langmuir model, the model reflects the number of adsorption sites on the surface of the material. Under these conditions, the excellent result of monolayer adsorption is to reach the maximum adsorption capacity. This occurs when the initial concentration of antimony solution is high enough to bind to all surface sites. It is clear that when the starting concentration range is large enough to occupy all surface sites, the Langmuir model performs better. The highest adsorption capacities for antimony(III) of Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) were 32.91 mg g− 1 and 28.56 mg g− 1, respectively, based on the results of the Langmuir isotherm model fitting.
Table 4
Isotherm fitting results for the adsorption of Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) on Sb(III).
| | Parameter/unit | Sb(Ⅲ) |
Fe3O4@MIL-100(Fe) | Freundlich | Qm/mg g− 1 | 33.1833 |
| | KF/mg g− 1 | 73.5485 |
| | R2 | 0.9813 |
| Langmuir | Qm/mg g− 1 | 32.9101 |
| | KL/L mg− 1 | 7.47×10− 4 |
| | R2 | 0.9838 |
Fe3O4@MIL-101(Fe) | Freundlich | Qm/mg g− 1 | 28.7673 |
| | KF/mg g− 1 | 35.0169 |
| | R2 | 0.9961 |
| Langmuir | Qm/mg g− 1 | 28.5552 |
| | KL/L mg− 1 | 0.0058 |
| | R2 | 0.9997 |
3.6 Ion coexistence experiment
In practical applications, some other substances in the adsorption system would interfere with the adsorption of the target adsorbate (including heavy metals, salts, etc.), competing for adsorption sites on the adsorbent and thus affecting the adsorption performance to some extent. Therefore, it is necessary to explore the selectivity of Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) for the target adsorption. Firstly, the impact of coexisting cations on the adsorption efficiency of Fe3O4@MIL-100(Fe) was investigated. The experimental design involved introducing the adsorbent into Sb(III) solution containing 0.01 M cations Na+, K+, Mg2+and Ca2+. The results showed that the impact on adsorption followed the order Mg2+ > Ca2+ > Na+ > K+. With Mg2+ having the greatest inhibitory effect on adsorption, leading to a decrease in Sb(III) adsorption rate of over 15%. The main reason for this was the different ionic radii and electronegativities of the cations. The ionic radius of Mg2+, K+, Na+, and Ca2+ are 0.072, 0.138, 0.102, and 0.1, respectively. When the ionic radius is smaller, it is conducive to free diffusion in the pores of MOFs and interaction with the adsorption sites. At the same time, the performance of Fe3O4@MIL-101(Fe) in removing Sb(III) in different coexisting ion water environments was also explored. By introducing the adsorbent into Sb(III) solution containing 0.01 M anions Cl−, F−, NO3−, SO42−, and cations Na+, Mg+, Ca2+, and K+. The adsorption efficiency fell by 17.60%, 44.68%, 13.69%, and 24.92%, respectively, as shown in Fig. S3, after the addition of Cl−, PO43−, NO3− and SO42−ions. It could be concluded that Cl−, NO3− and SO42− had competitive adsorption with Sb(Ⅲ) but had little influence, while PO43− had a great influence. Antimony and phosphorus were thought to form a similar inner sphere complex because of their similar electron orbitals, shared main group membership, and chemically similar structures. As a result, the competition for adsorption sites would be what was causing the decrease in Sb(III) removal efficiency (Wang et al., 2021). However, there was almost no competition for Sb(Ⅲ) adsorption by cations Na+、Mg+、Ca2+、K+, and the adsorption efficiency of Sb(Ⅲ) decreased by less than 10%.
3.7 Adsorption regeneration studies
The ability to be reused is an important factor in assessing the use of adsorbents. In order to evaluate the reusability of Fe3O4@MIL-100(Fe) as an adsorbent, the used adsorbent material was separated using a magnet. Then soaked in a 30 ml 0.01 M HCl solution for 6 hours, and reused in a 50 mg L− 1 antimony solution 2 more times. As shown in Fig. S4, the adsorption of Sb(Ⅲ) by the adsorbent basically did not change after 3 uses, with the removal efficiency only decreasing by about 14%. After separating the Fe3O4@MIL-101(Fe) material, it was soaked in a 30 ml 0.1 M sodium hydroxide solution for 6 hours. Then reused in a 60 mg L− 1 antimony solution 2 more times, the result was shown in Fig. S5. After 3 complete adsorption-desorption tests, the adsorption capacity basically did not change, with the removal efficiency only decreasing by about 8%. The results indicated that Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe) not only had recyclability as adsorbents but also had a high potential for repeated use. In addition, the reusability stability of Fe3O4@MIL-101(Fe) was slightly higher than that of Fe3O4@MIL-100(Fe).
3.8 Study on adsorption mechanism
First of all, according to the infrared spectrum in Fig. 5(a), it could be observed that there were slight changes in the position and intensity of the characteristic peaks before and after adsorption. The absorption peak at 1382 cm− 1 decreased in intensity and shifted slightly, corresponding to the changes in the carboxylic functional groups of Fe3O4@MIL-100(Fe) after adsorbing Sb. Indicating that the adsorption process was related to the unsaturated sites on the material surface. The weaker absorption peak at 748 cm− 1 for Fe3O4@MIL-100(Fe) slightly increased, attributed to the out-of-plane deformation vibration of -OH in Fe-OH. After the adsorption of antimony, the absorption band at 545 cm− 1 underwent a slight shift, indicating the possible formation of Fe-O-Sb bonds between Fe3O4@MIL-100(Fe) and Sb(III) molecules. The FTIR changes before and after the adsorption of Sb(III) by Fe3O4@MIL-101(Fe) were shown in Fig. 5(e). The peak at 552 cm− 1 before adsorption was due to the coordination bond formed by carboxyl groups and Fe. After adsorption, the peak shifted to 540 cm− 1, possibly due to the formation of Fe-O-Sb complexes, which was the main adsorption mechanism (Li et al., 2019). The peak at 752 cm− 1 corresponded to the vibration of the C-H bond in the benzene ring. After adsorption, its intensity decreased, indicating a decrease in the content of benzene ring C-H groups in the reaction process. Thereby causing BDC2− to become free, suggesting that part of the crystal shape has been disrupted. The strong peak (Li et al., 2017) at 1300 cm− 1 was caused by the stretching vibration of the carboxyl group on the ligand H2BDC (Xie et al., 2017).
The coordination effect is an important mechanism for antimony adsorption in Fe-based MOF materials. Taking MIL-101(Fe) as an example, in the structure of MIL-101(Fe) with the chemical formula Fe3OCl(H2O)2(BDC)3. It could be inferred that each node contains three BDC2− and the remaining three coordination sites were connected to Cl− and H2O (Taylor-Pashow et al., 2009). When MIL-101(Fe) was immersed in an aqueous solution, Fe-OH was formed, due to the coordination of unsaturated sites (CUS) containing Lewis acid in its three metal clusters (Hong et al., 2009). Sb(Ⅲ) would exchange with the hydroxyl groups in the metal clusters, thus forming Fe-O-Sb coordination to remove Sb(Ⅲ) from the water. To gain a deeper understanding of the adsorption mechanism of Fe3O4@MIL-100(Fe)/MIL-101(Fe) for Sb(Ⅲ), XPS characterization of the materials before and after adsorption was carried out.
First, the changes in the elemental composition of Fe3O4@MIL-100(Fe) before and after adsorption were analyzed. The results were shown in Fig. 5(b). XPS full spectrum analysis showed that the material not only contains Fe, C, and O elements but also F elements, which was due to the addition of hydrofluoric acid during the synthesis process. The increased Sb element in the spectrum after adsorption proved the effective binding of Sb to the material. Additionally, in the XPS spectrum of Fe 2p, as shown in Fig. 5(c), the peak positions of Fe elements were at 729.9 eV, 726.5 eV, 716.5 eV and 712.7 eV corresponding to the characteristic peaks of Fe 2p3/2 and Fe 2p1/2 (Li et al., 2020). After the reaction, the characteristic peaks shifted to the right to 727.8 eV, 724.9 eV, 715.7 eV and 711.6 eV, respectively. The shift in binding energy positions demonstrated a chemical reaction, indicating the formation of Fe-Sb coordination bonds at unsaturated sites of the material. In the O 1s XPS spectrum, a characteristic peak appeared at 530.9 eV, which corresponded to Fe-O-C. After adsorbing Sb(III), an additional peak appeared at 540.2 eV in the Fe3O4@MIL-100(Fe) material, corresponding to Sb(III) 3d3/2, while the Fe-O-C peak significantly weakened with a slight shift to 531.9 eV. The peak corresponding to the Sb 3d5/2 position is at 533.3 eV. Therefore, it can be inferred that Sb(III) effectively adsorbs on Fe3O4@MIL-100(Fe). In conclusion, the unsaturated Lewis acid sites of the metal, forming Fe-O-Sb bonds, and electrostatic forces collectively contributed to the adsorption process of Sb(III) on Fe3O4@MIL-100(Fe).
Observing the XPS results of Fe3O4@MIL-101(Fe), it could be clearly seen that the three peaks corresponding to O 1s, C 1s, and Fe 2p were at binding energies of 530.70 eV, 283.33 eV, and 709.55 eV, respectively. After adsorption, an Sb 3d peak appeared, with binding energies at 538.06 eV and 530.25 eV, corresponding to Sb 3d3/2 and Sb 3d5/2, respectively. It could be also proven that Fe3O4@MIL-101(Fe) successfully adsorbed Sb(III). As shown in Fig. 5(g), in the Fe 2p spectrum, two peaks were convoluted with binding energies of 723.36 eV and 710.01 eV, corresponding to Fe 2p1/2 and Fe 2p3/2, respectively. After adsorption, they shifted to binding energies of 722.52 eV and 709.55 eV, respectively, due to the formation of Fe-Sb coordination. In addition, a small amount of unreacted Fe3+ was attached to the surface of the Fe3O4@MIL-101(Fe) material during the synthesis process, which was released from the pores of Fe3O4@MIL-101(Fe). When it encountered water and reacted to form hydrated iron oxide (HFO), corresponding to two peaks at binding energies of 725.66 eV and 712.20 eV. The formation of HFO generated more active sites and improved the adsorption efficiency of the material for Sb(III). It could be inferred that the Fe-O-Sb coordination formed by the incomplete coordination of Fe ions in the Fe3O4@MIL-101(Fe) metal cluster with Sb(III) and the in-situ formation of HFO were the main adsorption mechanisms. As shown in Fig. 5(h), the O 1s spectrum was deconvoluted into three peaks before adsorption, corresponding to the metal bond Fe-O, the C-O bond in the carboxyl group of terephthalic acid, and the hydroxyl group-OH at binding energies of 530.86 eV, 532.91 eV, and 533.85 eV, respectively. After adsorption, a new Sb-O bond appeared at a binding energy of 532.62 eV, further proving the successful adsorption of Sb(III). The peak area of OH decreased by 18.8% after adsorption, indicating that the terminal -OH of Fe3O4@MIL-101(Fe) was the key functional group for removing Sb(III). In addition, the peak area of C-O decreased after adsorption, which was related to the C-O connected to terephthalic acid. It corresponded to the FTIR spectrum analysis results, where some BDC2− turned into a free state. It could be concluded from the O1s spectrum analysis that the Fe-O-Sb formed by the hydroxyl group was the key to adsorption. Therefore, it was known that the main mechanism for Fe3O4@MIL-101(Fe) to remove Sb(III) is based on coordination and the active sites provided by the in-situ formation of HFO.
Based on the above analysis, it could be concluded that the main mechanism of the two magnetic iron-based MOFs, namely Fe3O4@MIL-100(Fe) and Fe3O4@MIL-101(Fe). The adsorption of Sb(III) was due to the coordination of Fe-O-Sb formed by the incomplete coordination of Fe ions in the metal clusters with Sb(III), as shown in Fig. 6.