3.4 Characterization
The micromorphology of EC-MMIPs and EC-NMIPs was characterized by SEM as can be seen in Fig. 6. As shown in the figure, the microspheres of A and B appear to agglomerate after being wrapped by a layer of imprinted polymer, because the process of polymerization and cross-linker reduces the dispersion of particles. Remarkably, the surface of EC-MMIPs was rougher than that of EC-NMIPs. This was due to imprinting voids after removal of template molecules in EC-MMIPs. The blotting cavity formed on the surface of the blotting layer increases the adsorption area and the number of binding sites, thus improving the adsorption capacity of EC-MMIPs31.
The spectra of FI-IR were shown in Fig. 7A. In all samples, the peak at 580 cm− 1 belonged to the Fe-O stretching vibration of Fe3O4 nanoparticles. The curve of Fe3O4@SiO2, the new characteristic peaks at 803 cm− 1, 480 cm− 1 and 1090 cm− 1 were attributed to the stretching vibration of S-i-O and Si-O-Si, respectively. The peaks at about 1565 cm− 1 and 1460 cm− 1 in Fe3O4@SiO2-CH = CH2 were assigned to the C = C-H group in the modified after MPS. Finally, the peaks at 2950 cm− 1, 1150 cm− 1 and 1730 cm− 1 in the spectra of EC-MMIPs were due to stretching vibrations of C-H, C-O and C = O in EGDMA, respectively, while the peak at 1730 cm− 1 was also the characteristic peak of C = O in MAA. The absorption peaks indicated that all reactions were successfully synthesized during the preparation of EC-MMIPs.
The crystal structures of all materials were determined by X-ray diffraction patterns, and spectra were presented in Fig. 7B. Six characteristic peaks: (220), (311), (400), (422), (511) and (440) were observed for all the samples 32, which indicates that the surface modification did not alter the crystalline structure of Fe3O4 nanoparticle.
Figure 8A indicated magnetic properties of Fe3O4, Fe3O4@SiO2-CH = CH2 and EC-MMIPs, the saturation magnetization were 67.6 emu/g, 47.4 emu/g and 37.6 emu/g, respectively. Compared with Fe3O4, the saturation magnetization of Fe3O4@SiO2-CH = CH2 and EC-MMIPs gradually decreases, which is due to the surface modification and functionalization of Fe3O4, which form a polymer coating and imprinted layer of a certain thickness on the surface of Fe3O4. However, it doesn’t affect the separation of EC-MMIPs by the magnetic field in short time.
The thermal stability of prepared nanoparticles was shown in Fig. 8B. As the result, both samples lost approximately 2.8% of their mass at 260 ℃, which was mainly due to desorption of the organic solvent and the evaporation of water in the polymer structure 33. When the temperature was continuously increased to 800 ℃, the mass loss of Fe3O4@SiO2-CH = CH2 was about 8.82%, which was caused by the thermal loss of silanol group and MPS on the surface. Compared with Fe3O4@SiO2-CH = CH2, the mass loss of EC-MMIPs was 26.2%, which was mainly due to the thermal decomposition of the imprinted layer34, indicated that the good thermal stability of EC-MMIPs within 260 ℃.
3.5 Adsorption performance study
The isothermal adsorption curves of EC-MMIPs and EC-NMIPs are shown in Fig. 9A. With the increase in concentrations, the binding amount gradually increased and reached a dynamic equilibrium. When the EC concentration exceed 80 µg/mL, the adsorption capacity of EC-MMIPs and EC-NMIPs tends to be saturated. The adsorption capacity of EC-MMIPs was significantly higher than that of EC-NMIPs, about 2.2 times that of EC-NMIPs. It can be attributed to the fact that the surface of EC-MMIPs has more imprinted cavities than the EC-NMIPs surface.
The adsorption isotherm describes how molecules are adsorbed to the surface of an adsorbent. Therefore, Langmuir and Freundlich models (Eqs. (3) and (4), respectively) were used to fit the adsorption isotherm data.
Langmuir model: \(\frac{{C}_{e}}{{Q}_{e}}=\frac{{C}_{e}}{{Q}_{m}}+\frac{1}{{bQ}_{m}}\) (3)
Freundlich model: \(\text{log}{Q}_{e}=\text{log}k+\frac{1}{n}\text{log}{C}_{e}\) (4)
In the equation, Qm (µg/mg) is the theoretical maximum adsorption capacity, Ce (µg/mL) is the equilibrium concentration of EC, and Qe (µg/mg) represent the adsorption capacity at adsorption equilibrium, b is the equilibrium constant (mL/µg) of the Langmuir model, k is the Freundlich model equilibrium constant and n is a constant. The relevant parameters and R2 of the two models were calculated, the results are shown in Table 1. The Langmuir model (R2EC − MMIPs = 0.9929, R2EC − NMIPs = 0.9967) was better fitted than that Freundlich model (R2EC − MMIPs = 0.95637, R2EC − NMIPs = 0.9848), Fig. 9B showed the Langmuir regression curve, which indicated that EC-MMIPs was monolayer adsorbed with homogeneous structure 35.
Table 1
Adsorption isotherm constants of Langmuir model and the Freundlich model.
| Langmuir | Freundlich | |
Qm | b | R2 | k | n | R2 |
EC-MMIPs | 27.73 | 0.041 | 0.9929 | 2.3302 | 1.9612 | 0.9563 | |
EC-NMIPs | 11.31 | 0.040 | 0.9967 | 1.5813 | 2.5521 | 0.9846 | |
Table 2
Adsorption rate constants of pseudo-first-order rate kinetic model and pseudo-second-order kinetic model.
| Pseudo-first-order | Pseudo-second-order | |
Qe | k1 | R2 | Qe | k2 | R2 |
EC-MMIPs | 15.13 | 0.1414 | 0.9752 | 19.76 | 0.0026 | 0.9984 | |
EC-NMIPs | 11.73 | 0.2002 | 0.9402 | 9.26 | 0.0117 | 0.9987 | |
The adsorption dynamic curves of EC-MMIPs and EC-NMIPs on EC are shown in Fig. 9C. The adsorption capacity increased with the increase over time, reaching saturated in 30 ~ 40 min. The maximum adsorption capacities of EC-MMIPs (Qe=18.53 µg/mg) and EC-NMIPs (Qe=8.77 µg/mg) were reached at 40 and 30 min, respectively. At the beginning of the adsorptive process, there were a large number of unoccupied imprinted cavities on the surface of EC-MMIPs, and the carboxyl groups on MAA form hydrogen bonds with EC, so that EC is quickly adsorbed to the surface of EC-MMIPs, until all the cavities are occupied and the adsorption equilibrium was reached. The results showed that the adsorption performance of EC-MMIPs was better than that of EC-NMIPs, which was related to the specific matching between the imprinted cavity on the surface of EC-MMIPs and EC.
In order to study the adsorption mechanism, the Pseudo-first-order adsorption kinetic model and the Pseudo-second-order adsorption kinetic model were used to fit the experimental data. Equations (5) and (6).
Pseudo-first-order : \(\text{ln}\left({Q}_{e}-{Q}_{t}\right)=ln{Q}_{e}-{k}_{1}t\) (5)
Pseudo-second-order : \(\frac{t}{{Q}_{t}}=\frac{1}{{k}_{2}{Q}_{e}}+\frac{t}{{Q}_{e}}\) (6)
where Qe and Qt meant the amounts of EC on the sorbent at equilibrium and t was the adsorption time (min), respectively. k1 was the Pseudo-first-order rate constant and k2 belongs to the Pseudo-second-order rate constant. The relevant parameters and R2 of the two models were calculated, and the results are shown in Table 2. The Pseud-o-second-order kinetics model (R2EC − MMIPs = 0.99846 R2EC − NMIPs = 0.9987 was better fitted than that the Pseudo-first-order kinetics (R2EC − MMIPs = 0.97521, R2EC − NMIPs = 0.94023). Figure 9D shows the Pseudo-second-order kinetics regression curve, this indicated that the whole adsorption process is mainly chemisorption. Which meant that in the EC-MMIPs cavity, ethyl carbamate could form hydrogen bonds with methacrylic acid to achieve chemical adsorption.
In order to evaluate the selectivity of EC-MMIPs for the adsorption of ethyl carbamate, methyl carbamate and butyl carbamate were chosen as competitive substrates. Meanwhile, the selectivity of EC-MMIPs and EC-NMIPs to ethyl carbamate was further evaluated by imprinting factor (α) and selectivity factor (β) determination28, which were calculated according to Eqs. (7) and (8), respectively.
$$\alpha ={Q}_{MMIP}/{Q}_{NMIP}$$
7
$$\beta ={\alpha }_{EC}/{\alpha }_{other}$$
8
Among them, QMMIP and QNMIP (µg/mg) were adsorption capacities of EC-MMIPs and EC-NMIPs, respectively. αEC and αother were the imprinting factors for template and analogs.
The results are shown in the table. α value reflects the difference of EC-MMIPs and EC-NMIPs on EC adsorption, β value reflects the selective adsorption capacity of adsorbent on EC in complex mechanism. The results showed that EC-MMIPs still had good adsorption effect on ethyl carbamate in the presence of competitive substrates, and its adsorption capacity was significantly greater than that of structural analogues.
Table 3
The selectivity parameters of EC-MMIPs and EC-NMIPs
analyte | QEC−MMIPs | QEC−MMIPs | α | β |
EC | 17.55 | 7.62 | 2.30 | \ |
MC | 7.64 | 7.2 | 1.06 | 2.16 |
BC | 3.6 | 3.3 | 1.09 | 2.11 |
The experimental results were based on the initial adsorption capacity of EC-MMIPs on EC (100%). The adsorption rates of four cycles of elution and adsorption experiments were shown in Fig. 10, and the adsorption rates were 98.4%, 97.5%, 98.1% and 92.6% successively. The results showed that the adsorption rate of EC-MMIPs decreased after five cycles of adsorption, and there was adsorption rate of 92.6% at the fifth adsorption. This was because the spatial structure of EC-MMIPs was relatively stable, the binding site was relatively firm, and the structure of the imprinted cavity could remain stable under acid or high temperature.