Jianming Pan*a,
Wenjing Zhua,
Xiaohui Daia,
Xuesheng Yanb,
Mengyin Ganc,
Linzi Lic,
Hui Hangc and
Yongsheng Yanc
aSchool of Chemistry and Chemical Engineering, Jiangsu University, Zhenjiang 212013, China. E-mail: zhenjiangpjm@126.com (Jianming Pan)
bSchool of Energy and Power Engineering, Jiangsu University, Zhenjiang 212013, China
cSchool of the Environment, Jiangsu University, Zhenjiang 212013, China
First published on 28th October 2013
Magnetic molecularly imprinted microcapsules (MMIMs) were synthesized by Pickering emulsion polymerization. In this work, an oil-in-water Pickering emulsion stabilized by halloysite nanotubes (HNTs) was first established in the presence of a few hydrophilic Fe3O4 nanoparticles as magnetic separation carriers. The imprinting system was fabricated by radical polymerization and subsequent combination with functional and polymeric monomers in the oil phase. The formation mechanism of the Pickering emulsion and MMIMs is discussed in detail, and the as-prepared MMIMs are successfully evaluated as sorbents for the recognition of λ-cyhalothrin. The results demonstrated that the MMIMs exhibited magnetic sensitivity (Ms = 8.45 emu g−1), a hollow structure, a semipermeable external surface and excellent robustness. The batch mode experiments proved that the imprinting effect synchronously improved the adsorption kinetics and equilibrium for the MMIMs. The selective recognition experiments also suggested high affinity and selectivity of MMIMs towards λ-cyhalothrin over fenvalerate and diethyl phthalate.
Molecular imprinting is a facile and versatile technique used for preparing polymers with specific binding sites, namely molecularly imprinted polymers (MIPs). In order to fabricate tailor-made binding sites, molecular interactions between the template molecule and the functional monomer in a self-assembly step are first obtained. Then the self-organised architecture formed is fixed by additional crosslinking polymerization. Subsequently, the removal of the template molecule from the polymer matrix leaves behind binding sites possessing functional groups complementary to the template molecules.16 Inspired by the benefits of molecular imprinting and Pickering emulsion, Ye's group reported several novel and important studies about the imprinted polymer beads derived from Pickering emulsion polymerization.17–19 For example, using water-in-oil Pickering emulsion polymerization, the molecular imprinting of proteins was carried out to prepare spherical hydrogels with pre-designed selectivity for proteins.17 Furthermore, a new interfacial nano and molecular imprinting method based on Pickering emulsion polymerization was also developed.19 These studies adopted spherical SiO2 particles to irreversibly adsorb at the oil and water interface, as opposed to particles of non-spherical shapes. The irreversible adsorption at oil and water interface is commonly caused by capillary energy that is several orders of magnitude higher than the thermal energy.20 However, Lehle etc. demonstrated that for non-spherical colloids at free interfaces capillary interactions appear to be dominant.21 There is, therefore, a clear interest in the synthesis of MIPs by Pickering emulsion polymerization stabilized solely by non-spherical particles. In order to meet the need for a stable emulsion, the spherical SiO2 particles needed to be modified to adjust their surface wettability, which was time consuming and complicated.
In recent years, disk-shaped Laponite clay has been reported to stabilize water-in-oil emulsions or oil-in-water emulsions. For example, Cauvin et al. successfully prepared polymer latex particles via Pickering emulsion polymerization using Laponite RD clay.22 Recently, Isabelle Capron's group fabricated several oil-in-water Pickering emulsions stabilized solely by cellulosic colloidal nanorods of different origins.23 In previous studies, our group adopted attapulgite (ATP) with fiber bundle morphology as the stabilized particles to obtain magnetic/hollow double-shelled imprinted sorbents.24 The ATP particles used in our work had diameters of 300 nm and lengths of 1.0–3.0 μm. Compared with cellulose, Laponite RD and ATP, halloysite nanotubes (HNTs), a naturally occurring clay mineral with large reserves in China, have smaller sizes, open-ended tubular structures and superior surface areas, which make them attractive for the preparation of a more stable Pickering emulsion.25 Moreover, HNTs with a chemical formula of Al2Si2O5(OH)4·nH2O also possess hydrophilic surfaces.26 Thus, HNTs appear to be excellent candidates to produce a stable oil-in-water emulsion in addition to their size and shape versatility. However, the work required to take advantage of HNTs to build a stable emulsion without modification has never been investigated to the best of our knowledge.
To get a rapid separation of chemical species, magnetic nanoparticles such as Fe3O4 have recently attracted considerable attention in Pickering emulsion polymerization. The synthesis of magnetic hollow silica was reported through a Pickering emulsion solely stabilized by cetyltrimethylammonium bromide modified Fe3O4 particles.27 Liu et al. prepared superparamagnetic polyaniline hybrid hollow microspheres with sodium citrate modified Fe3O4 nanoparticles as a template.28 Pickering emulsion polymerization based on Fe3O4 particles can be used for the fabrication of magnetic composites, which can be easily collected and separated by an external magnetic field without additional centrifugation or filtration. However, many pure Fe3O4 particles adsorbed at the oil and water interface may have problems associated with the formation of large aggregates and easy leakage.
Inspired by the studies mentioned above, the molecular imprinting and magnetic separation concepts were introduced into a Pickering emulsion polymerization, and than the magnetic molecularly imprinted microcapsules (MMIMs) were synthesized. In this work, we chose 4-vinylpyridine (4-VP) as the functional monomer to recognize the target pollutant molecule λ-cyhalothrin, HNTs as a stabilizer for the oil-in-water Pickering emulsion and a few hydrophilic Fe3O4 nanoparticles as magnetic separation carriers, which provided imprinted and magnetic microcapsules. The whole process of the synthesis of MMIMs and the recognition of λ-cyhalothrin is presented in Fig. 1. The characterization, adsorption equilibrium, kinetics, and selectivity recognition of the MMIMs were investigated in detail.
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| Fig. 2 Photos of the water phase dispersion (a), and Pickering emulsion before (b) and after (c) ultrasonication. | ||
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5, v/v), the imprinted template molecules were removed. Finally, binding sites with stereochemistry complementary to λ-cyhalothrin were formed in the MMIMs. The optical micrographs of Pickering emulsion (a) and the MMIMs before (b) and after (c) elution are shown in Fig. 3. Fig. 3a shows a typical stable Pickering emulsion that was used to produce the MMIMs. The emulsion droplets were tiled on the glass slide and exhibited a spherical hollow structure without collapse. Moreover, the Pickering emulsion prepared in this work had relatively broad droplet size distributions, and a mean droplet diameter of approximately 80 μm estimated from the optical micrograph. After heating at 65 °C to initiate polymerization, the surface of the spherical MMIMs before elution was rough, which suggested that the HNT particles adsorbed at the oil–water interface were subsequently locked into the external surface of the capsule (Fig. 3b). As a result of this, the HNT building blocks were firmly attached onto the surface of polymer network which enhanced the mechanical properties of the MMIMs.31 It can be clearly seen from Fig. 3c that hollow structures existed in the MMIMs after elution, and the capsule shells were asymmetric and nonuniform with a thickness range of 7.0–20 μm.
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| Fig. 3 Optical micrographs of Pickering emulsion (a), and MMIMs before (b) and after (c) elution with water and ethanol. | ||
C stretching vibrations from the aromatic ring, were due to 4-VP.33 The appearance of absorption bands at 3064 cm−1 and 3020 cm−1, assigned to H–C
C, also gave direct evidence for the action of 4-VP. Furthermore, other absorption bands due to the aromatic stretching vibrations of the styrene units were also observed around 1491 cm−1, 2920 cm−1 and 2846 cm−1.
SEM images of the MMIMs (a), a single broken MMIM (b), and the external (c) and internal (d) surfaces of the MMIMs are shown in Fig. 5. The SEM image of the MMIMs prepared with Pickering emulsion polymerization revealed the formation of an intact spherical structure with a size distribution of 80 ± 10 μm (Fig. 5a). The microspheres were coarse and symmetrical without dimples under the conditions of the SEM analysis, suggesting excellent mechanical stability. The hollow nature of the capsules was visualized using an SEM image of a single broken MMIM in Fig. 5b. As shown in Fig. 5c, the external surface consisted of randomly distributed HNTs which were deposited on the exterior surface of the imprinted polymer shell rather than being embedded within it, indicating that the surface of the HNTs was sufficiently wettable by the dispersed oil phase without further modification. But only a few HNT particles were embedded into the imprinted polymer shell. This observation suggests that the surface wettability of HNTs was different from most modified inorganic colloids, and the incorporation of HNTs into the composite MMIMs was dependent on the addition of NaCl to the aqueous phase as previously described for Laponite clays.24 In Fig. 5d, many crosslinked polymer units arising from the nature of the interfacial phase separation were observed on the internal surface of the MMIMs. Both the external and internal surfaces of the MMIMs possessed denser but semipermeable structures, and surely played an important role in molecular capture by the obtained MMIMs. The EDX spectra of area 1 (d) and area 2 (e) were also measured and are shown in Fig. 5. Peaks for the Fe, O, C, Al, Si and Au elements were observed together for the exterior surface of the MMIMs as shown in Fig. 5e. The Au peak was due to the electrically-conducting material which was deposited by low vacuum sputter coating of the sample, and the Al and Si peaks resulted from the stabilized HNT particles. The low percentage of Fe in the pattern in Fig. 5e indicated the presence of magnetic carrier Fe3O4 on the exterior surface of the MMIMs. Besides Fe, Al, Si and Au peaks, a higher percentage of C and O confirmed the successful synthesis of the imprinted polymer. In Fig. 5f, only the peaks for the C and O elements were observed in the EDX spectrum of area 2. This phenomena is consistent with the results from the SEM image of the internal surface of the MMIMs, in which there were only a few HNTs existing in the polymer layer of the internal surface.
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| Fig. 5 SEM images of MMIMs (a), a single broken MMIM (b), and the external (c) and internal (d) surfaces of the MMIMs, and EDX spectra of area 1 (e) and area 2 (f). | ||
The MMIMs and MNIMs (magnetic non-molecularly imprinted microcapsules) were further characterized by TGA and DTG, and the corresponding curves are shown in Fig. 6. As shown in Fig. 6, the MMIMs and MNIMs cannot be easily decomposed within the initial temperature range (<300 °C), and TGA curves also indicated that both of them decomposed in a single step at temperature >350 °C. Moreover, the HNT content was about 10 wt% for the MMIMs and MNIMs, which was determined by the remaining mass of thermal resistance after full decomposition. The TGA analysis also revealed that the prepared MMIMs included both inorganic and organic composites. The MMIMs and MNIMs had the same decomposition profile and weight loss, and this result confirmed that the MMIMs and MNIMs had similar morphological structures and size distributions.34 Furthermore, two exothermic peaks around 407.5 °C and 400.0 °C for the MMIMs and MNIMs are shown in the DTG curves with obvious weight losses in the TGA curves, which were assigned to the significant decomposition of bulk polymers. However, two wide exothermic peaks around 623.3 °C and 648.5 °C for the MMIMs and MNIMs, respectively, were also observed without corresponding changes in the TGA curves, indicating the phase transition of the magnetic carriers.35
Magnetic properties play an important role for the application of MMIMs in fast extraction and convenient separation. The magnetic hysteresis loops analysis of the MMIMs and as-prepared hydrophobic Fe3O4 particles in this work are shown in Fig. 7a. The hysteresis loops show that there was no magnetic hysteresis, which indicated that both MMIMs and as-prepared hydrophobic Fe3O4 revealed superparamagnetic behavior. The Fe3O4 particles had a saturation magnetization of 54.13 emu g−1, and the MMIMs exhibited a value of 8.45 emu g−1. The significant decrease of the magnetization value can possibly be attributed to the presence of additional imprinted polymer layers and the introduction of a few Fe3O4 particles into the MMIMs. A photograph of the MMIMs suspended in water in the absence and presence of an externally placed magnet is shown in Fig. 7b. The homogeneously dispersed MMIMs could adhere to the inner sides of the wall of the vial when the external magnetic field was applied, and the test solution was clear and transparent. The results strongly suggest that the magnetic MMIMs could be attracted by an external magnetic field effectively, and that the yellow MMIMs are feasible magnetic separation carriers. Moreover, magnetite leakage was crucial to the performance of the sorbent in different pH environments. Thus, the number of Fe(III) ions that were likely to leach from the MMIMs was determined using a graphite furnace atomic absorption spectrophotometer (Fig. 7c). At pH = 8.0, 0.12 μg of leached Fe(III) ions were detected from 50 mg of the MMIMs. Moreover, the weight of the leached Fe(III) ions slightly increased from a pH value 7.0 to 3.0, and then obviously increased at a lower pH of 2.0. At pH = 2.0, the maximum weight of leached Fe(III) ions was only 2.32 μg, suggesting that the MMIMs prevented magnetite leakage successfully. In recent years, silica, carbon and polymers have been used to coat magnetic nanoparticles, and then the preparation of magnetic molecularly imprinted polymer based magnetic composites could overcome the problem of magnetite leakage.36,37 But the step for synthesizing the magnetic composites prior to the imprinting polymerization were time-consuming and complicated. Thus, Pickering emulsion polymerization combined with a few Fe3O4 particles as magnetic carriers may be considered to be a simple and effective way to overcome the limitation of magnetite leakage.
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50 v/v) solution, and the functional adsorption behaviour of the MMIMs was investigated in detail. First, the adsorption capacity at different initial concentrations was analyzed, and the adsorption isotherms of the MMIMs and MNIMs were plotted (Fig. 8a). From Fig. 8a, when the equilibrium concentration increased, the equilibrium adsorption capacity (Qe) for λ-cyhalothrin first increased sharply, then increased slightly, and finally reached a maximum, as expected. It could also be seen that the adsorption capacities for λ-cyhalothrin were in the order MMIMs > MNIMs, and this was probably because the MMIMs demonstrated good specificity for the imprinted molecule. In order to obtain the maximum binding capacity of the MMIMs and MNIMs, Scatchard analysis was carried out.38 The Scatchard equation is expressed as following:
![]() | (1) |
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| Fig. 8 Equilibrium data (a), modeling (b) and ΔQ values (c) for the adsorption of λ-cyhalothrin onto MMIMs and MNIMs. | ||
Modeling of the adsorption of λ-cyhalothrin onto MMIMs and MNIMs by the Scatchard equation is shown in Fig. 8b. As shown, good fitting by the Scatchard equation is observed because the R2 values are 0.9832 and 0.9659 for the MMIMs and MNIMs, respectively. Moreover, the calculated maximum binding capacities of the MMIMs and MNIMs were 39.27 μmol g−1 and 25.74 μmol g−1, respectively. Al-Qodah's group studied the adsorption characteristics of λ-cyhalothrin in aqueous solutions using oil shale ash (OSA) as a sorbent.39 In their work, the maximum binding capacity was 13.0 μmol g−1, which was just one third of that in our work. This result indicates the advantage of our hollow microspheres.
To investigate the imprinting effect, the values of ΔQ were calculated using eqn (2), and the relationship between ΔQ and the initial concentration is shown in Fig. 8c.
| ΔQ = Qe,m − Qe,n | (2) |
In Fig. 8c, ΔQ significantly increased over the concentration range of 0–80 mg L−1, indicating that the empty imprinted sites were gradually occupied by λ-cyhalothrin upon increasing the testing concentration. Then ΔQ was approximately constant over the concentration range of 100–250 mg L−1, and then slightly increased in the concentration range of 300–350 mg L−1. This result implied that the specific binding sites reached saturation when the initial concentration of λ-cyhalothrin was 250 mg L−1, and then non-homogeneous binding sites with low affinity sites may be mainly responsible for the adsorption mechanism when the testing concentration exceeded 250 mg L−1.
As a means to study the effect of the contact time, the adsorption kinetics data and modeling by the pseudo-second-order equation are shown in Fig. 9a and Fig. 9b, respectively, and the half equilibrium times (tA and tB) are also marked in Fig. 9a. The pseudo-second-order equation is shown in eqn (3):40
![]() | (3) |
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| Fig. 9 Adsorption kinetic data (a) and modeling (b) for the adsorption of λ-cyhalothrin onto MMIMs and MNIMs. | ||
The values of the half equilibrium times, tA and tB, were 119.4 min and 108.1 min, and the related QA and QB were 21.62 μmol g−1 and 13.57 μmol g−1, respectively. The results showed that the MMIMs needed more time to reach the adsorption equilibrium than the MNIMs, while their adsorption rate was higher than that of MNIMs, especially in the first half of the adsorption time. This phenomenon further proved that the imprinting effect synchronously improved the properties of the adsorption kinetics and the equilibrium. R2 for the pseudo-second-order kinetic model was 0.9995 and 0.9968 for the MMIMs and MNIMs, respectively, indicating that a chemical process could be the rate-limiting step in the adsorption process.41
The specificity of the binding sites was investigated by studying the selectivity of the MMIM particles. Fenvalerate and diethyl phthalate had structures similar to λ-cyhalothrin and therefore were selected as template analogs (Fig. 10a). The uptake of λ-cyhalothrin, fenvalerate and diethyl phthalate by MMIMs and MNIMs is depicted in Fig. 10b. The differences in the re-binding capacities for the MMIMs or MNIMs can reflect the specific adsorption amounts of λ-cyhalothrin, fenvalerate and diethyl phthalate at the λ-cyhalothrin imprinted sites. ΔQ was also obtained using eqn (2). As evident in Fig. 9, the adsorption capacity of the MMIMs for λ-cyhalothrin was higher than those for fenvalerate and diethyl phthalate, while the adsorption capacities of the MNIMs were low and almost equal for the template and template analog molecules. By calculation, the values of ΔQ were 8.752 μmol g−1, 2.905 μmol g−1 and 2.115 μmol g−1 for λ-cyhalothrin, fenvalerate and diethyl phthalate, respectively. The results suggested that MMIMs were specific to λ-cyhalothrin but non-specific to fenvalerate and diethyl phthalate. Moreover, the external surface of the MMIMs was hydrophilic, resulting from the existence of hydrophilic HNTs, while the internal surface of the MMIMs was hydrophobic due to the use of hydrophobic monomers such as St and 4-VP. Owing to these properties, it was easy to pass the test solution through the semipermeable HNT shell on the external surface of the MMIMs, then λ-cyhalothrin molecules could be easily assembled at the imprinted sites.
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| Fig. 10 Chemical structures of the template and template analog molecules (a), uptake of λ-cyhalothrin, fenvalerate and diethyl phthalate by MMIMs and MNIMs (b). | ||
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5, v/v), until no λ-cyhalothrin leakage was observed. Finally, the prepared MMIMs were dried at 50 °C under vacuum. For comparison, magnetic non-molecularly imprinted microcapsules (MNIMs) were also prepared as a control in parallel but without the addition of λ-cyhalothrin.
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50 v/v) solution, and then the suspension was shaken in a thermostatically controlled water bath at 25 °C. After the desired time, MMIM (or MNIM) particles were isolated by an external magnetic field, and the solutions were immediately filtered through a millipore cellulose nitrate membrane (pore size was 0.45 mm) to remove suspended particles. The concentration of λ-cyhalothrin in the filtrate was determined by a UV-vis spectrophotometer at 278 nm (UV-2450, Shimadzu, Japan). The amount of captured λ-cyhalothrin was calculated by subtracting the amount of free λ-cyhalothrin from the initial amount added to the mixture.
To measure the specificity of the MMIMs, we incubated 10 mg of the MMIMs (or MNIMs) with 100 mg L−1 of λ-cyhalothrin, fenvalerate and diethyl phthalate in 10 mL of ethanol–water (50
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50 v/v) solution, and then proceeded to the binding experiments. After that, the concentrations of λ-cyhalothrin, fenvalerate and diethyl phthalate in the filtrate were determined by a UV-vis spectrophotometer at 278 nm, 277.5 nm and 275 nm, respectively. The selectivity of the imprinted polymers was determined by comparing the equilibrium adsorption ability to the template λ-cyhalothrin with that of the structural analogs.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c3ra43178a |
| This journal is © The Royal Society of Chemistry 2014 |