Jiangdong
Dai
a,
Yongli
Zou
c,
Zhiping
Zhou
*a,
Xiaohui
Dai
b,
Jianming
Pan
b,
Ping
Yu
d,
Tianbian
Zou
a,
Yongsheng
Yan
b and
Chunxiang
Li
*b
aSchool of Material Science and Engineering, Jiangsu University, Zhenjiang 212013, China. E-mail: Zhouzp@ujs.edu.cn; Fax: +86-0511-88791800; Tel: +86-0511-88790683
bSchool of Chemistry and Chemical Engineering, Jiangsu University, Zhenjiang 212013, China. E-mail: ujs2013txh@163.com
cSchool of Environment and Safety Engineering, Jiangsu University, Zhenjiang 212013, China
dSchool of Computer Science, Jilin Normal University, 1301 Haifeng Street, Siping 136000, China
First published on 14th October 2013
In this work, a facile and general protocol to synthesize molecularly imprinted microspheres (MIMs), combining reverse atom transfer radical polymerization with precipitation polymerization, is described. Well-tuned surface properties in the as-obtained microspheres were achieved through the “living” nature of the active ATRP-initiators present on the surface in order to further functionalize the microspheres with hydrophilic poly(2-hydroxyethyl methacrylate) (PHEMA) brushes. The presence of a PHEMA shell on the MIMs was confirmed by SEM, FT-IR and water contact angle studies, and some quantitative information is also provided. Batch adsorption experiments were carried out in pure water to investigate the equilibrium, kinetics and selectivity properties of the imprinted materials. The adsorption data of the ungrafted imprinted materials for sulfamethazine (SMZ) were fitted well to the Freundlich isotherm model. However, after grafting, the Langmuir isotherm fits the data better, mainly because of the changes to the surface properties that increase the hydrophilicity and suppress the hydrophobically driven non-specific interactions. The imprinted microspheres exhibit a large adsorption capacity, and are also specific to SMZ but non-specific to other antibiotics. The obtained materials also show rapid kinetics and great reusability and stability, displaying potential for practical applications for the selective removal of pollutants from aqueous environments.
Over the past decade, and even with the rapid progress of a research hotspot such as the molecular imprinting technology, a number of challenges still remain to be addressed. Particularly, the previously synthesized MIPs can be successfully used for efficient molecular recognition of a large range of target molecules, predominantly non-aqueous solvents.17 However, current protocols often fail to generate MIPs exhibiting the capacity for capturing specific templates from pure aqueous media, due to the significant hydrophobically driven non-specific binding between the molecule and the exposed material's surface.18,19 Besides, excessive cross-linkers are commonly employed to fix and stabilize the imprinted cavities, thereby making it difficult to adjust and control their binding properties. However, there are still few versatile approaches for the development of new MIPs applicable in pure aqueous systems.
In order to suppress the non-specific binding, two useful strategies have been developed by improving the surface hydrophilicity of the MIPs closer to that of biological receptors, which can be potentially applicable in separation or sensors in aqueous environments. The first one is based on the direct addition of appropriate amounts of hydrophilic co-monomers in the imprinting process, including 2-hydroxyethyl methacrylate (HEMA),20 acrylic acid (AA),21N-isopropylacrylamide (NIPAAm),22 or acrylamide (AAM)23 as functional monomers, as well as poly(ethylene glycol diacrylate) (PEGDA),24 and N,N-methylenebisacrylamide (MBAA)25 as cross-linkers. In spite of the simplicity and directness for the above methods, the optimization of the formulation components during the imprinting process is rather complicated and time-consuming, because the materials' properties are largely influenced by many parameters (e.g. the type and amount of the hydrophilic co-monomers added) or have a limited range of application. The second one focuses on post-modifications of already preformed MIPs by chemical modification of the surface functional groups (e.g. epoxide ring opening26 or covalent coupling of ligands27) or surface-grafting of hydrophilic shielding polymers.28 The preparation of hydrophilic MIPs is thus more versatile and flexible, by involving the independent processes of a first normal imprinting method and the subsequent modification. The grafting of hydrophilic polymers from the MIPs surfaces has draw great attraction, due to the hydrophilicity of the surfaces and functional layers which prevents biological macromolecules from blocking the imprinted cavities.29
Well-defined polymers with various tailored architectures were prepared via controlled “living” radical polymerization techniques (CRPs) in the past decade,30 including atom transfer radical polymerization (ATRP), nitroxide-mediated radical polymerization (NMP), reversible addition-fragmentation chain transfer (RAFT) polymerization, and iniferter-induced “living” radical polymerization. With respect to the free radical polymerization, the use of CRPs in the synthesis of highly cross-linked 3D polymers is considered to generate more homogeneous structures, because of the improved match in chain growth and chain relaxation.31 Compared to other CRPs, ATRP is chemically versatile and compatible with a broad range of usable monomers and functional groups, and presents a good tolerance towards a relatively high degree of impurities, whose controllability lies in a fast, dynamic equilibrium established between the dormant species (alkyl halides) and active radicals, with transition-metal complexes acting as reversible halogen atom transfer reagents.32 Recently, owing to the existence of “living” fragments, ATRP, as one of most powerful CRPs, has been utilized in molecular imprinting for the controlled synthesis of advanced MIPs with well-tuned architectures and improved binding properties, including bulk polymers,33 microspheres,34 MIP nanotube membranes,35 surface-imprinted core–shell particles.36 To the best of our knowledge, however, the preparation of MIPs with pure water-compatible properties bearing functional polymer brushes by a facile grafting-from method via ATRP, and especially by reverse atom transfer radical polymerization (RATRP) taking advantage of the “living” nature of the alkyl halide fragments, has not been reported to date.
The aim of this study was therefore to obtain imprinted materials capable of selective recognition and separation of the analytes from pure aqueous media with minimum non-specific binding. As a consequence of the abuse in the use of sulfamethazine (SMZ), herein selected as the template molecule, it has been found in aquatic environments, increasing the public concern on the potential human health risks due to serious side effects such as allergies, carcinogenesis, and possible development of antibiotic resistance.37,38 Imprinted microspheres with surface-immobilized “living” fragments were prepared via a method combining RATRP with precipitation polymerization in a methanol–water mixture, and then used as macro-ATRP agents for further modification with hydrophilic polymer brushes (PHEMA). The physical and chemical properties of the as-prepared materials were characterized by FT-IR, SEM, water contact angle tests, and water dispersion stability studies. The binding properties of the ungrafted MIPs and grafted MIPs in pure water was investigated in detail.
:
1.0; v/v) were successively added into a 50 mL one-neck round-bottom flask. After a long self-assembly reaction time at room temperature, CuBr2 (11.2 mg, 0.05 mmol), PMDETA (0.021 mL, 0.1 mmol), and AIBN (24.63 mg, 0.15 mmol) were added, and the reaction mixture was then deoxygenized with nitrogen for 0.5 h and sealed. The flask was then submerged in an incubator shaker at a rate of 160 rpm and the polymerization was carried out at 60 °C for 24 h. The as-synthesized products were collected by centrifugation and subsequently eluted through a Soxhlet extraction with methanol–acetic acid (9.0
:
1.0; v/v) until no template could be detected in the extraction solution. Non-imprinted microspheres (NIMs) were prepared under the same conditions, except for the absence of the template.
:
1.0, v/v) were successively added into a one-neck round-bottom flask (25 mL). After being degassed under ultrasonication and exchanged with nitrogen for 0.5 h, the flask was sealed and immersed in a water bath at 40 °C and stirred for 24 h. After centrifugation, the resulting solid products were thoroughly washed with methanol until no white sediments were detected when ether was added to the washing solutions; and then dried at room temperature under vacuum to a constant weight, giving MIPs with polymer brushes with a yield of 110.5 mg. Non-imprinted microspheres with PHEMA brushes (HNIMs) were also prepared following the above procedure, with NIMs with alkyl-halides groups instead of MIMs, with a yield of 109.8 mg.
The calculated SEM size data reflect an average of more than 200 particles in a representative area from the SEM images, which were obtained according to the following formulas:
Dynamic light scattering (DLS) measurements were also carried out in a thermostat bath regulated at room temperature on a Bettersize 2000 apparatus (Dandong Baite Instrument Co., China) in order to measure the autocorrelation functions.
The MIMs, NIMs, HMIMs and HNIMs were dispersed in ethanol under ultrasonication, with a concentration of 15 mg mL−1, and then dropped on clean glass surfaces to prepare the polymer thin films. After the solvent was allowed to evaporate at ambient temperature overnight, a KSV CM200 contact angle instrument (Finland) was utilized to determine their static water contact angles. Two measurements were taken for each sample, with the mean being used for analysis.
A UV-2450 UV-vis spectrophotometer (Shimadzu Corporation, Japan) was used to detect the concentration of the samples by their corresponding absorbance. A reverse-phase HPLC system (Agilent 1200 series, U.S.A.) was equipped with a UV-vis detector to achieve the simultaneous detection of several samples.
Suspensions of MIMs, NIMs, HMIMs and HNIMs in pure water (1.0 mg mL−1) were first dispersed by ultrasonication, respectively, and then allowed to settle down for 2.0 h at 25 °C to check their dispersion stability.
O stretching), 1258 and 1150 cm−1 (C–O–C stretching) confirm the existence of EGDMA in the polymers.39 Moreover, the small peak at 1638 cm−1 belongs to some unreacted C
C double bonds of EGDMA molecules used as cross-linkers in the polymers. The characteristic peaks arising from the C
N stretching (1600 and 1558 cm−1) and C
C stretching (1460 cm−1) of the pyridine rings reveal that the 4-VP monomer participates in the imprinting polymerization.40 The C–H stretching vibration of the alkyl chain appears at 2958 and 2989 cm−1 for the –CH2 and –CH3 groups, respectively. The peak at 651 cm−1 is attributed to the C–Br group, demonstrating the presence of “living” groups. After the surface-initiated polymerization of HEMA, the characteristic broad band at 3400 cm−1 is assigned to the O–H stretching of HEMA. The vibration intensity of C–Br and C
N decreases appreciably. All the results indicate the successful synthesis of imprinted polymers and the subsequent grafting of the hydrophilic monomer on the “living” initiator on the surface.
Scanning electron microscopy was used to characterize the morphology, size, and size distribution of the obtained polymer microspheres. Fig. 3 shows the SEM images of MIMs, NIMs, HMIMs, and HNIMs. All four samples are smoothly spherical with a narrowly dispersed size distribution. The number-average diameter (Dn) obtained from the images for the MIMs and NIMs is 3.529 μm and 3.994 μm, respectively. In Table 1, the polydispersity indices (U) calculated for the MIMs and NIMs are 1.093 and 1.112, respectively. Compared to the ungrafted MIMs and NIMs, the thickness of the grafted hydrophilic polymer shells for HMIMs and HNIMs is 22 and 18.5 nm (according to ΔDn/2), respectively, with low U values. The statistical data from the SEM images is basically in accordance with the results obtained through dynamic light scattering (DLS) measurements (in Fig. S1†). These results further indicate the successful grafting of PHEMA brushes onto the MIMs/NIMs (Fig. 3).
| Samples | ΔW% | D n (μm) | U | L (nm) | Contact angle (°) | Yield % |
|---|---|---|---|---|---|---|
| MIMs | — | 3.994 | 1.093 | — | 128.8 ± 2.6 | 77.47 |
| HMIMs | 10.5 | 4.036 | 1.099 | 22.0 | 60.2 ± 1.5 | — |
| NIMs | — | 3.529 | 1.112 | — | 122.7 ± 2.1 | 72.48 |
| HNIMs | 9.8 | 3.568 | 1.101 | 19.5 | 59.3 ± 1.8 | — |
Water contact angle experiments were performed to investigate the surface hydrophilic properties of the prepared materials. The profiles of water drops on MIM/NIM and HMIM/HNIM films are shown in Fig. 4. The static water contact angles were determined to be 128.8° and 122.7° for the MIM and NIM films, respectively. After surface-grafting the hydrophilic polymer brushes, the static water contact angles of the HMIM and HNIM films were significantly reduced to 60.18° and 59.27°, respectively, exhibiting a significantly higher hydrophilicity than the ungrafted ones, and demonstrating the presence of PHEMA brushes on the surfaces of the HMIMs and HNIMs. Moreover, the dispersion stability of the materials prepared in water has been efficiently improved by the surface-grafting of hydrophilic polymer brushes.41Fig. 4c and f show the dispersion of the MIMs/NIMs and HMIMs/HNIMs in a concentration of 1.0 mg mL−1 in pure water at ambient temperature after resting for 2.0 h. It is clear that the ungrafted materials present much more sedimentation in pure water compared to the grafted ones, which demonstrate that the PHEMA chains are anchored on the surface of the MIMs/NIMs by covalent binding.
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| Fig. 5 Adsorption isotherms of MIMs, NIMs, HMIMs and HNIMs with SMZ in pure water (a), the imprinted factors for the ungrafted and grafted microspheres (b). | ||
Two classic isotherm models, namely Langmuir and Freundlich, were applied to simulate the equilibrium characteristics of the adsorption. The Langmuir model describes an idealized adsorption taking place at specific homogeneous sites within the adsorbent, not involving any intermolecular interaction of the adsorbate. In most cases, the Freundlich model, as an empirical equation, can be considered as a generalization of the Langmuir model suitable for a heterogeneous surface, removing the limitations of the idealization.
In general, the linear forms of the Langmuir42 and Freundlich43 models are expressed as:
![]() | (1) |
![]() | (2) |
As shown in Table 2 and Fig. 6, the experimental data were found to fit well the Freundlich isotherm in terms of the R2 value for the ungrafted microspheres. However, after the surface-grafting with the PHEMA brushes, the adsorption data of the HMIMs and HNIMs towards SMZ fitted better the Langmuir model compared to the Freundlich model. These results may be caused by the change in the hydrophilicity of the exposed surface, which decreases the intermolecular interactions of SMZ with the template molecule occupying a recognition site.
| Samples | The Langmuir model | The Freundlich model | |||||
|---|---|---|---|---|---|---|---|
| Q e,exp (μmol g−1) | Q m,c (μmol g−1) | K L (L μmol−1) | R 2 | K F ((μmol g−1) (L μmol−1)1/n) | 1/n | R 2 | |
| MIMs | 47.532 | 74.074 | 0.0138 | 0.9760 | 2.017 | 0.7018 | 0.9966 |
| HMIMs | 38.664 | 54.945 | 0.0182 | 0.9975 | 1.981 | 0.6838 | 0.9848 |
| NIMs | 36.974 | 60.241 | 0.0113 | 0.9623 | 2.076 | 0.7306 | 0.9967 |
| HNIMs | 25.782 | 36.364 | 0.0191 | 0.9954 | 1.990 | 0.6880 | 0.9742 |
![]() | ||
| Fig. 6 The Langmuir (a) and Freundlich model (b) fittings for the adsorption of SMZ on MIMs, NIMs, HMIMs and HNIMs, respectively. | ||
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| Fig. 7 Adsorption kinetic data of SMZ on HMIMs and HNIMs and the linear fitting to the pseudo-second-order model (inset). | ||
The rate of adsorbate uptake on the adsorbent is well described by adsorption kinetics. In this work, two kinetic models were used to analyze the kinetics of the adsorption data, the pseudo-first-order44 and pseudo-second-order45 models, the linear form of which can be expressed as eqn (3) and (4), respectively.
![]() | (3) |
![]() | (4) |
Here, Qe (μmol g−1) and Qt (μmol g−1) are the SMZ adsorbed amount at equilibrium and at time t, respectively, k1 (min−1) is the pseudo-first-order kinetics constant and k2 (g μmol−1 min−1) is the constant of the pseudo-second-order kinetics equation.
The kinetic parameters for the adsorption of SMZ on HMIMs and HNIMs according to the two models are tabulated in Table 3. The low R2 values and notable differences between the experimental and theoretical data for both HMIMs and HNIMs clearly demonstrate the poor fitting to the pseudo-first-order kinetics equation. From Fig. 7 and Table 3, it can be clearly seen that the pseudo-second-order model fits the experimental data quite well, and that the experimental and theoretical data are in good agreement with high R2 values. This indicates the suitability of the second-order kinetics model to describe the adsorption process of SMZ on the obtained polymers.
| The pseudo-first-order model | The pseudo-second-order model | ||||||
|---|---|---|---|---|---|---|---|
| Samples | Q e,exp (μmol g−1) | Q m,c (μmol g−1) | k 1 (min−1) | R 2 | Q m,c (μmol g−1) | k 2 (g μmol−1 min−1) | R 2 |
| HMIMs | 33.652 | 23.682 | 0.0497 | 0.765 | 33.652 | 0.005769 | 0.9993 |
| HNIMs | 23.241 | 20.739 | 0.0545 | 0.9589 | 23.317 | 0.005318 | 0.9996 |
![]() | ||
| Fig. 8 Adsorption selectivity of SMZ on the ungrafted and grafted MIMs and NIMs in single-antibiotic solutions (a) and in the presence of competitive pollutants (b). | ||
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c3ra44602f |
| This journal is © The Royal Society of Chemistry 2014 |