Yuxin Zhangabc,
Xue Quac,
FeiFei Wangc,
Gang Wuc,
Jinyang Lic,
Hua Hongc and
Changsheng Liu*abc
aThe, State Key Laboratory of Bioreactor Engineering, East China University of Science and Technology, Shanghai 200237, PR China. E-mail: qv_xue@163.com
bKey Laboratory for Ultrafine Materials of Ministry of Education, East China University of Science and Technology, Shanghai 200237, PR China
cEngineering Research Centre for Biomedical Materials of Ministry of Education, East China University of Science and Technology, Shanghai 200237, PR China
First published on 25th September 2015
The formation of thin films with imprinting sites that can be accessed more rapidly by target molecules is an improvement in bulk molecular imprinting polymers. To achieve suitable properties for specific application, on the basis of our previous study of bulk erythromycin (ERY) imprinted polymers, we here rationally design, generate and test surface-imprinted polymers specific for ERY. ERY-A surface-imprinted glass fibers (GF-MIPs) were fabricated using glass fibers as the matrix, methacrylic acid (MAA) as the functional monomer, ethyleneglycol dimethacrylate (EGDMA) as the cross-linker and azobis(4-cyanovaleric acid) as the initiator. Then, we specifically studied the effect of the solvent on the recognition performance of the GF-MIPs. 13C-NMR and isothermal titration calorimetry (ITC) measurements were employed to demonstrate that the addition of NH3·H2O can block the interactions between the –COOH group and the tertiary amine on ERY-A. The results of static adsorption and dynamic separation experiments also indicate that an increase of specificity can easily be obtained by mediating the solvent environment, thus satisfying the more stringent requirements of precise separation.
Erythromycin (ERY) is a collection of macrolide compounds produced by Saccharopolyspora erythrae. ERY-A is an active ingredient with the highest antibacterial activity among the erythromycins.12 In our previous work, we demonstrated methacrylic acid (MAA) to be the optimal functional monomer for ERY imprinting because MAA can provide multiple H-binding and strong electrostatic interactions for the ERY template.13 Compared to non-imprinted materials, the generated imprinted adsorbents extracted ERY from its industrial crystal mother liquor with greater specificity. However, this separation was still considered unsatisfactory because, in addition to ERY-A, ERY derivatives such as ERY-E and erythromycin enol ether (ERYee) also remained in the final extracts. The chemical structures of these three ERY compounds in Fig. 1 indicate that all of them have highly similar structures, and contain a tertiary amine group that can interact with MAA via electrostatic interaction. Unlike oriented H-binding, electrostatic interaction has been reported to have no direction that would arouse nonspecific binding, which is probably one of the reasons that precise separation cannot be achieved.14
Fig. 1 Chemical structures of (a) erythromycin A (ERY-A), (b) erythromycin E (ERY-E), (c) erythromycin enol ether (ERYee), (d) dexamethasone (DEX) and (e) kanamycin (KANA). |
The nature of the solvent used for the binding process can substantially influence the expression of specificity.15–17 For example, strong polar solvents have been reported to weaken the H-binding interactions between MIPs and the template.18,19 Protic solvent may also influence the electrostatic interaction, and protic solvents with high dielectric constants have been verified to interfere in the formation of functional monomers–template complexes.20,21 Several researchers have employed the solvent effect to mediate the binding selectivity of the adsorbents. For example, the effect of the polarity of the environment on molecular recognition ability, the variation of polymer recognition properties caused by the change of buffer concentration, pH and presence of organic solvents and the effect of the water content of the selected washing solvent on the recovery of MIP have been studied.22–24 Therefore, appropriate solvents can be used to achieve precise separation in structurally similar complexes, i.e., ERY systems.
In this study, we propose a strategy to block electrostatic interactions between MAA-based MIPs and ERY by utilizing a solvent containing NH3·H2O. We synthesized ERY-A surface-imprinted glass fibers GF-MIPs using MAA as a functional monomer and EGDMA as a cross-linker. We performed 13C-NMR and isothermal titration calorimetry (ITC) measurement to demonstrate that the addition of NH3·H2O can block the interactions between MAA and the tertiary amine of ERY-A. Static adsorption and dynamic separation experiments indicate that the imprinting factor and the selectivity of GF-MIPs for ERY-A are improved when an amount of NH3·H2O is added to the solvents. The results indicate that increasing the recognition accuracy of MIPs by simply mediating the solvent environment is feasible: this increased recognition accuracy would affect biomedical separation and diagnostics applications that require precise recognition.
The “crystal mother solution” is the residual liquid from the ERY crystallization process in industrial production, which includes small amounts of ERY-A and other ERY derivatives, some inorganic matter and other unidentified impurities. The solvent is a 5–10% acetone–water mixture.
ACPA (0.60 g) was dissolved in dichloromethane in a three-neck flask in an ice-salt bath, followed by the addition of 0.98 g of EDCI, 0.69 g of HOBT and 1.04 g of TEA. After 1 h of stirring, 3.00 g of amino-GF were added to the solution and the temperature of the bath was increased to 20 °C for 12 h. Then, the fibers were rinsed successively with dichloromethane, ethanol and water. After the fibers were dried under vacuum, initiator-grafted fibers GF–ACPA were obtained.
Modified fibers GF–ACPA (3.00 g) were added into a three-neck flask containing 100 mL of a mixed solvent of acetonitrile, followed by the addition of 0.44 g of ERY-A, 0.21 g of MAA and 2.2 g of EGDMA. The mixture was stirred constantly and purged with nitrogen gas for 1 h. The polymerization was then performed at 60 °C for 16 h. Thereafter, the template molecule was extracted from the resulting fibers by sequential washing with a methanol and acetic acid (v/v = 9:1) solution followed by washing with methanol until no residue of ERY-A was observed in the rinse solution. Finally, the purified GF-MIPs were dried under vacuum. The non-imprinted GF-NIPs were prepared according to the same procedure, except for the addition of the ERY-A template.
(1) |
The imprinting factor, IF, was used to demonstrate the difference in adsorption capacity between GF-MIPs and GF-NIPs for ERY-A. The IF was calculated according to the following equation:
(2) |
The specific adsorption capacity of GF-MIPs was investigated using kanamycin (KANA) and dexamethasone (DEX) for comparisons. The static adsorption tests of GF-MIPs and GF-NIPs for KANA and DEX were carried out mutually independently.
Furthermore, the effects of additional NH3·H2O on the electrostatic interaction were verified by isothermal titration calorimetry (ITC 200, Microcal, USA). All binding experiments were performed in solutions corresponding to those from previous adsorption experiments. In individual titrations, 2.0 μL of MAA (10 mM) was added from a microsyringe at intervals of 2 min into ERY-A solution (1 mM, 200 μL). All measurements were performed at 25 °C, with the microsyringe stirring at 1500 rpm. Control experiments were performed by injecting the MAA, along with additional NH3·H2O, into an ERY-A solution.
Fig. 2a shows the FTIR spectra of the grafted fibers GF-MIPs and GF-NIPs. Compared to the spectrum of bare GF, some new bands at 2923 cm−1, 2854 cm−1 and 1727 cm−1 appeared in the FTIR spectra of GF-MIPs and GF-NIPs. These bands represent the characteristics adsorption peaks of –CH3, –CH2–, and OC–O, respectively, which indicates that the polymers were successfully “grafted from” GF. Meanwhile, the morphologies of GF-MIPs and GF-NIPs were investigated by SEM. As shown in Fig. 2b, the GF substrates were coated by polymers, in contrast to the relatively smooth surface of GF. Magnified images of the GF-MIPs and GF-NIPs revealed rough surfaces that consisted of patches of polymerized protuberances. These results indicate that the polymerization process proceeded well.
Fig. 2 (a) FTIR spectra for GF, GF-MIPs and GF-NIPs. (b) Scanning electron microscopy (SEM) images of GF, GF-MIPs and GF-NIPs. |
We performed an adsorption isotherm study to evaluate the adsorption performance of the GF-MIPs and GF-NIPs. Using static binding assays, we determined that the adsorption capacities of the two samples differed substantially, as shown in Fig. 3. The nonlinear curve fitted to a one-site Langmuir binding model then yielded a perfect fit and a equilibrium constant of k = 2.38 mL μmol−1 for GF-MIPs (Table 1). The GF-NIPs exhibited less affinity (k = 1.72 mL μmol−1) for the template. In addition, the Qm for GF-MIPs (19.59 μmol g−1) was higher than that for GF-NIPs (Qm = 12.79 μmol g−1). However, the imprinting factor of GF-MIPs was not so high (IF = 1.53), which indicates that many targets were adsorbed nonspecifically by the GF-NIPs, which is unfavorable for further specific adsorption.
Qm (μmol g−1) | k (mL μmol−1) | IF | |
---|---|---|---|
GF-MIPs | 19.59 | 2.38 | 1.53 |
GF-NIPs | 12.79 | 1.72 |
The electrostatic interaction between the template and the fibers is likely the key point. Ionic bonds has been reported to be sufficiently strong to enable complex formation in a polar environment.14 However, the electrostatic interaction is nondirectional,30 which would cause nonspecific binding even in MIPs with template geometry-matched cavities. ERY-A and its derivatives all contain the tertiary amine group that can accept a proton. In our previous study, we used 13C-NMR measurement to demonstrate that a strong electrostatic interaction exists between the tertiary amine of ERY and the –COOH of MAA.13 On the basis of chemical shift changes of the C atoms on the ERY molecular structure when interacting with the functional monomer MAA, the strength of each binding site could be shown directly. We used the same approach to study the interaction of the two groups in a water–acetonitrile solvent. As shown in Fig. 4, Δδ represents the concrete values of the 13C chemical shifts on ERY-A when interacting with functional monomers. Colorful spots corresponding to the absolute value of Δδ (|Δδ|) on each carbon atom were pictured on the ERY-A structural formula to depict the alteration of the template magnetic environment. Fig. 4(a1) shows that large displacements of a number of resonances arise from the C atoms (C′3, C′4, C′7, and C′8 etc.) in the vicinity of the basic tertiary amine demonstrating that the protonation of the amine group and subsequent interaction, presumably with the opposite charge corresponding to the COO− anion, led to a substantial change in the magnetic environment of the adjacent C atoms.
Given that NH3 can also accept a proton, we attempted to use NH3·H2O to block the electrostatic interaction between –COOH and the tertiary. After an appropriate amount of NH3·H2O was added to the solvent, the obvious chemical shifts caused by the electrostatics became extremely weak, as shown in Fig. 4(a2) suggesting that NH4+ interacted with –COO− and successfully prevented the interaction between the tertiary amine and the –COOH group.
Meanwhile, more direct evidence for the blocking effect of the NH3·H2O was provided by isothermal titration calorimetry (ITC). To investigate the contributions of electrostatic and hydrogen-bond interactions upon the formation of the MAA/ERY-A complex, the binding behavior of MAA and ERY-A were further studied by the addition of NH3·H2O as a blocker for the electrostatic attraction between oppositely charged MAA and ERY-A. An initial binding experiment was carried out by adding MAA to the acetonitrile/water solution of ERY-A without NH3·H2O. Fig. 4(b1) shows the typical exothermic heat for MAA/ERY-A binding, from which the binding affinity (1.39 × 105 M−1) and enthalpy (−7.4 kcal mol−1) were calculated. The molar ratio of ERY-A and MAA was just 1:1 when the exothermic heat reached equilibrium. Combining these results with the results of the 13C-NMR analysis, we concluded that the tertiary amine of the ERY-A interacted with the –COOH group of MAA in a molar ratio of 1:1 and that this exothermic heating process was observable. We subsequently studied the binding behavior of MAA and ERY-A in the presence of NH3·H2O. The NH3·H2O was introduced before titration, where the molar amount of NH3 was slightly greater than the molar amount of MAA (mol:mol = 1.05:1). Fig. 4(b2) shows that almost no exothermic heat was observed, which clearly indicates that electrostatic interaction played a predominant role in the formation of the MAA/ERY-A complex and that the addition of NH3·H2O prevented the electrostatic interaction between the tertiary amine and the –COOH group. Because the useful range for an accurate binding affinity measurement by standard ITC is between 103 and 108 M−1, the destabilized hydrogen bond interactions between these two small molecules in aqueous solution might be too minuscule to be detected by ITC.31
The effect of the molar relationship between the blocker NH3·H2O and the –COOH incorporated into the polymers on the imprinting factor was studied. The imprinting performance of the MIPs and NIPs with various NH3/–COOH molar ratios is presented in Fig. 5a. The binding capacity of MIPs for ERY obviously decreased with increasing NH3/–COOH molar ratio. However, the IF increased gradually and the maximum value of more than 7 appeared at an NH3/–COOH molar ratio of 1:1, and a slight decrease was observed when an overdosage of NH3 was introduced. These results indicated that NH3·H2O prevented the electrostatic interaction between ERY and MIPs, thus inhibiting the nonspecific binding and improving the imprinting performance, also consistent with the NMR and ITC results. Then, We repeated the adsorption isotherm study in acetonitrile/water solution containing 1.05 eq. of NH3·H2O. Similarly, the Langmuir isotherm model was also used to evaluate the adsorption behaviors of GF-MIPs and GF-NIPs. The dashed curve shown in Fig. 5 indicates that the Langmuir equation fitted well for GF-MIPs, although the maximum adsorption capacity (Qm) was significantly decreased (Table 2). For non-imprinting fibers, the adsorption capacity over the entire range of concentrations was close to zero, and the binding isotherm could not be adequately fit using the Langmuir model because of the large margin of error. Thus, we regarded the Qe of GF-MIPs at a concentration of 2.18 μmol mL−1 as an approximate Qm value. Although the Qm values of both of the two fibers decreased, their IF values increased significantly by a factor of approximately 7.58. The GF-MIPs exhibited a remarkably good imprinting effect.
Qm (μmol g−1) | k (mL μmol−1) | IF | |
---|---|---|---|
GF-MIPs | 7.35 | 2.56 | 7.58 |
GF-NIPs | ≈0.97 | ∼ |
The selectivity tests of GF-MIPs were carried out under equilibrium binding conditions by using KANA and DEX as contrasting adsorbates. Their chemical structures are shown in Fig. 1. The equilibrium adsorption capacity (Qe) and the distribution coefficient (KD) of the selected adsorbates between the solution and the fibers are shown in Fig. 6. KD is defined as
(3) |
Fig. 6 Qe and KD of adsorbates on GF-MIPs and GF-NIPs under equilibrium binding conditions. Concentrations of the starting solution are all 2.73 μmol mL−1. |
As shown in Fig. 6, the amount of ERY-A adsorbed onto GF-MIPs with a value of 17.99 μmol g−1, was much higher than the amounts of other adsorbates. After a balanced amount of NH3·H2O was added, the adsorbed amount of ERY-A, 6.58 μmol g−1, was still the highest among all adsorbates (even though its adsorption capacity decreased). The calculated values of the distribution coefficients KD exhibited the same trend. The KD values of GF-MIPs for ERY-A were observed to be the highest for both “NH3·H2O free” and “NH3·H2O containing” groups: 7.33 mL g−1 and 2.51 mL g−1, respectively. GF-MIPs exhibited better adsorption capacity for the template than all of the other adsorbates. GF-MIPs still adsorbed large amounts of KANA in the test group without NH3·H2O, even though the amounts of KANA adsorbed onto GF-MIPs and GF-NIPs were not drastically different. However, in the group with additional NH3·H2O, there was little KANA adsorbed by GF-MIPs and GF-NIPs. Because KANA contains four amino groups, we speculated that the electrostatic interactions between these amino and –COOH groups on the fibers led to nonspecific adsorption. After sufficient NH3·H2O was added to form a barrier to the electrostatic interaction, the amount of KANA adsorbed plunged because of the lack of corresponding imprinting cavities as well as the lack of electrostatic interaction. Understandably, very little DEX, which does not contain any nitrogen-containing radicals, was adsorbed onto the two fibers in both the NH3·H2O-containing solution and the NH3·H2O-free solution. These results indicate that the imprinting fibers possessing microcavities with a good memory for the template work well in our acetonitrile/H2O system, where NH3·H2O can deactivate the –COOH and thus result in excellent specific adsorption performance. After NH3·H2O was added, even in the presence of hydrophobic interaction, these contradistinctive adsorbates had no complementary shapes with the imprinting cavities of GF-MIPs, thus resulting in little adsorption.
The nature of the solvent used for the adsorption experiment is also known to influence the imprinting effect of the MIPs. This effect is quite complicated for aqueous solutions.32,33 In general, a higher percentage of water can provide more hydrophobic solvent conditions for interaction. Because, hydrophobic interactions are nondirectional, they are detrimental to the specificity but can provide the power of adsorption.34 Discerning whether the hydrophobic interaction is benefit is difficult. Moreover, in the presence of polar solvents, particularly water, the theoretical H-bond interactions between solutes and adsorbents are destabilized.35,36 Therefore, we performed static adsorption experiments with NH3·H2O in acetonitrile–water solvents with percentage compositions of acetonitrile ranging from 20% to 100% (given the solubility of ERY). We then calculated the adsorption capacities of GF-MIPs and GF-NIPs for ERY-A using HPLC detection. Recent studies have shown that noncovalent imprinted polymers has been used mostly in the presence of polar solvents, especially water, to satisfy the requirements of applications; these solvents severely disturb the interactions based on hydrogen bonding among the molecules. Interactions such as ionic bonds and hydrophobic interactions, the predominant interactions in aqueous solution, have been suggested to be sufficiently strong to allow for specific adsorption in a polar solution.37,38 For our system, hydrogen bonds were also destabilized in acetonitrile/water solution and ionic bonds were hardly existent because of the blocking effect. Therefore, the imprinting mechanism here might be more complicated. Though simple hydrophobic interactions are generally nonspecific, these interactions are strong in aqueous solution and should thus make a critical contribution to adsorption. The complementary imprinting voids that match the steric structure of the template are presumed to provide the specificity of adsorption. The mechanism of this specific adsorption based on the combination of hydrophobic and other non-electrostatic interactions is not entirely clear; however, the literature contains numerous studies that demonstrate that noncovalent imprinted polymers exhibit good imprinting efficiency in aqueous solutions, without the benefit of electrostatic interactions.39,40
All results are shown in Fig. 7. Overall, the results indicated that the adsorbed amount of ERY-A tends to decrease with increasing percentage of acetonitrile in solutions because of the weakening of the hydrophobic interaction between GF-MIPs and ERY-A caused by the increasing proportion of the organic solvent. With low percentages of acetonitrile-20% and 30%-GF-MIPs exhibit a high binding capacity for ERY-A; however, the IF values were relatively low, because strong hydrophobic interactions under these conditions caused undesired nonspecific adsorption. When the percentage of acetonitrile was increased to 40%, the specificity of GF-MIPs for ERY-A had begun to manifest. In this case, the IF value increased to 7.14. We also observed that the IF values remained approximately the same as those of the solutions that contained more than 40% of acetonitrile (the IF values in 90% and 100% acetonitrile solutions could not be calculated because the Qe values of the GF-NIPs in these solutions were close to zero). Under these conditions, the specificity of the GF-MIPs for ERY-A did not change significantly with increasing acetonitrile percentage. These hydrophobic interactions and steric shape might explain why the specificity of GF-MIPs for the template did not significantly change as the percentages of acetonitrile was varied from 40% to 80%. On the whole, we chose the 40% acetonitrile–water solution as the mobile phase for further dynamic adsorption experiments considering both specificity and adsorption capacity of GF-MIPs.
To investigate the selectivity of GF-MIPs, competitive adsorption experiments were performed in a solution of ERY-A, ERY-E and ERYee standards (molar ratio = 5:3:2, which is similar to the molar ratio of the crystal mother liquid). Fig. 8 shows the binding quantity of the three ERY imprints and those for their corresponding non-imprinted control samples. In the absence of NH3·H2O, the GF-MIPs adsorbed much more ERY-A and other ERY-derivatives than GF-NIPs at each concentration. However, no differences were observed in the adsorption of GF-MIPs for these three ERY samples. GF-MIPs showed little specificity toward ERY-A while using structurally similar substances as competitive adsorbates. After the blocker was added, a comparison of the binding capacity of GF-MIP for different ERY samples revealed that NH3·H2O substantially influenced the selectivity. The binding of a relatively large quantity of ERY-A was achieved, and the binding performances of NIPs for various ERY were all poor, showing no difference. These results suggest that NH3·H2O as a blocker can effectively block nonspecific adsorption and improve the selectivity of the GF-MIPs.
Fig. 8 Adsorption capacity of GF-MIPs and GF-NIPs for ERY-A, ERY-E and ERYee. Total concentration of all three ERY: 2.73 μmol mL−1. |
A competitive adsorption study in a dynamic experiment model was performed to provide more robust evidence for template selective binding and to demonstrate the potential application in the ERY recovery from the ERY crystal mother liquid. In this study, we dissolved (in acetonitrile/water) the powder that we obtained by drying the “ERY crystal mother solution”. Then, these solutions (with or without NH3·H2O) continued to flow through the chromatographic columns that composed with the GF-MIPs or GF-NIPs bed. Meanwhile, the effluents were collected at regular intervals and the concentrations of the three analytes (ERY-A, ERY-E, ERYee) at each point were detected by HPLC. Fig. 8 shows that, as the solution passed through the column, ERY-A, ERY-E and ERYee all clearly flowed from the GF-MIPs column later than they flowed from the GF-MIPs column, both in the case of the “with NH3·H2O” group and in the case of the “NH3·H2O free” group. Obviously, the GF-MIPs exhibited better adsorption properties for ERY-A and its derivatives in the dynamic adsorption process. However, even the GF-MIP column could hardly separate the three very similar compounds (Fig. 9a). As we previously discussed, the adverse effects of the electrostatic interactions severely hindered the molecular recognition. A strong electrostatic interaction masked other interactions, and this electrostatic interaction existed between MAA and both ERY derivatives. Thus, fine separation for ERY-A from its derivatives using GF-MIPs directly is difficult, even when employing a dynamic model. Therefore, the “blocker”, NH3·H2O, was also added during the dynamic adsorption process. Fig. 9c shows the breakthrough curve of ERY-A, ERY-E and ERYee in the GF-MIPs column after NH3·H2O was added to the solutions. The breakthrough times of all three samples clearly differed. The leaking volume of ERY-A was estimated to be 4.2 BV, whereas those for ERY-E and ERYee were estimated to be 2.5 BV and 1.4 BV, respectively. During this process, ERY-A and other derivatives maintained a dynamic process of adsorption and desorption. Because the GF-MIPs bed had specificity for ERY-A, the intensities of interactions between the column and various ERY differed. Thus, these results show that the GF-MIPs bed column has good selectivity and specificity for ERY and tends to adsorb ERY-A preferentially over other derivatives under a dynamic condition. The dynamic binding test again demonstrated the effectiveness of employing NH3·H2O as a blocker to block the electrostatic interaction and improve the imprinting efficiency, which exhibits attractive application prospects for the precise separation of ERY-A from its recrystallization wastewater.
Fig. 9 Breakthrough curves of a GF-MIPs bed column and a GF-NIPs bed column; flow rate: 0.31 BV h−1; solution: 40% acetonitrile in water; (a) and (b) NH3·H2O free; (c) and (d) with 0.1% NH3·H2O. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra09497f |
This journal is © The Royal Society of Chemistry 2015 |