Yinwen Liab,
Huilong Guoab,
Jian Zhengab,
Jianqun Ganab,
Yan Zhangab,
Xiaoxiao Guanab,
Kun Wua and
Mangeng Lu*a
aKey Laboratory of Cellulose and Lignocellulosics Chemistry, Chinese Academy of Sciences, Key Laboratory of Polymer Materials for Electronics, Guangzhou Institute of Chemistry, Chinese Academy of Sciences, Guangzhou 510650, PR China. E-mail: mglu@gic.ac.cn; liyinwen06@126.com
bUniversity of Chinese Academy of Sciences, Beijing 100039, PR China
First published on 15th October 2014
Novel macromolecular star polymers with triazole and cyclodextrin (CD) segments as branch points and poly(oligo(ethylene glycol)methacrylate) (POEGMAs) as dense hydrophilic branches were synthesized via a combination of azide–alkyne click chemistry and atom transfer radical polymerization (ATRP). Firstly, a tetrafunctional linking agent (PETP) was prepared by the reaction of pentaerythritol (PE) and propargyl bromide, and then a four arm β-CD terminated star polymer (PE-CD) was obtained through the click chemistry reaction. Finally, thermally-responsive star polymers (PE-CD–POEGMAs) with PE as the central core, triazole and CD segments as branch points, and POEGMAs as side branches were synthesized by the ATRP of MEO2MA and OEGMA using PE-CD terminated with bromines as macroinitiators. A study on the thermoresponsivity and morphology of PE-CD–POEGMAs indicated that polymeric nano-aggregates existed as multimolecular micelles and behaved with tunable thermosensitivity, which were driven by the strong hydrophobic–hydrophilic interactions in the inner core and outer shell. The encapsulation capacities towards multi-guest molecules were investigated and the results indicated that water soluble guests could be encapsulated by PE-CD–POEGMAs, and the guest encapsulation capacities were derived from the special star molecular structure properties of PE-CD–POEGMAs and the synergistic encapsulation phenomenon of different guest molecules. This unique amphiphilic star polymer illustrated the potential applications in supramolecular science, drug delivery and other nanotechnology applications.
Stimuli-responsive polymers are often referred to as intelligent polymeric systems because they exhibit reversible property changes between micellar and unimer states in response to changes of external conditions such as pH, temperature, ionic strength and light irradiation, among them, thermoresponsive polymers are potentially interesting for a wide range of applications such as enzyme recycling, protein chromatography, drug delivery, or tissue engineering.14–22 Classic thermoresponsive polymers exhibit aqueous LCSTs include poly(N-isopropylacrylamide) (PNIPAAm), poly(N-acryloylpyrrolidine), poly(vinyl methyl ether), polypeptides, poly(dimethylaminoethyl methacrylate), which have been by far the most studied and applied.23–25 Recently, poly(oligo(ethylene glycol)methacrylate)s (POEGMAs) were reported to possess similar or even superior thermosensitivity than PNIPAAms. POEGMAs have good phase transition reversibility and tunable lower critical solution temperature (LCSTs) in aqueous medium, the biocompatibility of POEGMAs is also excellent and attractive. To date, POEGMAs have been widely incorporated into block or star copolymers, polymeric brushes and hydrogels, which endow these materials with more interesting properties.26–35 However, to endow star polymers with thermoresponsivity, thermo-responsive monomers or polymeric parts are usually introduced as building blocks; PNIPAAms have been successfully incorporated to various dendrimers or star polymers to form thermo-responsive core–shell nanostructures,36–39 but only few works have been done on introducing POEGMAs into star polymers especially with cyclodextrins (CDs).
Encapsulation is one of the most attractive areas in contemporary supramolecular chemistry and shows great potential in drug delivery, medical diagnostics and materials science. Encapsulation materials include liposomes, chitosan, crown ethers, and cyclodextrins etc. can be defined as functional polymers which show superior encapsulation properties due to their special macromolecule structures and unique physicochemical characteristics.40–50 amphiphilic linear block or pseudo block polymers are known for their ability to self assemble into polymeric nano-aggregates which have been considered as good candidates for encapsulation investigations and applications, however, the formed nano-aggregates are usually unstable and easily dissociate with altered environmental parameters.51–53 Compared with amphiphilic linear polymers, amphiphilic nonlinear polymers such as dendrimers, star polymers, and hyperbranched polymers with branched architectures can stably exist as unimolecular micelles or multimolecular micelles in aqueous solution because of their unique chemical structures, and their encapsulation behaviors have been studied and mainly focused on single guest encapsulation.54–57 Most recently, the encapsulation phenomena of multi-guest molecules using amphiphilic hyperbranched polymers was reported by Tian et al.58 However, there are still few attentions and researches on encapsulation of amphiphilic thermal responsive star polymer with CDs and hyperbranched POEGMAs as building blocks for multi-guest molecules.
Our research group previously investigated the synthesis and supramolecular self-assembly of a variety of stimuli-responsive POEGMAs with complex architectures. Motivated by recent attempts in the most attractive areas of encapsulation in contemporary supramolecular host–guest chemistry, herein the synthesis and characterization of thermoresponsive star polymers with PE as the central core, triazole and CD segments as the branch points, and POEGMAs as branches were reported, and the encapsulation behaviors of this newly synthesized star-shaped polymers using rose bengal (RB), levofloxacin lactate (LL), rhodamine B (Rh) and congo red (CR) as guest molecules were investigated in details.
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| Scheme 1 The molecular structures of rose bengal (RB), levofloxacin lactate (LL), rhodamine b (Rh) and congo red (CR). | ||
:
1) for at least three times. The purified PE-CD–Br48 was collected, washed with acetone, and dried under reduced pressure. Yield: ≈65%. FT-IR (KBr): 3385 cm−1 (O–H); 1720 cm−1 (C
O). 1H NMR (DMSO-d6, TMS): δ (ppm) 7.95 (1H, methine proton in 1,2,3-triazole); 5.70–5.95 (2,3-OHs of β-CD); 4.90–4.98 (1-Hs of β-CD); 3.31–3.92 (8H, C(CH2)4, overlaps with 2,3,4,5,6-Hs in β-CD); 1.85–1.90 (CH3).
:
1.5 v/v), PE-CD–Br48 (1 eq.) initiator and copper bromide (57 eq.) was added to a Schlenk tube, degassed via three freeze–thaw–pump cycles and back-filled with argon. Then 2,2-bipyridyl (120 eq.) was added. The mixture was heated at 50 °C in an oil bath for six hours. The experiment was stopped by opening the flask and exposing the catalyst to air. The final mixture was diluted in ethanol and passed through a short silica column (60–200 mesh) in order to remove copper catalyst. Then, the filtered solution was diluted with deionized water and subsequently purified by dialysis in water (Roth, ZelluTrans membrane, molecular weight cut-off: 7000). Last, freeze-drying in vacuum PE-CD–POEGMAs was obtained as clear viscous solid. Yield: ≈43%. The synthetic routes employed for the preparation of PE-CD–POEGMAs are shown in Scheme 2.
The LCSTs were determined by UV-vis spectroscopy (U-3010 Spectrophotometer), and transmittance of the polymeric aqueous solutions (1 mg mL−1) was recorded at temperatures ranging from 20 °C to 70 °C. The lower critical solution temperature (LCST) of the aqueous polymer solution at specific concentration was determined as the temperature corresponding to 10% decrease in the optical transmittance. The hydrodynamic diameters (Dh) of the capsules and their polydispersity indices (PDI) were determined by dynamic light scattering (DLS) on a Malven Zetasizer Nano System (Nano-zs90). The emulsions were passed through 1.0 μm filters before DLS measurements. The measurements were conducted in a 3.0 mL quartz cuvette, using a 670 nm diode laser, and the scattering angle used was 90°. Each set of Dh and PDI values was the average from five measurements. The morphology and architecture of nano-sized aggregates were further visualized by transmission electron microscopy (TEM), and the samples were prepared by placing polymer aqueous solution on copper grids in a biochemical incubator thermostatted at 25 °C or 50 °C, and stained with phosphotungstic acid before observation on a JEM-100CX II microscope operated at 80 kV.
Firstly, as shown in Scheme 2, the synthesis of the four-arm star polymers started from the synthesis of tetrakis(2-propynyloxymethyl)methane (PETP). The synthetic methods of PETP reported in previous literatures are somewhat ambiguous and the results are even completely contradictory.60–62 In order to improve the synthetic method and productivity of PETP, treatment of pentaerythritol by our modified method with propargyl bromide and NaH synthesized the target PETP in good yield. The FT-IR and 1H NMR spectra of PETP are shown in Fig. 1 and 2(a), separately. The chemical shifts at 4.12 (8H, –OCH2), 3.54 (8H, C(CH2)4), and 2.43 (4H, CH) were attributed to protons originating from pentaerythritol and propargyl segments. Moreover, in the FT-IR spectrum of PETP, the disappearance of the stretching vibration peak of the hydroxyl group at 3443 cm−1, together with the appearance of the characteristic absorption peaks of alkynyl groups (2111 cm−1, 3285 cm−1) suggested that the terminal hydroxyl groups of pentaerythritol completely reacted with propargyl bromide.
Next, PE-CD was synthesized by the click reaction between PETP and an excess of CD-N3. In the 1H NMR spectrum of PE-CD (Fig. 2(b)), the characteristic signals for β-CD at δ = 3.20–4.30, 4.40–4.90, 5.70–5.95 ppm and the proton peak of the 1,2,3-triazole ring at δ = 7.95 ppm appeared, indicating the occurrence of the 1,3-dipolar cycloaddition reaction. Moreover, in the FT-IR spectrum of PE-CD, the stretching vibration peak of the hydroxyl reemerged suggesting that CD terminals were bonded to the PETP-end. Meanwhile, the characteristic absorption of the azido group at 2104 cm−1 and those of the alkynyls at 2111 cm−1 disappeared, which further confirmed the complete click and removal of the unreacted CD-N3. The MALDI-TOF-MS result of PE-CD (Fig. S1 in the ESI†) also showed that the m/z of PE-CD + xNa+ was 4878.23, which is quite agreement with the theory molecular weight (4931). Moreover, we also used SEC measurement to further confirm the molecular weight, although the molecular weight was somewhat larger than the actual molecular weight, but the PDI (Mw/Mn) was just 1.07. Therefore, based on above analysis PE-CD was successfully synthesized.
To graft thermoresponsive POEGMAs chains to the CD terminated PE-CD, selective esterification was first conducted on the CD moieties to introduce bromines into PE-CD. BIBB was used to react with the hydroxyl groups of β-CD. As a result, PE-CD based macroinitiators bearing several bromrines at the CD moieties were obtained. The 1H NMR spectra of PE-CD–Brx are shown in Fig. 3. Signals associated with the 2-bromoisobutyryl residue (–C(CH3)2Br) in PE-CD–Brx were clearly discernible at δ = 1.85–1.90 ppm, indicating that bromines have been successfully introduced into PE-CD. According to previous reports, due to the difference in activity among the 2,3,6-OHs selective modification can be fulfilled by carefully controlling the reaction conditions, normally the hydroxyls adjacent to C-2, -3 and -6 of β-CD (2,3,6-OH) are all able to react with BIBB during a typical esterification procedure. However, the actual conversion ratio of this reaction was not up to 100%, because bromoisobutyryl bromide is very active, and easily react with the residual H2O in the reaction system, in order to maximum control the number of hydroxyls of CDs to react with bromoisobutyryl bromide, we first reduced the H2O as best as we could, then added excessive amount of bromoisobutyryl bromide to PE-CD to ensure the proper ATRP macroinitiators what we wanted and designed. The best mole ratio of PE-CD to BIBB was 1
:
1.5x for the synthesis of PE-CD–Brx (x ≈ 16), 1
:
2.5x for the synthesis of PE-CD–Brx (x ≈ 48). The number average x of Br was calculated to be 15.7 and 47.5 by 1H NMR based on integral ratios of resonance peaks from triazole rings at 7.95–8.0 ppm and –OCO–C(CH3)2Br groups at 1.85–1.90 ppm. The synthesis and characterization of PE-CD–Brx are summarized in Table 1. Combined the FT-IR, 1H NMR, SEC, and the MALDI-TOF-MS (Fig. S2 and S3 in the ESI†) results of PE-CD–Brx the basic ideal ATRP macroinitiators were synthesized.
| Samples | Mn,theorya | Mn,NMRb | m/zc | Mn,SECd | PDId |
|---|---|---|---|---|---|
| a Calculated in accordance with the theory feed ratio.b Calculated in accordance with the 1H NMR results.c The MALDI-TOF-MS results.d Molecular weights and molecular distributions (Mw/Mn, PDI) were determined by SEC using DMF as eluent relative to polystyrene standards. | |||||
| PE-CD | 4931 | — | 4878.23 | 5904 | 1.07 |
| PE-CD–Br16 | 7315 | 7136 | 7419.03 | 8740 | 1.12 |
| PE-CD–Br48 | 12 083 |
11 306 |
12 560.67 |
19 320 |
1.15 |
Using PE-CD–Brx with 2-bromoisobutyryl active initiations as the macroinitiators, and MEO2MA and OEGMA as comonomers, star polymers, PE-CD–POEGMAs (P1 and P2) were synthesized via ATRP, and the synthesis and characterization are summarized in Table 2. The FT-IR and 1H NMR spectra of PE-CD–POEGMAs are shown in Fig. 4 and 5. In the FT-IR spectrum of PE-CD–POEGMAs (P2), the stretching vibration peak of the carbonyl group (C
O) increased compared with PE-CD–Br48. Moreover, in the 1H NMR spectrum of PE-CD–POEGMAs (P2), although the signals of 2,3,4,5,6-Hs (protons on C-2, C-3, C-4, C-5 and C-6 position of β-CD) overlapped with the Hs of the methylene protons and the methoxyl protons in PEG chains in the region of δ = 3.40–4.10. The characteristic signals of β-CD, together with that of the 1,2,3-triazole ring, can also be observed at δ = 4.40–4.85, 5.70–5.95 and 7.95, indicating that PE-CD–POEGMAs was successfully synthesized.
| Samples | Macroinitiator | nMEO2MA : nOEGMA |
Mn,SECb | PDIb | LCSTc (°C) |
|---|---|---|---|---|---|
| a Synthesized by the ATRP of MEO2MA and OEGMA using PE-CD–Brx as macroinitiators.b Molecular weights and molecular distributions (Mw/Mn, PDI) were determined by SEC using DMF as eluent relative to polystyrene standards.c Measured with a concentration of 1.0 mg mL−1, temperature increase at 1 °C min−1 by UV-vis spectroscopy. | |||||
| P1a | PE-CD–Br16 | 95 : 5 |
82 747 |
1.24 | 41.03 |
| P2a | PE-CD–Br48 | 95 : 5 |
155 135 |
1.28 | 43.71 |
The potential applications of polymers in biomaterials related fields are known to be generally related to the aqueous media. Therefore, the thermoresponsivity and morphology of the synthesized PE-CD–POEGMAs in an aqueous solution were observed by DLS and TEM. The typical intensity diameter distributions of P2 at 25 °C and 50 °C are shown in Fig. 6. At 25 °C, these particles with Z-average diameters of 156.8 nm with PDI = 0.23 for P2, suggested that the polymer might exist as polymeric aggregates rather than unimolecular micelles in aqueous solution, which is driven by the strong hydrophobic–hydrophilic interactions in the inner core and outer shell. While when the temperature rose above the LCST, it was found obviously that PE-CD–POEGMAs could self-assemble into more evenly nano-sized aggregates, the basically uniform aggregates formed with a Z-average diameter (DZ) of 104.3 nm with a narrow PDI of 0.072 for P2.
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| Fig. 6 Size distributions of the aggregates formed by P2 in aqueous solution (0.2 mg mL−1) at 25 (a) and 50 °C (b), separately. | ||
To examine visually the size and morphology of PE-CD–POEGMAs, the typical TEM image of P2 is presented in Fig. 7. Spherical micelles with a concentration of 0.2 mg mL−1 were found to be uniformly dispersed in the aqueous solution. These micelles, constructed from PE-CD–POEGMAs, showed light core surrounded by a black, thin corona, presenting a typical micellar characteristic, and it was apparent that the polymers appeared as uniform particles with the diameter of 70–120 nm, which was consistent with the DLS analysis. This result indicated that these micelles consist of hydrophobic PE and triazole rings as the inner core and hydrophilic POEGMA chains as the external shell. Scheme 3 summarizes the thermally-induced self-assembly behaviors for PE-CD–POEGMAs. It existed as aggregates in aqueous solutions and the thermoresponsiveness of the POEGMAs in the shell of micelles allowed a controlled phase transition into aggregates above LCST.63–66
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| Fig. 7 Typical tem images obtained by aqueous solutions of P2 (0.2 mg mL−1) at 25 (a) and 50 °C (b). | ||
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| Scheme 3 Schematic illustrations of the thermally-induced self-assembly and possible encapsulation behaviors with single or multi-guests for PE-CD–POEGMAS. | ||
Generally, polymeric micelles can be prepared by adding water to an organic solution of polymers until the required amount of water for micelle formation is obtained. However, previous reports have demonstrated that micelles can also be formed by direct dissolved amphiphilic polymers in water.58,59 In this work, the stable multimolecular micelles could be formed by direct dissolved PE-CD–POEGMAs into water. The self-assembly process was fast and did not require other special conditions. Therefore, this multimolecular micelle system prepared by the newly synthesized PE-CD–POEGMAs might be more fascinating. To confirm quantitatively the formation of multimolecular micelles, the CMC was estimated by fluorescence spectrophotometry using pyrene as a hydrophobic probe. The excitation spectra of pyrene in the P2 solutions with various concentrations are shown in Fig. 8(a). The peak intensity increased and red shift was all observed with increased PE-CD–POEGMAs concentration, indicating the formation of micelles. The intensity ratio (I385/I373) of the pyrene excitation spectra versus the logarithm of the copolymer concentration is shown in Fig. 8(b). The CMC was obtained from the intersection of the baseline and tangent of the rapidly rising I385/I373, and the value was determined as 0.0043 mg mL−1 which further confirmed as multimolecular micelles in an aqueous solution for PE-CD–POEGMAs.
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| Fig. 8 (a) Excitation spectra of pyrene as a function of P2 concentrations in PBS buffer (pH = 7.4); (b) plot of I385/I373 against logarithm of P2 concentration. | ||
Fig. 9 represents changes of fluorescence intensities of LL and Rh depending on different concentrations of P2, separately. The enhanced fluorescence emission intensities of LL or Rh with increase of the polymer concentration indicated that PE-CD–POEGMAs encapsulated LL or Rh in the hydrophilic shell of PE-CD–POEGMAs micelles. Similar tendency was also observed for other guest molecules (RB and CR with P2 in Fig. S5 in the ESI†). All the polymeric guests (LL, RB, Rh and CR) investigated in this study were revealed a steady increase of the amount of encapsulated even at very low concentration without the presence of CMC. However, different from previous report, the above fluorescence enhancement results indicated the interactions of water soluble guests (LL, RB, Rh and CR) with the hydrophilic shell of the PE-CD–POEGMAs micelles, and also suggested that LL, RB, Rh and CR could not diffuse through the hydrophilic shell and interact with the hydrophobic micellar core. PE-CD–POEGMAs have large hydrophilic POEGMAs chains and small hydrophobic core, water soluble guest molecules were mainly encapsulated in the hydrophilic shell, which resulted in the fluorescence enhancement effect.
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| Fig. 9 Fluorescence emission spectra of LL (a) and Rh (b) at pH = 7.4 in the presence of different P2 concentrations. | ||
The encapsulation results of P1 with LL, RB, Rh and CR are shown in Fig. S6 in the ESI,† It was interesting to observe that the P1 also showed guest encapsulation capacities, but the increases of the fluorescence intensities with increasing of the polymer concentration were obviously lower than that of P2. While for P2, it showed more obvious increase in the fluorescence intensity with increasing of its concentration, which indicated that P2 can encapsulate guest molecules more efficiently. Although PE-CD–POEGMs had similar molecular structure, there were indeed existed differences for P1 and P2 with 16 and 48 branched POEGMAs. These results indicated that the encapsulation capacities were not only dependent on the polymer concentration but also dependent on the polymer molecular structures of PE-CD–POEGMAs.67
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| Fig. 10 Fluorescence emission spectra of LL + Rh (a), and CR + Rh (b) at pH = 7.4 in the presence of different P2 concentrations. | ||
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| Fig. 11 Fluorescence emission spectra of Rh + LL + RB (a), and RB + LL + Rh (b) at pH = 7.4 in the presence of different P2 concentrations. | ||
To further investigate the encapsulation capacity and mechanism of PE-CD–POEGMAs towards multi-guest molecules, consequently, gradual multi-guest encapsulation experiments were conducted.58 Rh was firstly added into P2 solution, and then LL or CR or RB was added with different amount, separately. The results of LL and CR are shown in Fig. 12 and RB is shown in Fig. S8 in ESI.† The results showed that the peak intensities decreased after the addition of the other guests LL, CR, RB, separately. Obviously, the encapsulation for P2 to Rh was far to the encapsulation balance and saturation, in other words, when go on adding LL or CR or RB, P2 would go on encapsulating the new added guest molecules. Therefore, Rh was encapsulated in the inner layer and behaved fluorescence decrease effect.
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| Fig. 12 Fluorescence emission spectra of Rh + P2 solutions with gradual adding of LL (a) or CR (b) solutions at pH = 7.4, respectively. | ||
When two guest molecules were simultaneously encapsulated into the P2 solution, then the third one was gradually added to the double guests system, and the results are shown in Fig. 13 and in Fig. S9 in ESI.† Taking Rh for example, when Rh + CR were simultaneously encapsulated into P2 solution, and then LL was gradually added, the results showed that the peak intensities of Rh increased, similar result was obtained for Rh + LL with gradually added CR. While for CR + LL with gradually added Rh, the peak intensities of CR + LL behaved puzzled which was resulted from the overlapped emission wavelengths of CR and LL.
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| Fig. 13 Fluorescence emission spectra of CR + Rh + P2 (a), LL + Rh + P2 (b) solutions with gradual adding of LL (a), CR (b) solutions at pH = 7.4, respectively. | ||
The possible explanation was that during the guest encapsulation process, both guest and host molecules would rearrange to maximize the interactions, and different guest molecules showed different synergistic encapsulation abilities based on their molecular properties.36,68 These results further indicated that besides the molecular structures of PE-CD–POEGMAs, the synergistic encapsulation phenomenon and molecular recognition property were also the driving force. Thus, the encapsulation capacity and interaction mechanism of PE-CD–POEGMAs towards multi-guest molecules are derived from the synergistic encapsulation phenomena of different guest molecules and the molecular recognition property of the hyperbranched structure, and the schematic representation for possible encapsulation mechanism of PE-CD–POEGMAs with single or multi-guests are shown in Scheme 3.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra10407b |
| This journal is © The Royal Society of Chemistry 2014 |