Xue Liua,
Yu Houa,
Xiuping Tanga,
Qiuhua Wua,
Chenglin Wub,
Jie Yia and
Guolin Zhang*a
aLiaoning Province Key Laboratory for Green Synthesis and Preparative Chemistry of Advanced Materials, College of Chemistry, Liaoning University, Shenyang, 110036, P. R. China. E-mail: glzhang@lnu.edu.cn; Fax: +86-24-6220-2380
bSchool of Pharmaceutical and Chemical Engineering, Taizhou University, Taizhou, 317000, P. R. China
First published on 6th January 2016
Multicompartment micelles are prepared via the hierarchical co-assembly of two diblock copolymers, poly(ε-caprolactone)-b-poly(ethylene glycol) (PCL-b-PEG) and poly(ε-caprolactone)-b-poly(4-vinylpyridine) (PCL-b-P4VP) in aqueous solution. These two polymers first assemble into mixed shell micelles through hydrophobic interaction among PCL chains. PCL chains form the micellar core, while PEG and P4VP chains form the micellar shell. Regulating the pH value above the pKa of P4VP can induce hydrophobic phase-segregated P4VP patches forming on the surface of mixed shell micelles. When hydrophilic PEG chains cannot stabilize theses micelles with hydrophobic patches, they will furthermore assemble as the subunits into MMs with different morphologies. These MMs can be revealed by transmission electron microscopy through P4VP chains positive staining.
This concept of MMs drew inspiration from organized biological systems, such as perfectly functioning proteins, which possess complex quaternary structures composed of several subunits combining diverse properties, environments, and functions. A simple natural example for such systems is serum albumin, which owns several independent “binding pockets” of different quality, and enables selective uptake and release of different “transport goods” in blood, such as poorly water-soluble compounds.9 These subunits are first constructed through the precise folding of peptides, and then the assembled subunits further proceed the hierarchical assembly into the final multi-subunit protein structure.
Inspired from these natural structure, MMs are also constructed by multi-level assembly, taking multi-block copolymers or multiple copolymers as the basic blocking units.10 The assembling process in solution can be driven by various noncovalent interactions, such as hydrophobic interactions, electrostatic interactions, hydrogen bonding and so on. However, most of the time, with increasing size and complexity of the subunits, the kinetic obstacles become significant and trapping of metastable species can occur, preventing well-defined solution hierarchies of low polydispersity on an appropriate timescale.11,12 Müller and his coworkers carried out a series of systematical studies about the MMs constructed with simple linear ABC triblock terpolymers through the directed step-wise hierarchical self-assembling method.13–16 The intermediate pre-assembly of subunits without precedent structural control was fabricated in the first step. Homogeneous MMs were constructed via solvent-regulated hierarchical self-assembly of the intermediate pre-assembled subunits. Compared with the previous one-step dissolution (or direct dialysis) method, this directed self-assembly led to a step-wise reduction of the degree of conformational freedom and dynamics and avoided undesirable kinetic obstacles during the structure build-up.
Müller's method to prepare MMs through directed step-wise self-assembly using pre-assembled subunits is very enlightening. However, there exit some problems for the basic building blocks–triblock terpolymers, which usually involve in numerous and complicated synthetic procedures. In addition, the structural adjustment of the MMs assembled by triblock terpolymers is realized through regulating the polymerization degree of each block, which results in more synthetic tasks. The nanostructure assembled by triblock terpolymers can also be prepared through direct mixing of two kinds of diblock copolymers, which is also called co-assembly strategies.17 The materials constructed via co-assembly strategies have shown potential as smart carriers in drug delivery processes.18–20 Such concepts have also been employed for the preparation of MMs.21–24 For example, micelles with a mixed shell can be assembled by ABC triblock terpolymers. The insoluble B block forms the micellar core, and the soluble A and C blocks extent into the solution to form the mixed shell. Such mixed shell micelle can also be constructed by mixing AB and BC amphiphilic diblock copolymers, and the assembling process is shown in Scheme 1. Compared with the MMs constructed by triblock terpolymers, the composition, structure and property of the MMs can be conveniently designed and adjusted only through changing the composing proportion of these two diblock copolymers. Therefore, in this research, we selected two amphiphilic diblock copolymers as the basic building blocks to construct the subunit of MMs.
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| Scheme 1 Schematic representation of the micelle with a mixed shell assembled by one triblock terpolymer or two diblock copolymers. A and C: soluble blocks; B: insoluble block. | ||
A pH-responsive mixed shell polymeric micelles (MSPMs) were prepared as the subunit to construct MMs through the co-self-assembly of two amphiphilic diblock copolymers: poly(ε-caprolactone)-b-poly(ethylene oxide) (PCL-b-PEG) and poly(ε-caprolactone)-b-poly(4-vinylpyridine) (PCL-b-P4VP) in solution. Hydrophobic PCL chains aggregated and formed the core of the MSPMs, while the hydrophilic PEG chains and P4VP chains spreading around the surface of the MSPMs formed the mixed shell. P4VP is a pH dependent polymer with a pKa at ca. 4.5–4.7.25 Below the pKa, P4VP is soluble as a weak cationic polymer due to the protonation of the pyridine groups. Above the pKa, due to the deprotonating effect, P4VP turns hydrophobic. Therefore, when regulating the pH value in solution above the pKa of P4VP, phase transition from hydrophilicity to hydrophobicity happened to P4VP. Accordingly, MSPMs evolved into MMs with various structures and morphologies. The structure and morphology of the MMs depend on the composition of the MSPMs. When P4VP content is less, PEG chains can stabilize the micelles. Hydrophobic P4VP chains collapse on the surface of the micelles and form separated patches, and MSPMs transform into core–patch–corona micelles (CPCMs). Further increasing the content of P4VP chains on the surface of MSPMs, separated and hydrophobic P4VP patches will aggregate into continuous phase. If there are enough hydrophilic PEG chains, ‘inverse hamburger’ micelles can be formed and stable in solution without aggregation. When PEG chains cannot stabilize the micelles anymore, MSPMs will transform into transient and unstable Janus-type micelles, which will further assemble into MMs with novel morphologies, including ‘hamburger’ micelles, ‘football’ micelles and ‘vesicle-like’ micelles. The morphology types depend on the assembling number of the participant subunits. The structure and morphology of the MMs could be observed clearly through staining the TEM (transmission electron microscope) samples with uranyl acetate.
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3 v
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v, 8 mL) was added. After freeze–degas–thaw cycles, polymerization was performed at 45 °C for 4 hours. The mixture was purified by dialyzing against water in a dialysis bag with a molecular cutoff of 7 KD, and PCL-b-P4VP was obtained after lyophilization.| Mn from 1H NMR (×104) | Mn from GPC (×104) | PDI | |
|---|---|---|---|
| PCL–Br | 1.14 | 0.99 | 1.19 |
| PEG-b-PCL | 1.11 | 1.59 | 1.11 |
| PCL-b-P4VP | 2.05 | 1.92 | 1.08 |
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| Scheme 2 Schematic representation of the structure of the as-prepared subunits based on the mixed shell polymeric micelles (MSPMs). | ||
During the preparing process of the MSPMs, PEG-b-PCL and PCL-b-P4VP were dissolved in the THF solution with the same concentration (1 mg mL−1). Therefore, the MSPMs with different compositions (PEG-b-PCL/PCL-b-P4VP = 3/1, 1/1, 1/4 and 3/17, mass ratio) were prepared through directly mixing these two diblock copolymers THF solutions with various volume ratios before replacing the co-solvent into the selective solvent, and the final achieved MSPMs with corresponding mass ratios of PEG-b-PCL to PCL-b-P4VP. A similar method had been applied to confirm the formation of the MSPMs instead of a simple mixture of PEG-b-PCL micelles and PCL-b-P4VP micelles.31 PCL-b-P4VP micelles would aggregate and precipitate when P4VP chains turn hydrophobic in alkaline solution, while MSPMs can keep stable with the protection of hydrophilic PEG chains. There was no precipitation appearing in alkaline MSPMs solution, which can effectively confirm that MSPMs have been formed.
DLS and SLS tests were applied to determine the morphological parameter of these subunits. Fig. 2A shows the plot of the translational diffusion coefficient (D) versus q2 of the MSPMs with four compositions. From the fitted line, the translational diffusion coefficient D0 were calculated by extrapolating q2 to 0 at a polymer concentration of 1.0 mg mL−1. The translational diffusion coefficient D of the micelles are almost constants, which suggests the MSPMs are spherical. The hydrodynamic diameter distribution f(Dh) of the MSPMs is shown in Fig. 2B (scattering angle = 90°), which suggest that the Dh of the MSPMs is very narrowly distributed. The average hydrodynamic radius (Rh) according to Stokes–Einstein equation, radius of gyration (Rg) and Rg/Rh value are listed in Table 2. Along with the increase of the relative content of PCL-b-P4VP in the MSPMs, it should be pointed out that the Dh of the MSPMs has an increase from 90.8 to 121.7 nm. The hydrophobic PCL chain length of PCL100-b-P4VP87 is longer than that of PCL80-b-PEG45, which enlarged the grain diameter of the final MSPMs. It is well known that the Rg/Rh value reflects the morphology or conformation of polymer chains or the density distribution of particles in solution.32 Compared with the uniform sphere (Rg/Rh ≈ 0.775), the Rg/Rh of the MSPMs is a little larger, which suggests the structure of the MSPMs is relatively incompact.33 Moreover, from MSPMs (3/1) to MSPMs (3/17), the Rg/Rh value increased from 0.813 to 0.953 and the structure of the MSPMs turned more and more incompact. We observed the morphology of the as-prepared subunits, and MSPMs (3/17) were chosen as the monitoring object (Fig. 3). The micellar size observed in the TEM image is similar than that from the DLS results, which is ca. 100 nm. However, the TEM images present the samples under dried state, so the resulted sizes are less than those in solution. From the TEM image, we can see that, P4VP chains are stained by uranyl acetate and show a higher contrast. There exists a little phase-separation among PEG and P4VP chains on the surface of the subunits, which can be owe to the compatibility of two polymers. P4VP is hydrophilic in this situation, and therefore such phase-separation cannot result in an aggregation.
| MSPMs (PEG-b-PCL/PCL-b-P4VP) | Rg/nm | Rha/nm | Rg/Rh |
|---|---|---|---|
| a We substitute Rh at the scattering angle of 90° for those obtained by angular extrapolation for simplification because all of the micellar systems involved in this study have monodisperse and narrow size distributions, no remarkable angular dependence of the translational diffusion coefficient Dt of these systems are observed in the scattering angle range of 35–135°, i.e., Rh calculated from Dt by the Stokes–Einstein equation do not have a remarkable angular dependence. | |||
| MSPMs (3/1) | 73.9 | 90.8 | 0.813 |
| MSPMs (1/1) | 95.5 | 107.1 | 0.892 |
| MSPMs (1/4) | 109.9 | 115.7 | 0.949 |
| MSPMs (3/17) | 116.0 | 121.7 | 0.953 |
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| Fig. 3 TEM image of the subunit composed of PEG-b-PCL/PCL-b-P4VP (3/17) stained by uranyl acetate (pH = 2.0). | ||
Light scattering tests were applied to characterize the as-prepared MMs with different compositions. The results are presented in Fig. 4 and Table 3. From the plot of Dt versus q2 and the distribution of Dh, the translational diffusion coefficient D of the MMs are almost constants, which demonstrate the freshly-formed MMs with different compositions still keep spherical. The Dh of MMs is narrowly distributed, which confirms the homogeneity of the MMs. However, compared with the original MSPMs, the Rh of MMs increase obviously. The main reason for this is that the MMs can consist of several subunits, which enlarge their grain diameter. For the subunits with different compositions, along with the increase of their hydrophobic area, more subunits assembled together and formed a larger aggregation, which make the corresponding MMs exhibit an increasing grain diameter. At the same time, the increase in the assembling subunits make the structure of the MMs more incompact.
| Multicompartment Micelles (MMs) (PEG-b-PCL/PCL-b-P4VP) | Rg/nm | Rha/nm | Rg/Rh |
|---|---|---|---|
| a We substitute Rh at the scattering angle of 90° for those obtained by angular extrapolation for simplification because all of the micellar systems involved in this study have monodisperse and narrow size distributions, no remarkable angular dependence of the translational diffusion coefficient Dt of these systems are observed in the scattering angle range of 35–135°, i.e., Rh calculated from Dt by the Stokes–Einstein equation do not have a remarkable angular dependence. | |||
| MMs (3/1) | 74.1 | 92.8 | 0.798 |
| MMs (1/1) | 100.8 | 121.1 | 0.832 |
| MMs (1/4) | 111.9 | 131.8 | 0.849 |
| MMs (3/17) | 124.5 | 145.5 | 0.856 |
1H NMR and 2D NOE spectra were used to further study MSPMs and their corresponding assembly-MMs. MSPMs (1/1) were taken as the observing object in D2O under acidic condition, while MMs (1/1) could be formed through raising pH value in MSPMs solution. In Fig. 5, peaks a (8.0–8.7) and b (7.1–7.6), due to P4VP blocks, are evident in the spectrum of MSPMs, which means that P4VP blocks on the surface of MSPMs are water soluble. On the contrary, for MMs, peaks owing to P4VP blocks disappear, indicating that P4VP blocks turn hydrophobic and MSPMs transform into MMs. When two protons of chemically different monomers are in close proximity (distance < 0.5 nm), cross peaks will be present in the 2D NMR spectrum.34 Therefore, 2D NOE may provide valuable insights into MSPMs and MMs. Fig. 6 shows the NOESY spectra of MSPMs (1/1) and MMs (1/1). Cross peaks could be observed at the intersection of the 1H NMR signals of P4VP and PEG in the spectrum of MSPMs (Fig. 6A), which confirms PEG and P4VP chains homogeneously mixed in the shell of MSPMs. However, the cross peaks are not observed in the spectrum of MMs (1/1) (Fig. 6B), meaning that microphase separation occurs among PEG and P4VP chains and MMs come into being.
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| Fig. 6 2D NOE spectra of MSPMs (A) and MMs (B) in D2O. Arrows indicate where cross peaks between P4VP and PEG should occur in case of close proximity. | ||
Furthermore, TEM was applied to visualize the structure of the MMs. The details of the TEM samples can be enhanced by stains. Herein, uranyl-acetate, which can positively stain the P4VP chains of the MMs, was used to enhance the contrast of the various composition compartments in the MMs. In the TEM images, P4VP chains are stained by uranyl-acetate and show darker contrast. From these TEM images, MMs with different phase separation structures can be clearly observed. The morphology of these MMs is dependent on the composition of the subunits.
When P4VP chains are less, hydrophilic PEG chains can stabilize the micelles, and hydrophobic aggregation cannot occur among micelles themselves. In Fig. 7A, stained hydrophobic P4VP chains aggregate as the dark patches spread around the surface of the MMs (3/1), indicating that MMs (3/1) are mainly CPCMs. The size of CPCMs is ca. 100 nm in the TEM image, which is smaller than that from the DLS results (200 nm). Both TEM image and DLS results show a uniform size distribution of CPCMs.
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| Fig. 7 TEM images of the MMs constructed by the subunits with four compositions of PEG-b-PCL/PCL-b-P4VP (pH = 7.0). | ||
When P4VP contents further increase and the composition of the MSPMs reaches to 1/1, from the TEM image (Fig. 7B), we can see that, the morphology of the MSPMs (1/1) transforms into ‘inverse hamburger’ micelles. So many hydrophobic P4VP patches aggregate that continuous P4VP hydrophobic phase comes into being on the surface of the micelles. Such ‘inverse hamburger’ micelles can also further evolve and assemble under some conditions. For example, creating a non-solvent environment for PEG chains, ‘inverse hamburger’ might proceed colloidal polymerization and form worm-like ‘colloidal polymers’, which have appeared in some literatures.35 However, in our system, PEG chains are still sufficient and hydrophilic to stabilize the micelles and prevent their aggregation. Therefore, only ‘inverse hamburger’ micelles can be observed. The resulted ‘inverse hamburger’ micelles possess a size of ca. 150 nm, which is a little smaller than that from DLS results (ca. 220 nm).
According to Müller's literature,13 further increasing the hydrophobic P4VP components, the morphology of the MSPMs can transit into transient Janus-type micelles (Scheme 3(4)). Janus-type micelles have too many hydrophobic P4VP areas and less hydrophilic PEG chains so that they cannot be stable in solution anymore, which makes them difficult to be caught solely in solution. However, we find diverse hierarchical assembling morphologies by Janus-type micelles in Fig. 7C, including ‘hamburger’ and ‘football’ micelles. ‘Hamburger’ micelles can be assembled by two subunits. When the assembling subunits appear in different sizes, the resulted hierarchical assembled morphology can be interesting ‘pinecone’ micelles—a kind of special ‘hamburger’ micelles. Multi-subunits can also assemble into ‘football’ micelles. Though TEM image presents various morphologies of MMs, their size distribution from DLS results (Fig. 4B) is still relatively narrow, and the Rh we got is ca. 250 nm, which indicates that the MMs constructed by MSPMs (1/4) may focus on ‘hamburger’ micelles mainly.
Furthermore, when MSPMs (3/17) acted as the basic building subunits to construct MMs, the MMs with a completely fresh structure could be observed in the TEM images (Fig. 7D). We speculate that this kind of structure of MMs might be vesicle-like, which is rarely observed in MMs system.36 Under some conditions, amphiphilic copolymers with P4VP blocks can form vesicular structures. For example, the relatively short P4VP block biases the formation of bilayered structures in a selective solvent.37 However, different from the vesicular structure in the literatures, the vesicular wall in our system seems thicker in the TEM image and their structure is also more compact from the Rg/Rh results in Table 3. The reason for this is probably that the building unit for our vesicle-like structure is Janus-type micelles, instead of direct macromolecular amphiphile in the literatures. The forming mechanism of such structure need further research and discussion.
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