Hongyan Zhuab,
Yan Cuic,
Jie Wang*ad and
Huibin Qiu*c
aShanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China. E-mail: wangjie@sinap.ac.cn
bUniversity of Chinese Academy of Sciences, Beijing 100049, China
cSchool of Chemistry and Chemical Engineering, State Key Lab of Metal Matrix Composites, Shanghai Jiao Tong University, Shanghai 200240, China. E-mail: hbqiu@sjtu.edu.cn
dShanghai Advanced Research Institute, Zhangjiang Lab, Chinese Academy of Sciences, Shanghai 201204, China
First published on 25th March 2019
Coil–coil block copolymers rarely self-assemble into flat low-curvature micelles due to the lack of proper interchain association. Here, we report a facile route to prepare disk-like micelles through the self-assembly of amphiphilic polystyrene-b-polybutadiene-b-poly(2-vinylpyridine) triblock copolymers in a mixture of acetone and cyclohexane, which shows distinct selectivity towards the PS, PB and P2VP blocks. Subtle solvation/aggregation of these blocks in this frustrating solvent system provides access to low-curvature micellar structures, and thus favors the formation of uniform disk-like micelles. Further variation of the volume ratio of the mixed solvents also leads to the emergence of other interesting morphologies, including disk arrays, disk clusters and perforated disk-like micelles. This work provides a complementary insight into the solution self-assembly of block copolymers in a view of selective solvents and demonstrates a distinctive pathway to unconventional micellar nanostructures through the use of complex solvent systems.
Among these morphologies, disk-like micelles were relatively rarely observed and so far were generally fabricated by the use of (i) rod–coil BCPs with a conjugated block;16–18 (ii) crystalline–coil BCPs with a crystallization block (through crystallization-driven self-assembly)19–21 and (iii) polypeptide-derived BCPs.22–24 The presence of a rigid core-forming block appeared to be essential for the formation of flat (low-curvature) self-assembly nanostructures. Due to the lack of requisite stiffness, coil–coil BCPs were considered to be unfavourable for the formation of disk-like micelles, although a limited number of exceptions were found previously.25–29 These normally involved the introduction of particular counterions in the self-assembly of coil–coil BCPs with an ionic corona-forming block by adjusting the interfacial energy,30–32 or chemical modification of one chain block to finely tune the incompatibility toward the selective solvents.33–35 Consequently, it has remained a challenge to assemble coil–coil BCPs into discotic micellar morphologies via a simple, efficient and tunable route.
Herein, we developed a facile strategy to prepare disk-like micelles through the self-assembly of amphiphilic polystyrene-b-polybutadiene-b-poly(2-vinylpyridine) (PS-b-PB-b-P2VP) triblock copolymers in a frustrating solvent system that consists acetone and cyclohexane. This also enabled the formation of disk arrays, disk clusters and perforated disk-like micelles simply by tuning the volume ratio of acetone and cyclohexane, which provided further insights into the formation of low-curvature micelles and the sophisticate association between amphiphilic BCPs and solvents.
GPC was carried out on a Viscotek TDAMax Multidetector Gel Permeation Chromatograph. The detectors and the chromatography were controlled in an oven (25 °C). THF (Fisher) was used as the eluent, with a flow rate of 1.0 mL min−1. Samples were dissolved in the eluent (2 mg mL−1) and filtered with a filter (Titan, polytetrafluoroethylene membrane with 0.22 μm pore size) before analysis. Calibration was conducted using TDS-PS-NB-polystyrene standards (PS105K and PS245K) from Viscotek. To determine the molar mass of the block copolymers, aliquots of the first block were taken and the absolute molar mass of the first block was determined by GPC. The absolute molecular weights of the other two blocks were then determined by combining the molecular weight Mn of the first block from GPC measurements with the block ratio of the triblock copolymer which was obtained by integration of the 1H NMR spectrum (see ESI† for analytical details).
Atomic force microscopy (AFM) experiments were performed using a Bruker Dimension ICON scanning probe microscope equipped with a ScanAsyst-HR scanning accessory. Imaging was scanned by a ScanAsyst-Air prober (tip radius 5 nm) under ScanAsyst mode in the air at room temperature. Images were analyzed by NanoScope Analysis, an open source software program for AFM images. Samples were prepared by placing one drop (ca. 20 μL) of the solution onto a piece of freshly peeled mica.
Transmission electron microscopy (TEM) experiments were performed using a Tecnai G2 Spirit transmission electron microscope operating at 120 kV and equipped with a 4k × 4k Eagle CCD. Samples were prepared by placing one drop (ca. 10 μL) of the solution on a carbon-coated copper grid resting on a piece of filter paper to remove excess solvent. No staining of the samples was necessary.
Polymer | PDI | Mn (g mol−1) | Block ratio (P2VP/PS) | Block ratio (P2VP/PB) |
---|---|---|---|---|
PS260-b-PB170-b-P2VP300 | 1.14 | 67800 | ∼1.2 | ∼1.8 |
PS370-b-PB230-b-P2VP350 | 1.22 | 87800 | ∼0.9 | ∼1.5 |
PS580-b-PB660-b-P2VP920 | 1.25 | 192800 | ∼1.6 | ∼1.4 |
In a typical self-assembly experiment, PS-b-PB-b-P2VP was dissolved in THF to make a concentrated unimer solution (20 mg mL−1). An aliquot (40 μL) of the unimer solution was quickly injected into a mixture of acetone and cyclohexane. In this case, acetone serves as a near-Θ solvent for PS, but poor solvent for PB and good solvent for P2VP,13 while cyclohexane is a Θ solvent for PS,38 good solvent for PB, but poor solvent for P2VP (Fig. 1). The solubility parameters of the polymers (PS, PB, and P2VP) and solvents, and the Flory–Huggins parameters (χ) (polymer–solvent interaction strengths) were listed in Tables S1 and S2,† respectively.
In consideration of the distinct solubility feature of the PS, PB and P2VP blocks, we firstly explored the self-assembly of PS580-b-PB660-b-P2VP920 in pure acetone and cyclohexane, respectively. In acetone, the solution appeared as a white suspension, and AFM images indicated the presence of random aggregates of spherical micelles (Fig. 2a and c). According to the solubility preference, these spherical micelles were supposed to possess a PB core and a P2VP corona, with the PS block partially swelled (acetone is a near-Θ solvent for PS) and deposited at the core–corona interface. The association of the less solvable PS block may thus render the coagulation of the spherical micelles into irregular clusters. In cyclohexane, AFM images showed the formation of a mixture of spherical micelles and worm-like micelles (Fig. 2b and d). While the P2VP block aggregated into a core and the PB block formed the corona of a spherical micelle, the solvation of the PS block in such a Θ solvent was rather frustrated (the polymer chain normally forms coil but does not fully extend in a Θ solvent).39 It presumably caused the coalescence of the spherical micelles and consequently the emergence of the elongated micellar structures.13,40 This was also indicated by the dumbbell-like shape of the short worm-like micelles (denoted by red arrows) and the beam pod-like feature of the longer species (denoted by green arrows) (Fig. 2d). It seems that the PS-b-PB-b-P2VP triblock copolymer self-assembled in an unconventional manner in both acetone and cyclohexane, majorly as a consequence that PS swells but not actually dissolves in these solvents. However, the solubility of PS increases in a mixture of acetone and cyclohexane due to the cosolvency effect.41–43 Thus, it would be interesting to reveal the self-assembly behaviour of the PS-b-PB-b-P2VP triblock copolymer in various acetone/cyclohexane mixtures.
To this end, acetone and cyclohexane were mixed in different volume ratios and used for the self-assembly experiments. In the cases of relatively low acetone/cyclohexane ratios (≤30/70), PS580-b-PB660-b-P2VP920 predominantly formed uniform spherical micelles (Fig. S7b–d†). With an increasing in the amount of acetone (acetone/cyclohexane = 40/60), the spherical micelles were slightly deformed and concave dimples were formed on the surface (Fig. S7e†). This was presumably due to the swell of the P2VP core and the compression of the PB corona in a heavier acetone atmosphere.
A further increase of acetone (acetone/cyclohexane = 45/55) led to the formation of disk arrays with the coexistence of discrete disks (Fig. 3). AFM height and 3D images showed that the disk arrays consisted of lateral connected disks with height of ∼6 nm. The boundary (height ∼ 15 nm) where the disks connected with each other was significantly higher than the disk center, forming the “mountains”, and the area of the “basins” was slightly smaller than that of the individual disks, indicating a considerable collision of the disks. This strongly indicated that the disk arrays formed directly in solution, rather than as a consequence of a dry effect where loosely packed aggregates would be most possible.
The aforementioned large disk arrays disappeared in the 50/50 acetone/cyclohexane mixture, in which relatively small clusters were detected instead (Fig. S7g†). The disks were again laterally linked together, with aggregation number varying from 2 to 15. At acetone/cyclohexane = 55/45, the solution mainly produced disk trimers and dimers, and a large portion of individual disks (Fig. 4a and e). Morphologically pure disk-like micelles with diameter of ∼100 nm (estimated standard deviations σ = 23 nm by AFM) and height of ∼6 nm were observed at acetone/cyclohexane = 60/40 (Fig. 4b and f). AFM 3D images showed that the disk-like micelles possessed a slight rough surface (Fig. 4c and d). Moreover, TEM images further confirmed the presence of disk-like micelles (Fig. 4g), although the diameter appeared to be much smaller, probably due to the invisible corona under the electron beam.
Interestingly, perforated disk-like micelles emerged when the acetone/cyclohexane ratio was increased to 65/35 (Fig. 5 and S7h†). The size of holes varied in a wide range from 5 nm to 100 nm, and the relatively large holes generally adopted irregular shapes (Fig. 5b and c). Notably, the periphery of the holes (height > 10 nm) was obviously higher than the intact disk areas (height ∼ 8 nm). It appeared that the perforation occurred after the formation of the disk-like micelles through a process similar to piercing a paper. The perforated disk-like micelles were also detected by TEM images (Fig. 5d and e), excluding a drying effect (for AFM, samples were deposited on mica, a relatively hydrophilic surface, while for TEM, samples were deposited on carbon film, a relatively hydrophobic surface).
For acetone/cyclohexane ≥70/30, where acetone became dominant, PS580-b-PB660-b-P2VP920 majorly self-assembled into spherical micelles (Fig. S7i–k†).
It was apparent that the combination of acetone and cyclohexane sophisticated the self-assembly of PS580-b-PB660-b-P2VP920. Although the exact mechanism was not clear yet, it was postulated that: (i) due to the cosolvency effect, the PS block dissolves well in the acetone/cyclohexane mixtures with moderated volume ratios and thus essentially/additionally stabilizes the resulting micellar structures; (ii) with an increase in the acetone fraction, the PB corona gradually contracts and aggregates, while the P2VP core swells, leading to a decrease in the corona/core volume ratio, and consequently the transition from high-curvature spherical micelles to low-curvature discotic micelles; (iii) at acetone/cyclohexane of 45/55–55/45, the PB block partially collapses but yet retains as a soft/adhesive layer along the interface of the PS corona and the P2VP core, and thus causes the tethering and collision of the disk-like micelles; (iv) the further solvation and stretching of the P2VP core under a higher acetone/cyclohexane ratio destabilizes the disk structures and thus perforation occurs (compared to the intact disk micelles that formed at acetone/cyclohexane of 60/40, an increase of acetone might cause the shrinkage of the PB corona and a swelling of the hydrophilic P2VP core, resulting in an eruption of the P2VP blocks from the center of disks and the formation of pores. However, the equilibration of the micellar structure would be substantially restricted by the slow chain migration of the high-molecular-weight polymer blocks and the fact that the evolution of the P2VP domain might be kinetically prevented by the collapsed PS corona, leading to the immergence of a mixture of perforation disks with various pore sizes).
In a further experiment, IPA, which is a good solvent for the P2VP block, but a poor solvent for the PS and PB blocks, was employed to replace the role of acetone. However, across the full range of mixed IPA/cyclohexane solvents, PS580-b-PB660-b-P2VP920 exclusively self-assembled into spherical micelles, but failed to formed disk-like micelles (Fig. S8†). Again, it indicated that the combination of acetone and cyclohexane, which create a frustrating situation for the dissolution and coalescence of the PS, PB and P2VP blocks, is essential for the formation of the low-curvature micellar structures.
We also explored the self-assembly of PS370-b-PB230-b-P2VP350 and PS260-b-PB170-b-P2VP300 with much smaller molecular weights than PS580-b-PB660-b-P2VP920 in the acetone/cyclohexane mixtures. In an analogous manner, PS370-b-PB230-b-P2VP350 self-assembled into spherical micelles under low (≤30/70) and high (≥80/20) acetone/cyclohexane ratios, but formed complex micellar structures in the middle regions (40/60–70/30) (Fig. S9†). Irregular disk arrays were formed at acetone/cyclohexane = 50/50 and 60/40 (Fig. S9f and g†), while ill-shaped toroidal micelles emerged at acetone/cyclohexane = 65/35 (Fig. S9h†). Besides, pearl necklace-like structures were also observed upon a slightly higher feeding of acetone (Fig. S9i†). Similarly, PS260-b-PB170-b-P2VP300 self-assembled into spherical micelles in 30/70 and 70/30 acetone/cyclohexane mixtures, but formed slightly perforated disk-like micelles from acetone/cyclohexane = 40/60 to 60/40 (Fig. S10†). The height of the resulting disk-like micelles decreased from ∼6 to ∼3 nm, while the diameter expanded, with an increase in the acetone fraction (Fig. S10b–d and f†).
Footnote |
† Electronic supplementary information (ESI) available: Experimental details and additional results. See DOI: 10.1039/c9ra01145e |
This journal is © The Royal Society of Chemistry 2019 |