INTRODUCTION
- Top of page
- Abstract
- INTRODUCTION
- EXPERIMENTAL
- RESULTS AND DISCUSSION
- CONCLUSIONS
- Acknowledgements
- REFERENCES AND NOTES
Amphiphilic block copolymers represent a very interesting class of polymeric materials with a rich phase behavior.1 These materials self-assemble from the nanometer through the micrometer length-scales, both in the bulk and in solution, and find applications in a broad range of areas, including microelectronics, colloids, and medicine.2
There are many synthetic techniques available for the preparation of block copolymers with well-defined composition, molecular weight (MW), and structure. Besides the classical synthetic routes of living anionic3 and quasi-living cationic4 polymerizations, and the new controlled radical polymerization methods such as nitroxide-mediated polymerization (NMP),5 atom transfer radical polymerization (ATRP),6 and reversible addition–fragmentation chain transfer (RAFT) polymerization,7 combination of two living/controlled polymerization methods has also been applied for the preparation of block copolymers, expanding the range of monomers that can be used.
Several examples on the combination of anionic polymerization with the different controlled radical polymerizations have been described in the literature.8 Usually, the first monomer is polymerized via anionic polymerization, followed by the modification of the chain ends into functional groups which can be used as initiating sites for the polymerization of the second monomer. In particular, anionic polymerization has been widely combined with ATRP6,9 and NMP6,10 for the preparation of block and graft copolymers, as well as for star copolymers.
The literature also includes some examples on the combination of anionic and RAFT polymerizations for the synthesis of block copolymers. In the first such study, Brouwer et al.11 described the chain extension of hydroxyl end-functional poly(ethylene-co-butylene) (number-average MW, Mn of 3800 g mol–1) prepared by the anionic polymerization of butadiene followed by hydrogenation, with styrene (Sty)/maleic anhydride via RAFT polymerization (block copolymers with MWs < 23,000 g mol–1). Following this first study, Xu and Huang12 synthesized a series of well-defined diblock terpolymers of poly(ethylene oxide)-b-poly(styrene-co-2-hydroxyethyl methacrylate) (PEO-b-P(Sty-co-HEMA)), with MWs ranging from 16,900 to 38,800 g mol–1, using anionic and RAFT polymerizations for the first and second blocks, respectively. In addition, the same researchers also synthesized a PEO-b-P(Sty-co-HEMA)-g-poly(ε-caprolactone) (PEO-b-P(Sty-co-HEMA)-g-PCL) graft quaterpolymer by the grafting of CL units from the hydroxyl groups of the HEMA units using ring opening polymerization (ROP). Moreover, Hillmyer and coworkers published on the combination of anionic and RAFT polymerizations for the preparation of several copolymers.13–15 First, they reported13 the synthesis of three different poly(ethylene-alt-propylene)-b-PEO-b-poly(N-isopropylacrylamide) (PEP-b-PEO-b-PNiPAm) triblock terpolymers, with PEP and PEO MWs of 3000 and 25,000 g mol–1, respectively, while the PNiPAm MW was varied at three values, 4000, 10 000, and 21,000 g mol–1. The synthesis of the first block was accomplished by the anionic polymerization of isoprene, followed by end-capping with one unit of ethylene oxide, and completed by the hydrogenation of the double bonds in the isoprene units to yield hydroxyl-terminated PEP. The resulting polymer was further anionically polymerized using a counterion different from that used in the first step to give PEP-b-PEO, which was subsequently end-functionalized by the attachment of a RAFT chain transfer agent (CTA). This diblock macroRAFT CTA was extended with NiPAm via RAFT polymerization to give the final PEP-b-PEO-b-PNiPAm triblock terpolymers. In another work,14 these researchers presented the synthesis of polyethylene-b-poly(N, N-dimethylacrylamide) (PE-b-PDMA) and PEP-b-PDMA diblock copolymers, with PE and PEP MWs both of 3000 g mol–1 and final diblock copolymer MWs of 12,000 and 15,000 g mol–1, respectively, combining living anionic and RAFT polymerizations, following a similar procedure to that described in the previous example. More recently, the same workers15 prepared PEP-b-(PDMA-grad-2-(methacrylamido glycopyranose)) (PEP-b-P(DMA-grad-MAG)) diblock terpolymers using the same macroRAFT PEP, which was further polymerized with DMA and trimethylsilyl-protected MAG (TMS-MAG) through RAFT polymerization, while the final diblock terpolymers were obtained after the hydrolysis of the TMS-MAG unit.
Thus, in the previous studies involving the combination of anionic and RAFT polymerizations, low-to-medium MW copolymers were prepared. In the present study, we aim at expanding this MW limit to high-to-very-high values. The particular monomer pair was chosen to secure a large thermodynamic incompatibility between the blocks of the resulting copolymers, so that they microphase separate in the bulk and be studied by electron microscopy. Although both monomers are polymerizable by both anionic and RAFT polymerizations, this work provides a proof of concept that the particular combination of polymerization methods can lead to diblock copolymers of very high MW. Extension to other monomers, specific to each of the two polymerization methods, would be straightforward.
This study addresses another timely issue in polymer science, that of size polydispersity in block copolymers. There has recently been an understanding that block copolymers can still microphase separate in the bulk, even when they are heterogeneous in size, implying that it is not necessary that their synthesis be carried out using living anionic polymerization when morphology formation is desired.16 Thus, block copolymers prepared using other, less demanding and less expensive methods, and, in particular, controlled radical polymerization, can also be used when self-assembly in the bulk is required. Although it does not prevent microphase separation, polydispersity highly influences the type of morphology obtained. A particular literature example17 most dramatically demonstrated this by presenting three diblock copolymers with the same average composition but a polydisperse second block with different polydispersity indices, giving lamellae, gyroids, or cylinders, depending on the polydispersity index. The mechanism by which polydispersity impacts microphase separation is through the reduced stretching energy exhibited by the polydisperse blocks which can fill space more efficiently, leading to the formation of larger domains and also to the shift of order–order transitions toward compositions higher in the polydisperse component.18 Polydispersity also affects the onset of microphase separation, facilitating it when the polydisperse block forms the minority domains, but opposing it in the reverse case. This study exactly presents the development of a model diblock copolymer system comprising a low-polydispersity first block made by living anionic polymerization, and a less homogeneous second block prepared by RAFT polymerization.
CONCLUSIONS
- Top of page
- Abstract
- INTRODUCTION
- EXPERIMENTAL
- RESULTS AND DISCUSSION
- CONCLUSIONS
- Acknowledgements
- REFERENCES AND NOTES
Three high MW amphiphilic Sty-2VPy and one Sty-4VPy diblock copolymers were prepared via the combination of living anionic and RAFT polymerizations. First, living anionic polymerization was employed for the preparation of OH-functionalized homopolyStys, where their OH-terminal groups were converted to polySty macroRAFT CTAs by the attachment of a 4-CPeDB CTA group. The macroRAFT CTAs were, subsequently, extended with 2VPy or 4VPy using RAFT polymerization in the presence of AIBN as initiator. The MWs of the diblock copolymers ranged between 42,000 and 271,000 g mol–1, which are the highest reported to date for the particular combination of polymerization methods. Films cast from chloroform solutions of the diblock copolymers were investigated in terms of their bulk morphologies using TEM. Sty462-b-2VPy187 formed hexagonally packed cylinders of P2VPy in a PSty matrix, while Sty111-b-2VPy395, Sty2160-b-2VPy836, and Sty2160-b-4VPy424 formed Sty or VPy spheres, confirming that the minority block consistently formed the discontinuous spherical microphase. It is possible that one of the samples, Sty2160-b-2VPy836, did not self-assemble to the expected cylindrical morphology but formed spheres as a result of the increased polydispersity of its second block, in line with previous findings regarding the effect of size heterogeneity on microphase separation in the bulk.