Open Access Article
Anhou Xu
*,
Quanxuan Lu,
Zhiyuan Huo,
Jiachen Ma,
Bing Geng,
Umair Azhar,
Luqing Zhang and
Shuxiang Zhang*
Shandong Provincial Key Laboratory of Fluorine Chemistry and Chemical Materials, School of Chemistry and Chemical Engineering, Shandong Engineering Research Center for Fluorinated Material, University of Jinan, Jinan 250022, China. E-mail: chm_xuah@ujn.edu.cn; fhxzhangsx@163.com
First published on 7th November 2017
A series of poly(dodecafluoroheptyl methacrylate)-b-poly(methyl methacrylate) (PDFMA-b-PMMA) diblock copolymer nanoparticles were prepared by reversible addition–fragmentation chain transfer (RAFT) dispersion polymerization of methyl methacrylate (MMA) in supercritical carbon dioxide. Nuclear Magnetic Resonance (NMR) and gel permeation chromatography (GPC) analysis confirmed an efficient and well-controlled block copolymerization. As the length of the PMMA block grows from the soluble PDFMA block it eventually becomes insoluble, which drives in situ polymerization-induced self-assembly (PISA). The influences of the length of CO2-philic PDFMA block, CO2-phobic PMMA block and polymerization pressure were investigated in this PISA process. Also spherical nano-objects were formed upon the synthesis of amphiphilic diblock copolymers in situ. It appeared that, as the length of CO2-philic block PDFMA was increased, there was a corresponding decrease in particle size and particle size polydispersity. Scanning electron microscope (SEM) images revealed that, during the microspheres formation, the greater degree of polymerization (DP) of MMA favoured well-controlled monodisperse microspheres.
Historically the self-assembly of block-selective solvents based amphiphilic block copolymers into nano-objects has been widely discussed, and this strategy is globally accepted to synthesize block copolymer nano-objects. These self-assembly processes have been achieved usually via two steps: (i) initial molecular dissolution of the copolymer chains and (ii) reduction of the solvency for one of the blocks to drive microphase separation. In principle, such self-assembled species are generated by the post-polymerization processing of mostly amphiphilic diblock copolymers using either a solvent or pH switch, dialysis, or thin film rehydration.7,8 Such protocols are typically performed at very low copolymer concentrations (≤1 wt% is common).9
Recently, polymerization-induced self-assembly (PISA) has enabled the preparation of block copolymer nano-objects with relatively high block copolymer concentration (10–30 wt%) based on either emulsion RAFT polymerization or dispersion RAFT polymerization.10–14 By following the PISA strategy, a solvophilic macro-RAFT agent-mediated RAFT polymerization under emulsion or dispersion conditions was performed, and highly concentrated block copolymer nano-objects were obtained through a one pot synthesis.15,16
Supercritical carbon dioxide (scCO2) is an attractive alternative to conventional solvents as a “green” solvent that is readily available, non-flammable, and possesses tunable solvent properties via pressure variation. Most polymers are insoluble in scCO2, while the majority of vinyl monomers tend to be soluble, and hence, scCO2 is a suitable medium for dispersion polymerizations. The use of scCO2 as medium in radical dispersion polymerizations was pioneered by DeSimone and co-workers,17 and also explored as medium for synthesis of block copolymer with RAFT polymerization as reviewed by Zetterlund and Howdle.18,19 Most attractive features of that process of block copolymer synthesis in scCO2 dispersion are good efficiency, simplicity and solvent-free synthesis of high-purity block copolymers in a one-pot, solvent-free synthesis. In addition, high blocking efficiencies can be achieved even at high conversion and high molecular weight.20
A number of groups have examined the general PISA approach for the preparation of soft matter nanoparticles of variable morphology in a range of mediums including polar (alcohols and water most commonly)13,21,22 and non-polar (typically alkanes) solvents.23,24 However, attempts to synthesize polymeric particles in scCO2 are few.3,25–27 A RAFT dispersion polymerization of MMA stabilized with poly(1H,1H,2H,2H-perfluorooctyl methacrylate) macro-RAFT in scCO2 along with the formation of micrometer-size spherical particles has been reported. But the size distribution of polymeric particles was not uniform and ranged between 1 and 6 μm.26 However, to the best of our knowledge, no monodispersed nano-sized spherical particles were obtained through this process. In this study, fluorinated block copolymers nanoparticles were synthesized by PISA in scCO2 using poly(dodecafluoroheptyl methacrylate-cumyldithiobenzoate) (PDFMA–CDB) macro-RAFT agent as the CO2-philic stabilizer. A series of PDFMA–CDB macro-RAFT agents and PDFMA-b-PMMA diblock copolymers with various lengths of PDFMA and PMMA blocks were synthesized via RAFT technique.
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| Scheme 1 Synthetic procedures of the fluorinated macro-RAFT agent PDFMA–CDB and PDFMA-b-MMA diblock copolymers. | ||
The chemical compositions of the fluorinated macro-RAFT agents and PDFMA-b-PMMA diblock copolymers were confirmed by 1H NMR spectra. Fig. 1 exhibits 1H NMR spectra of fluorinated macro-RAFT (Fig. 1A) and PDFMA32-b-MMA341 diblock copolymer (Fig. 1B). It can be seen in Fig. 1A, the signals at 7.10–7.94 ppm are characteristic of the two aromatic ortho to the dithio group, indicating that the RAFT agent moiety remains at the end of the polymer.28,29 The signals at 4.52–4.99 ppm are due to the –O–CH2–Rf group of DFMA; and signals at 5.94–6.35 ppm can be assigned to the –CHF– and –CH(CF3)2– groups. The absorption peaks at about 1.94 and 1.10 ppm are ascribed to –CH2– repeated units in backbone and –C–CH3 pendant group in DFMA units.30 By comparison with Fig. 1A, clearly, the emergent signals at 3.49–3.74 ppm in Fig. 1B are designated to the –O–CH3 group of MMA units,31 which suggested that the PMMA segments were coupled with PDFMA segments and the block copolymer was achieved.
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| Fig. 1 1H NMR spectrum for (A) the fluorinated macro-RAFT PDFMA32–CDB (Table 1, entry 2) and (B) diblock copolymer PDFMA32-b-PMMA341 (Table 2, entry 6). | ||
The time dependence of DFMA conversion and ln([M]0/[M]) of the polymerization under different DFMA/CDB ratios are shown in Fig. S1.† The conversion of DFMA increased smoothly with the increase of polymerization time while increased much slightly with the increase of DFMA monomer concentration (or the increase of DFMA to CDB ratio), as shown in Fig. S1(A).† As a result, almost identical DFMA conversion was obtained at the same polymerization time (as shown in Table 1), though the DFMA to CDB ratios distinctly varied. Moreover, it is found that the time dependence of ln([M]0/[M]) in the polymerization was nearly linear at investigated DFMA to CDB ratios, especially when the polymerization time was less than 8 hours [shown in Fig. S1(B)†], indicates that a living/controlled radical polymerization of DFMA was achieved in the presence of CDB.
| Entry | DFMA/CDB/AIBN composition (mol% in feed) | Conv.b (%) | Mn,thc | Mn,GPCd | Mn,NMRe | PDI | DPf | Cloud point (MPa) | Sample name |
|---|---|---|---|---|---|---|---|---|---|
| a The reaction temperature and time are 70 °C and 8 h respectively for all experiments.b The conversion was calculated by the weight method.c Determined by the formula: Mn,th = ([DFMA]0/[CDB]0) × MDFMA + MCDB.d Gel permeation chromatography (GPC) in THF with PS standards.e Calculated by the following equation: Mn,NMR = 5 × (I4.31–4.96/I7.10–7.95) × MDFMA + MCDB.f The degree of polymerization (DP) for each polymer was calculated by the 1H NMR spectrum. | |||||||||
| 1 | 10/1/0.25 | 85.7 | 3700 | 5100 | 6200 | 1.07 | 15 | 7.9 | PDFMA15–CDB |
| 2 | 30/1/0.25 | 88.3 | 10 900 |
9900 | 13 100 |
1.11 | 32 | 8.4 | PDFMA32–CDB |
| 3 | 50/1/0.25 | 88.9 | 17 600 |
11 000 |
22 000 |
1.12 | 55 | 8.9 | PDFMA55–CDB |
In order to investigate the influence of the CO2-philic units, i.e., PDFMA units on the PISA behaviour of the block copolymer PDFMA-b-PMMA, fluorinated macro-RAFT agents with different chain lengths were prepared. All the data are listed in Table 1, and the narrow polydispersity indexes (PDI) as shown in Table 1 and Fig. S2† indicate that the polymerizations bear living radical polymerization characteristics. Two methods were used to estimate copolymer molecular weights (Mn): NMR (Mn,NMR) and GPC (Mn,GPC). The Mn,NMR of PDFMA was calculated from the integration areas of CH2 absorptions [–O–CH2–Rf (4.52–4.99 ppm)] of DFMA and that of the aromatic protons (7.10–7.94 ppm) of CDB in the 1H NMR spectrum. Mn,GPC were consistently lower than those calculated by NMR. The difference Mn,GPC and Mn,NMR (especially entry 3), might be due to the inadequate solubility of these fluorinated macro-RAFTs in THF or due to the different molecular structure of these prepared fluoropolymers with standard samples of PS in GPC. By giving the inadequacy of GPC for these calculations, NMR was determined to be the best estimate of the degree of polymerization (DP) for each PDFMA–CDB homopolymer was calculated by Mn,NMR.
One of the most important features of the RAFT process is its ability to reinitiate the polymer chain to continue propagation in the presence of a second monomer, hence the capacity to produce a range of block copolymers increases. A series of PDFMA-b-PMMA diblock copolymers were subsequently prepared by using the synthesized fluorinated macro-RAFT agents in scCO2, the results of which are summarized in Table 2. Analysis on the GPC after chain extension shows unimodal systems for the diblock copolymers PDFMA-b-PMMA with the loss of the peak for PDFMA–CDB samples, which shows that the fluorinated macro-RAFT PDFMA–CDB effectively acted as a macro chain transfer agent. All the reactions were completed after 24 h. Monomer conversion (MMA) was nearly quantitative. Additionally, unimodal GPC chromatograms smoothly shifted towards the higher molecular weight side with increasing DP of the second block PMMA with no trace from unreacted macro-RAFT or bimolecular termination (Fig. 2, S3 and S4†). Importantly, these chain extended species, i.e., diblock copolymers PDFMA-b-PMMA showed relatively narrow PDIs (<1.5) and reasonable agreement with the theoretical molecular weight (Mn,th). The results of all characterizations confirmed the successful synthesis of the PDFMA-b-PMMA diblock copolymers in scCO2 (as shown in Table 2).
| Entry | Monomer/macro-RAFT composition (mol% in feed) | Yield % | Mn,thb | Mnc | PDI | DPd | Physical statee | Dnf | Dw/Dng | Sample name |
|---|---|---|---|---|---|---|---|---|---|---|
a Reactions performed with [MMA] = 0.8 M, [PDFMA–CDB] : [AIBN] = 2 : 1, in 50 ml high-pressure autoclave at 70 °C and 30 MPa for 24 h.b Mn,th = (([MMA]0)/[PDFMA–CDB]0) × MMMA + MPDFMA–CDB.c Gel permeation chromatography (GPC) in tetrahydrofuran with PS standards.d The degree of polymerization (DP) for each polymer was calculated by the GPC. The degree of polymerization of the second block PMMA, DPnPMMA were determined by using the following formula: DPn = [(Mn of diblock copolymer PDFMA-b-PMMA − Mn,NMR of PDFMA–CDB)/molecular weight of MMA monomer].e Based on the visual observations made immediately after the recovery of the polymers from the reactor, SB = solid block, WP = white powder.f Dn = particle size.g Dw/Dn = size distribution. n.a.: not applicable. |
||||||||||
| 1 | MMA/PDFMA15–CDB = 100/1 | 96 | 16 272 |
16 000 |
1.09 | 98 | SB | n.a. | n.a. | PDFMA15-b-PMMA98 |
| 2 | MMA/PDFMA15–CDB = 300/1 | 98 | 36 272 |
41 400 |
1.29 | 351 | SB and WP | n.a. | n.a. | PDFMA15-b-PMMA351 |
| 3 | MMA/PDFMA15–CDB = 500/1 | 99 | 56 272 |
59 500 |
1.42 | 533 | WP | 259 | 1.23 | PDFMA15-b-PMMA533 |
| 4 | MMA/PDFMA15–CDB = 700/1 | 99 | 76 272 |
74 200 |
1.41 | 680 | WP | 171 | 1.10 | PDFMA15-b-PMMA680 |
| 5 | MMA/PDFMA32–CDB = 92/1 | 98 | 22 272 |
23 500 |
1.21 | 112 | SB and WP | n.a. | n.a. | PDFMA32-b-PMMA112 |
| 6 | MMA/PDFMA32–CDB = 292/1 | 99 | 42 272 |
46 400 |
1.32 | 341 | WP | 165 | 1.22 | PDFMA32-b-PMMA341 |
| 7 | MMA/PDFMA32–CDB = 492/1 | 100 | 62 272 |
66 800 |
1.48 | 545 | WP | 152 | 1.14 | PDFMA32-b-PMMA545 |
| 8 | MMA/PDFMA32–CDB = 702/1 | 100 | 82 272 |
89 700 |
1.26 | 774 | WP | 153 | 1.06 | PDFMA32-b-PMMA774 |
| 9 | MMA/PDFMA55–CDB = 100/1 | 98 | 32 272 |
31 400 |
1.23 | 91 | SB and WP | n.a. | n.a. | PDFMA55-b-PMMA91 |
| 10 | MMA/PDFMA55–CDB = 300/1 | 99 | 52 272 |
58 800 |
1.42 | 365 | WP | n.a. | n.a. | PDFMA55-b-PMMA365 |
| 11 | MMA/PDFMA55–CDB = 500/1 | 99 | 72 272 |
71 500 |
1.43 | 493 | WP | 81 | 1.09 | PDFMA55-b-PMMA493 |
| 12 | MMA/PDFMA55–CDB = 700/1 | 100 | 92 272 |
108 500 |
1.33 | 862 | WP | 102 | 1.08 | PDFMA55-b-PMMA862 |
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| Fig. 2 GPC traces of the PDFMA32–CDB homopolymer (Table 1, entry 2) and PDFMA32-b-PMMAn diblock copolymers. | ||
:5000
:1 was carried out in scCO2 at 70 °C and 30 MPa (Table 2, entry 1), a clear transition of polymerization solution from transparent to opaque were observed due to formation of aggregates. The aggregates were spherical particles with PMMA core and PDFMA corona (Scheme 2), due to the soluble nature of PDFMA in scCO2 while PMMA remained insoluble. Fluorinated PDFMA-b-PMMA copolymer particles having uniform particle diameters ranged from about 80 nm to 300 nm were prepared by tuning the length of CO2-philic PDFMA block, CO2-phobic PMMA block and polymerization pressure. Nanoparticle structures have been previously observed upon changing the relative mass fraction of the constituent blocks.3 The length of CO2-philic fluorinated macro-RAFT agent, mass fraction of the constituent blocks and selective CO2 solvent have also strongly influence on these segregation behavior of block copolymer phase, resulting in nano-sized particle morphologies that are different from those observed for micro-sized polymer particles formed in conventional dispersion polymerization in scCO2.3,25,27
According to the literature,33,34 fluorinated polymers exhibit high solubility (>10 wt%) at 25–65 °C under 35 MPa, such as polyfluoroacrylates or polyfluoroethers. On the contrary, other hydrocarbon-based polymers except some poly(propylene oxide) (PPO)-based oligomers or poly(ethylene oxide) (PEO)-based oligomers show solubility lower than 0.1 wt% (or completely insoluble) even at the molecular weight as low as 1700, such as polystyrene, poly(methyl methacrylate), etc. In this study, the solubility of fluorinated macro-RAFT agents and diblock copolymers was measured in CO2 at temperatures of 70 °C and pressures ranged from 7.5 to 35 MPa. As shown in Table 1, for fluorinated macro-RAFT agents, PDFMAn–CDB, the cloud point pressures are in range of 7–9 MPa and it shows that these fluorinated homopolymers have good solubility in scCO2. Though, fluorinated macro-RAFT agents are extremely soluble in scCO2, PDFMA-b-PMMA diblock copolymers become insoluble with the increasing length of PMMA block. The cloud point pressures of PDFMA-b-PMMA diblock copolymers with different block lengths were determined in scCO2 at 70 °C. Only three diblock copolymers with short PMMA block length, PDFMA15-b-PMMA98, PDFMA32-b-PMMA112, and PDFMA55-b-PMMA91 gave cloud point pressure values of 28, 33 and 29 MPa, respectively, other diblock copolymers did not dissolve completely in scCO2 at 70 °C even up to 35 MPa.
Scanning electron microscope (SEM) images also reveal that, during the microspheres formation, the greater DP of MMA block would favours in the formation of monodispersive polymer nanoparticles (as shown in Fig. 3, S5 and S6†). At short PMMA block lengths, copolymer PDFMA-b-PMMA can be dissolved in scCO2, thus gives to solid block products. As shown in Fig. 3A, the resultant copolymers are constituted by irregularly schistose conglomeration. By increasing the core-forming PMMA block length, PDFMA-b-PMMA copolymers became undissolved, leading to phase segregation of the incompatible blocks which resulted in more block chains aggregation and some spherical aggregates (Fig. 3B). When the chain length was much higher than the point at which phase change occurred, aggregation of the PMMA blocks induced the formation of spherical aggregates and the SEM image in Fig. 3C and D demonstrates the formation of the spherical aggregates, which was consistent with previous results reported.35 But there was an apparent lack of morphology transition in previous reports,13,23 where a range of nanoparticles with the sphere to worm to vesicle order–order transitions were observed with increasing the length of solvophobic block for a fixed solvophilic block. Such difference might be ascribed to the high miscibility of the PDFMA and PMMA blocks in scCO2. Enhancement of miscibility between poorly compatible polymers is a well-known phenomenon for blends formation in scCO2.36
As the length of CO2-philic block PDFMA was increased, there was a corresponding decrease in particle size. The morphology change with increasing DP of the fluorinated macro-RAFT was evidenced by SEM as shown in Fig. 4. The particles, though retained narrow particle size distributions, showed decrease in diameter from 259 to 81 nm when the DP of CO2-philic block PDFMA increased from 15 to 55. The stabilizer with the longer fluorinated block also led to a narrow particle size polydispersity (Dw/Dn), which ranged from 1.23 to 1.09 for the PDFMA block with DP of 15 and 55, respectively. This is in agreement with studies involving the synthesis of cross-linked polymer microspheres in scCO2, where it was found that surfactants with longer fluorinated blocks tended to give rise to better particle size control.35 These results are also in accord with findings in conventional liquid solvents, where an increase in molecular weight of the polymeric dispersant increases the viscosity of the continuous phase and leads to a more efficient dispersion polymerisation.37 This provides better stabilization due to higher equilibrium amounts of stabilizer and a thicker layer of stabiliser on the particle surfaces.
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| Fig. 5 SEM images of PDFMA-b-PMMA block nanoparticles prepared in scCO2 at different polymerization pressure. Reactions performed with [MMA] = 0.8 M, MMA/PDFMA32–CDB/AIBN = 692/1/0.5 (mol% in feed) at 70 °C for 24 h. (A) 10 MPa (B) 20 MPa, (C) 30 MPa (entry 8 in Table 1). | ||
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra08202a |
| This journal is © The Royal Society of Chemistry 2017 |