Yu
Gu
,
Zongtao
Wang
,
Honghong
Gong
and
Mao
Chen
*
State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, Shanghai 200438, China. E-mail: chenmao@fudan.edu.cn
First published on 6th November 2020
Accessing well-defined ultra-high-molecular-weight (UHMW) polymers has long been one of the paramount challenges in polymer synthesis. Apart from the existing strategies, the CTA-differentiation-involving polymerization implemented facile generation of UHMW fluoropolymers with narrow polydispersities. Herein, aiming at achieving logical control of the differentiation process and accurate regulation of the molecular weight, we investigated the impact of different conditions and substrates on the reaction outputs. Moreover, the Mn effects on the thermal and mechanical performances of the derived materials were also examined. The results revealed that the obtained Mn can be easily directed upon alteration of the polymerization rate and the substrate structure (6.13 × 105–3.52 × 106 Da, Đ = 1.06–1.28), improving the efficiency and practicability of this approach for producing UHMW fluorinated materials to tailor for diverse applications.
However, the preparation of UHMW fluorinated polymers has rarely been implemented due to extra impediments of solubility and phase separation issues during fluorine-involving polymerizations,23–26 where the incorporation of C–F bonds can endow the corresponding materials with advantageous characteristics (super-hydrophobicity, low surface energy, excellent chemical resistance, etc.).25,27,28 Recently, our group developed the chain transfer agent (CTA)-differentiation-involving polymerization method29 based on the photo-controlled RDRP,30–44 which afforded a variety of UHMW fluoropolymers with low molecular weight distributions. Taking advantage of the spontaneous differentiation process of CTA driven by fluorous association, this dispersion polymerization can proceed at elevated Rp because of the heterogeneous nature with a high local monomer concentration. Meanwhile, the two differentiated CTA groups simultaneously meet the requirements of a high ratio of monomer to growing chain and the effective degenerative chain transfer process (high Rd), which overcame the mechanistic limitations in previous RDRPs.
Despite the robustness of the CTA-differentiation-involving polymerization in generating UHMW polymers, what remains uninvestigated is the effect of different reaction conditions and substrate species on the differentiation process, which plays a decisive role in determining the resulting molecular weights. Herein, we studied the impact of various factors (including feed ratios, light intensity and the length of the initial CTA) on the percentage of differentiation (POD) of CTA, providing guidance for the fine-tuning of the molecular weight as well as delivering mechanistic implications (Scheme 1). Furthermore, the influence of molecular weight on the thermal and mechanical properties of the UHMW fluoropolymers was also explored for the first time, promoting the bridging between synthesis and applications for this novel kind of material.
(1) |
Entry | Monomer | [M] (mol L−1) | [M]/[CTA]/[PC] | M nb (Da) | Đ | POD (%) |
---|---|---|---|---|---|---|
a All reactions were performed in 1.0 mL DMSO, PC = Ir(ppy)3. A 13 W white LED bulb (light intensity = 33 mW cm−2) was used as a light source. Irradiation times were controlled to reach full monomer conversion (0.5–3 h). b M n and Đ were determined by SEC measurements in DMF at 50 °C. | ||||||
1 | NFHMA | 0.25 | 50/1/0.1 | 6.72 × 105 | 1.18 | 2.49 |
2 | NFHMA | 0.50 | 100/1/0.1 | 1.18 × 106 | 1.25 | 2.83 |
3 | NFHMA | 0.75 | 150/1/0.1 | 1.56 × 106 | 1.06 | 3.20 |
4 | NFHMA | 1.00 | 200/1/0.1 | 1.79 × 106 | 1.18 | 3.72 |
5 | NFHMA | 0.50 | 300/1/0.3 | 2.38 × 106 | 1.18 | 4.19 |
6 | NFHMA | 0.50 | 200/1/0.2 | 1.82 × 106 | 1.08 | 3.66 |
7 | NFHMA | 0.50 | 50/1/0.05 | 6.86 × 105 | 1.20 | 2.44 |
8 | NFHMA | 0.50 | 100/1/0.4 | 8.45 × 105 | 1.32 | 3.95 |
9 | NFHMA | 0.50 | 100/1/0.2 | 9.80 × 105 | 1.16 | 3.41 |
10 | NFHMA | 0.50 | 100/1/0.05 | 1.60 × 106 | 1.08 | 2.08 |
11 | DDFHMA | 0.25 | 50/1/0.1 | 1.38 × 106 | 1.18 | 1.45 |
12 | DDFHMA | 0.50 | 100/1/0.1 | 1.70 × 106 | 1.09 | 2.36 |
13 | DDFHMA | 0.75 | 150/1/0.1 | 2.27 × 106 | 1.10 | 2.64 |
14 | DDFHMA | 1.00 | 200/1/0.1 | 2.36 × 106 | 1.12 | 3.40 |
15 | DDFHMA | 0.50 | 300/1/0.3 | 3.46 × 106 | 1.11 | 3.47 |
16 | DDFHMA | 0.50 | 200/1/0.2 | 2.87 × 106 | 1.11 | 2.79 |
17 | DDFHMA | 0.50 | 50/1/0.05 | 1.20 × 106 | 1.17 | 1.67 |
18 | DDFHMA | 0.50 | 100/1/0.4 | 1.13 × 106 | 1.11 | 3.56 |
19 | DDFHMA | 0.50 | 100/1/0.2 | 1.41 × 106 | 1.16 | 2.84 |
20 | DDFHMA | 0.50 | 100/1/0.05 | 2.01 × 106 | 1.07 | 2.00 |
We then investigated the effects of different reaction parameters on POD. As shown in Table 1 and Fig. 1b–d, for both monomers, the POD displayed positive relationships with the concentrations of monomer ([M]) and PC ([PC]), yet exhibited an inverse trend with the concentration of CTA ([CTA]) (Fig. 1c). This indicated a distinct condition-result correlation scenario where Mn is synergistically influenced by all the reaction components, which is different from a photo-induced electron transfer-reversible addition-fragmentation transfer (PET-RAFT) process.35 However, we noticed that this effect pattern is similar to the polymerization rate of PET-RAFT, which has been investigated and explained as eqn (2):45
(2) |
We hypothesized that, at the beginning of the reaction, a higher polymerization rate will raise the probability of the original CTA to be initiated and undergo monomer-addition, leading to a larger proportion of CTA evolving into the propagating species before the reaction gets into the equilibrium state (no monomer left in the solvent phase), exhibiting a higher POD. To validate this assumption, we conducted a series of reactions at a similar polymerization rate by keeping constant [M] and [PC]/[CTA] values according to eqn (2) (the impact of kt is negligible since kt ≪ kt,crossKRAFT[CTA]). The polymerization results are tabulated in Table 2, while the SEC curves showed no shoulder peaks for all the reactions (Fig. 2a and b), indicating excellent livingness of this approach. When [M] and [PC]/[CTA] were respectively fixed at 0.5 mol L−1 and 0.1, POD values stabilized at 2.80 for NFHMA and 2.40 for DDFHMA, resulting in linear relationships between the initial ratio of [M]/[CTA] and the obtained molecular weights (Fig. 2c), providing convenience for tailoring specific Mn values. Based on this evidence, we also attempted to extrapolate quantitative regression models correlating Mn with the reaction parameters with eqn (3):
(3) |
Fig. 2 (a) SEC curves for entries 1–4 in Table 2. (b) SEC curves for entries 5–8 in Table 2. (c) Linear relationships between Mn and the initial [M]/[CTA] values. (d) Linear regressions between the POD values and polymerization rates based on eqn (3). For NFHMA, POD = 7.56[M][CTA]−1/2[PC]1/2 + 1.65, goodness-of-fitting R2 = 0.84. For DDFHMA, POD = 8.46[M][CTA]−1/2[PC]1/2 + 0.88, goodness-of-fitting R2 = 0.95. For red dots, the monomer is NFHMA; for blue dots, the monomer is DDFHMA. |
Entry | Monomer | [M]/[CTA]/[PC] | M nb (Da) | Đ | POD (%) |
---|---|---|---|---|---|
a All reactions were performed in 1.0 mL DMSO, PC = Ir(ppy)3, [M] = 0.5 mol L−1. A 13 W white LED bulb (light intensity = 33 mW cm−2) was used as a light source. Irradiation times were controlled to reach full monomer conversion (0.5–3 h). b M n and Đ were determined by SEC measurements in DMF at 50 °C. | |||||
1 | NFHMA | 50/1/0.1 | 6.13 × 105 | 1.21 | 2.73 |
2 | NFHMA | 100/1/0.1 | 1.18 × 106 | 1.25 | 2.83 |
3 | NFHMA | 150/1/0.1 | 1.76 × 106 | 1.08 | 2.84 |
4 | NFHMA | 200/1/0.1 | 2.32 × 106 | 1.08 | 2.78 |
5 | DDFHMA | 50/1/0.1 | 8.43 × 105 | 1.27 | 2.39 |
6 | DDFHMA | 100/1/0.1 | 1.70 × 106 | 1.09 | 2.36 |
7 | DDFHMA | 150/1/0.1 | 2.47 × 106 | 1.11 | 2.43 |
8 | DDFHMA | 200/1/0.1 | 3.27 × 106 | 1.09 | 2.45 |
To further confirm the rate-dependence of the CTA-differentiation process, we next investigated the impact of light intensity, which has been acknowledged as an influential factor for the polymerization rate of PET-RAFT reaction.35 While other parameters were kept constant, different distances of the reaction mixture from the LED light bulb were employed to create various light intensities (0.52–33 mW cm−2). As displayed in Fig. 3a and b, at the same feed ratio of [M]/[CTA]/[PC] = 100/1/0.1, an enhanced light intensity resulted in a lower Mn, representing a higher POD. This trend is in correspondence with our recent research on the polymerization of pentafluorostyrene, where a weak light intensity was employed to fabricate large nanoparticles by generating less propagating chains compared with strong light.46
To further observe the dispersion polymerization process at different rates, we conducted kinetic experiments with NFHMA ([M]/[CTA]/[PC] = 200/1/0.2). As shown in Fig. 3c, the reaction proceeded with a two-stage regime when employing either a strong or weak light intensity. The evolvement of POD also follows a two-stage pattern where the values first increase and then remain steady under both conditions (Fig. 3d). Moreover, the stage transition points of POD and polymerization rate were in great correspondence (Fig. 3c and d, at 17 min and 30 min for reactions under strong and weak light, respectively). We believe that the first stage is the differentiation process which displayed a relatively low propagation rate, attributing to that the polymerization took place in both the solvent phase and the fluorous particles. When all monomers migrated into the particles, the polymerization site located entirely in the particles with higher local monomer concentrations, leading to elevated polymerization rates (the second stage in the kinetic curves). In contrast, the reaction under weak light irradiation underwent a longer differentiation process but ended with a lower POD, validating our assumption that a reduced polymerization rate would result in a less propagating chain.
After rationalization of the POD fluctuations under different conditions, we then investigated the influence of the PDMA length on the differentiation process in order to generate UHMW fluoropolymers with diverse block ranges. Since the CTA-differentiation involves in situ nucleation of fluorinated particles, we envisioned that the dispersion polymerization with a longer PDMA will require a longer time for CTA to reach enough fluorine incorporation to aggregate,47 extending the differentiation process. As shown in Table 3 and Fig. 4, when we employed PDMA of different lengths (Mn = 5.03 × 103–2.05 × 104 Da as determined by SEC measurements) as substituents on CTA, the polymerizations all generated UHMW polymers with narrow distributions (Đ < 1.28) (Fig. S16 and S17†), manifesting the robustness of the CTA-differentiation-involving polymerization. The resulted POD increased with the PDMA length under identical polymerization conditions ([M]/[CTA]/[PC] = 200/1/0.1) due to the extended differentiation period (Fig. 4a and b), which was also validated through kinetic experiments (Fig. 4c and d). Noticeably, the POD values for NFHMA were always higher than those for DDFHMA, which we believe is attributed to a faster assembly rate under a stronger fluorous interaction of the monomer with higher fluorine content. The above investigations evaluated the substrate-effect on the differentiation process, providing guidance for accessing well-defined UHMW fluoropolymers with versatile chemical compositions.
Fig. 4 M n and POD values obtained via polymerization from PDMA of different chain lengths. (a) Monomer = NFHMA. (b) Monomer = DDFHMA. All reactions were performed in 1.0 mL DMSO, PC = Ir(ppy)3, [M] = 0.5 mol L−1, [M]/[CTA]/[PC] = 100/1/0.1. A 13 W white LED bulb (light intensity = 33 mW cm−2) was used as a light source. (c) ln[M]0/[M]tvs irradiation time and (d) POD evolution plots for polymerizations of NFHMA from PDMA with different chain lengths with feed ratio = [M]/[CTA]/[PC] = 200/1/0.2. For red dots, Mn (PDMA) = 5.03 × 103 Da; for green dots, Mn (PDMA) = 1.58 × 104 Da. Note: the red plots in (c) and (d) are the same as the ones in Fig. 3c and d. |
Entry | Monomer | M n (PDMA)b (Da) | M nb (Da) | Đ | POD (%) |
---|---|---|---|---|---|
a All reactions were performed in 1.0 mL DMSO, PC = Ir(ppy)3, [M] = 0.5 mol L−1, [M]/[CTA]/[PC] = 200/1/0.1. A 13 W white LED bulb (light intensity = 33 mW cm−2) was used as a light source. Irradiation times were controlled to reach full monomer conversion (0.5–4 h). b M n (PDMA), Mn and Đ were determined by SEC measurements in DMF at 50 °C. | |||||
1 | NFHMA | 5.03 × 103 | 2.32 × 106 | 1.08 | 2.87 |
2 | NFHMA | 1.08 × 104 | 1.81 × 106 | 1.13 | 3.69 |
3 | NFHMA | 1.48 × 104 | 1.35 × 106 | 1.18 | 4.97 |
4 | NFHMA | 2.05 × 104 | 9.04 × 105 | 1.14 | 7.51 |
5 | DDFHMA | 5.03 × 103 | 3.27 × 106 | 1.09 | 2.45 |
6 | DDFHMA | 1.08 × 104 | 3.02 × 106 | 1.09 | 2.66 |
7 | DDFHMA | 1.48 × 104 | 1.77 × 106 | 1.12 | 4.56 |
8 | DDFHMA | 2.05 × 104 | 1.25 × 106 | 1.28 | 6.50 |
Finally, we probed the structure-property relationships of the UHMW fluoropolymers obtained from this approach to search for the potential applicability on materials design. Three poly(NFHMA) (PNFHMA) samples with varied molecular weights (PNFHMA-1, Mn = 6.72 × 105 Da, Đ = 1.18; PNFHMA-2, Mn = 1.88 × 106 Da, Đ = 1.12; PNFHMA-3, Mn = 3.20 × 106 Da, Đ = 1.09) prepared from the same CTA (PDMA with Mn = 5.03 × 104 Da) were selected and characterized for their thermal and mechanical performances. While the differential scanning calorimetry (DSC) measurements indicated similar Tg values for the three polymers (∼36 °C, Fig. 5a), a considerable difference in their mechanical performances on tensile test experiments was observed. As displayed in Fig. 5b, a polymer with the lowest Mn (PNFHMA-3) gave inferior tensile strength at 6.0 ± 0.2 MPa compared with the counterparts with higher Mn, while a further increase in Mn presented no improvements in the material's strength (tensile strength at 7.7 ± 0.3 and 7.9 ± 0.5 MPa for PNFHMA-1 and PNFHMA-2, respectively). Moreover, the highest elongation at break (254 ± 8%) of the UHMW fluoropolymers was afforded with medium Mn in the three samples, indicating that overhigh molecular weight will pose a negative effect on the toughness of the materials, which is caused by increased chain entanglements restraining chain straightening before break.48
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0py01366h |
This journal is © The Royal Society of Chemistry 2020 |