Yi Lin,
Toshikazu Sakaguchi* and
Tamotsu Hashimoto
Department of Materials Science and Engineering, Graduatde School of Engineering, University of Fukui, Bunkyo 3-9-1, Fukui 910-8507, Japan. E-mail: sakaguchi@matse.u-fukui.ac.jp
First published on 13th April 2020
Efficient gas-separation systems comprising gas-permeable membranes are important for energy conservation in various industrial applications. Herein, high-molecular-weight copolymers (2ab and 2ac) were synthesized in good yields by the copolymerization of 1-(p-trimethylsilyl)phenyl-2-(p-trimethylsilyl)phenylacetylene (1a) with 1-phenyl-2-(p-tert-butyl)phenylacetylene (1b) and 1-phenyl-2-(p-trimethylsilyl)phenylacetylene (1c) in various monomer feed ratios using TaCl5–n-Bu4Sn. Tough membranes were obtained by solution casting. The copolymers exhibited very high gas permeabilities (PO2: 1700–3400 barrers). Desilylation of 2ac membranes decreased the gas permeability, but desilylation of 2ab membranes resulted in a significant increase in the gas permeability. The highest oxygen permeability coefficient obtained was 9300 barrers, which was comparable to that of poly(1-trimethylsilyl-1-propyne), a polymer known to have the highest gas permeability.
In contrast, diarylacetylene polymers are tolerant toward pyrolysis and oxidation. Poly[1-phenyl-2-(p-trimethylsilyl)phenylacetylene] (PTMSDPA) and poly[1-phenyl-2-(p-tert-butyl)phenylacetylene] (PTBDPA) are the examples of diarylacetylene polymers, and show high PO2 values of up to 1000 barrers.9–12 Therefore, these polymers are promising materials for gas separation membranes. Hu et al. synthesized polymethylated indan-containing poly(diphenylacetylene), which is the most gas-permeable polymer ever recorded to date.13,14 Fukui et al. incorporated fluorenyl groups into poly(diarylacetylene) to improve gas permeability,15 and the highest PO2 value among fluorenyl-containing poly(diarylacetylene)s is 9800 barrers.16 The incorporation of naphthyl,17 SiMe3,5,6,18 tert-butyl,18,19 halogen20–22 into diarylacetylene is also often considered as a way to obtain high gas-permeable materials, but their gas permeability still lower than PTMSP.
In this study, the copolymerization of 1a with a tert-butyl-containing monomer (1b) and trimethylsilyl-containing monomer (1c) in various feed ratios was accomplished (Scheme 1). Free-standing membranes were fabricated from the resultant copolymers, and the desilylation of the membranes was performed using a mixture of trifluoroacetic acid/hexane. Gas permeabilities of the copolymer membranes were studied.
Our research group previously reported that the copolymers of TMSDPA and TBDPA showed higher gas permeabilities than those of the homopolymers, PTMSDPA and PTBDPA.18 Furthermore, the desilylation of the copolymer membranes enhanced the gas permeability. This suggested that some micro-scale voids were generated by the elimination of silyl groups. Therefore, the desilylation of the copolymers of 1-(p-trimethylsilyl)phenyl-2-(p-trimethylsilyl)phenylacetylene (1a), with two trimethylsilyl groups, is expected to further improve the gas permeability.
Gas permeability was measured using a Rikaseiki K-315-N gas permeability apparatus equipped with an MKS Baratron detector (MKS Instruments, Inc., Andover, Massachusetts, USA) at 25 °C. The downstream side of the membrane was evacuated at 0.2–1.0 Pa, while the upstream side was filled with a gas at approximately 1 atm (105 Pa). The increase in pressure in a downstream receiving vessel was measured. The permeability coefficient P expressed in barrers [1 barrer = 1 × 10−10 cm3 (STP) × cm/(cm2 × sec × cmHg)] was calculated from the slopes of the time–pressure curves in the steady state where Fick's law was obeyed. The diffusion coefficient (D) was determined by the time lag method using the following equation:
D = l2/6θ |
The density of membrane was determined by hydrostatic weighing using a Mettler Toledo balance (Mettler Toledo, Columbus, Ohio, USA) and a density determination kit. In this method, a liquid with a known density (ρ0) is required, and the membrane density (ρ) is obtained by the following equation:
ρ = ρ0 × MA/(MA − ML) |
Feed ratio | Copolymerb | |||
---|---|---|---|---|
(1a:1b or 1c) | Yield (%) | Mwc (g mol−1) | Mw/Mnc | |
a In toluene at 80 °C for 24 h; [1a] + [1b or 1c] = 0.20 M, [TaCl5] = 20 mM, [n-Bu4Sn] = 40 mM.b Methanol-insoluble product.c Measured by GPC (CHCl3). | ||||
1b | 1:4 | 91 | 902000 | 4.40 |
1:2 | 84 | 1260000 | 4.05 | |
1:1 | 81 | 546000 | 4.55 | |
2:1 | 73 | 820000 | 4.03 | |
4:1 | 71 | Insoluble | ||
1c | 1:4 | 87 | 1770000 | 3.57 |
1:2 | 81 | 2540000 | 2.13 | |
1:1 | 88 | 1350000 | 2.11 | |
2:1 | 90 | 872000 | 2.62 | |
4:1 | 80 | Insoluble |
The copolymerization of 1a with 1b in the feed ratio of 1:4 afforded the copolymer, 2ab(1:4), whose Mw was up to 902000. The copolymerizations of 1a with 1b in the feed ratios of 1:2, 1:1, 2:1, and 4:1 resulted in the production of copolymers, 2ab(1:2), 2ab(1:1), 2ab(2:1), and 2ab(4:1), respectively, in good yields. The molecular weights of 2ab(1:2), 2ab(1:1), and 2ab(2:1) were very high, but that of 2ab(4:1) could not be measured by GPC because 2ab(4:1) was insoluble in all solvents. The copolymerizations of 1a with 1c in the feed ratios of 1:4, 1:2, 1:1, and 2:1 under the same conditions afforded the copolymers [2ac(1:4), 2ac(1:2), 2ac(1:1), and 2ac(2:1), respectively] in high yields with high molecular weights (Mw = 872000–2540000). Similar to 2ab(4:1), the copolymer 2ac(4:1) was obtained in good yield, but the solubility was poor.
To verify the completion of the desilylation of copolymer membranes, IR measurements were carried out. The IR spectra of the membranes of 2ab(1:2), 2ac(1:2), and the desilylated analogues, 3ab(1:2) and 3ac(1:2), were shown in Fig. 1. The spectra of 2ab(1:2) and 2ac(1:2) showed the peaks at 1250 cm−1, assigned to the stretching of SiC–H bond, and 1120 cm−1 corresponding to the vibration of Si–C bond. No absorptions at 1250 cm−1 and 1120 cm−1 were observed in the spectra after desilylation (Fig. 1, 3ab and 3ac). The results suggest the completion of the desilylation reaction.
The solubilities of the copolymers were summarized in Table 2. Copolymers 2ab and 2ac showed the same solubility, and completely dissolved in relatively low polarity solvents such as toluene, chloroform, and tetrahydrofuran. However, 2ab(4:1) and 2ac(4:1) were insoluble in all solvents. Homopolymer of 1a is known to be insoluble in all solvents.23 Copolymers 2ab(4:1) and 2ac(4:1) mainly consist of the 1a component and therefore showed a similar solubility behavior as that of the homopolymer of 1a. Similar to 2ab, the desilylated polymer 3ab was soluble in low polarity solvents. However, 3ac was not soluble in any solvent. This variation in solubility before and after desilylation should come from the substituent of tert-butyl groups. Table 2 showed the substitution ratios for the phenyl groups. When the ratio was zero or more than 90%, copolymers were insoluble. Therefore, an appropriate ratio of substituents is necessary for the solubility of poly(diphenylacetylene).
Toluene | CHCl3 | THF | DMF | DMSO | Methanol | Substitution ratiob [%] | |
---|---|---|---|---|---|---|---|
a Symbols: (+) soluble, (±) partly soluble, (−) insoluble.b Ratio of the substituent (tert-butyl or SiMe3) for the phenyl groups on polymer side chain. | |||||||
2ab(1:4) | + | + | + | − | − | − | 60 |
2ab(1:2) | + | + | + | − | − | − | 67 |
2ab(1:1) | + | + | + | − | − | − | 75 |
2ab(2:1) | + | + | + | − | − | − | 83 |
2ab(4:1) | − | − | − | − | − | − | 90 |
2ac(1:4) | + | + | + | − | − | − | 60 |
2ac(1:2) | + | + | + | − | − | − | 67 |
2ac(1:1) | + | + | + | − | − | − | 75 |
2ac(2:1) | + | + | + | − | − | − | 83 |
2ac(4:1) | − | − | − | − | − | − | 90 |
3ab(1:4) | + | + | + | − | − | − | 40 |
3ab(1:2) | + | + | + | − | − | − | 33 |
3ab(1:1) | ± | + | + | − | − | − | 25 |
3ab(2:1) | − | ± | ± | − | − | − | 17 |
3ac(1:4) | − | − | − | − | − | − | 0 |
3ac(1:2) | − | − | − | − | − | − | 0 |
3ac(1:1) | − | − | − | − | − | − | 0 |
3ac(2:1) | − | − | − | − | − | − | 0 |
Membrane | Ratio | PO2a | PCO2a | PN2a | PO2/PN2 | PCO2/PN2 | Densityb |
---|---|---|---|---|---|---|---|
a Units: 1 × 10−10 cm3 (STP) × cm/(cm2 × sec × cmHg) (=1 barrer).b Determined by hydrostatic weighing; units: g cm−3. | |||||||
2ab | 1:4 | 2100 | 7830 | 1100 | 1.92 | 7.18 | 0.891 |
1:2 | 2900 | 10000 | 1550 | 1.87 | 6.44 | 0.854 | |
1:1 | 2200 | 8080 | 1130 | 1.94 | 7.13 | 0.884 | |
2:1 | 1700 | 6900 | 740 | 2.30 | 9.31 | 0.902 | |
2ac | 1:4 | 1800 | 6940 | 870 | 2.07 | 7.98 | 0.900 |
1:2 | 2700 | 9280 | 1470 | 1.83 | 6.31 | 0.866 | |
1:1 | 3000 | 10200 | 1610 | 1.86 | 6.35 | 0.858 | |
2:1 | 3400 | 10300 | 2060 | 1.65 | 5.00 | 0.787 | |
3ab | 1:4 | 6200 | 13000 | 4000 | 1.55 | 3.25 | 0.837 |
1:2 | 9300 | 18670 | 7500 | 1.24 | 2.49 | 0.757 | |
1:1 | 6600 | 13800 | 4800 | 1.38 | 2.88 | 0.812 | |
2:1 | 4400 | 10940 | 2990 | 1.47 | 3.66 | 0.848 | |
3ac | 1:4 | 980 | 4000 | 380 | 2.54 | 10.39 | 0.984 |
1:2 | 990 | 4100 | 390 | 2.54 | 10.51 | 0.972 | |
1:1 | 1070 | 4300 | 480 | 2.24 | 8.98 | 0.957 | |
2:1 | 1080 | 4500 | 490 | 2.21 | 9.20 | 0.951 | |
Poly(TMSDPA-co-TBDPA)18 | 1:1 | 2300 | 8300 | 1300 | 1.8 | 6.4 | |
DSpoly(TMSDPA-co-TBDPA)18 | 1:1 | 2700 | 8600 | 1600 | 1.7 | 5.4 | |
PTMSDPA12 | 1200 | 4900 | 560 | 2.1 | 8.7 | 0.91 | |
PTBDPA11 | 1100 | 4800 | 500 | 2.2 | 9.6 | ||
PTMSP12 | 9700 | 34000 | 6300 | 1.5 | 5.4 | 0.75 | |
Indan-polyacetylenes13,14 | 18700 | 44200 | 16600 | 1.13 | 2.66 | ||
Naphthyl-polyacetylenes17 | 4300 | 13000 | 2700 | 1.6 | 4.8 | ||
Flurenyl-polyacetylenes15,16 | 9800 | 24000 | 8100 | 1.2 | 3.0 | ||
Halogen-polyacetylenes20–22 | 5400 | 19000 | 3700 | 1.5 | 5.1 | 1.01 | |
PIM-1 (ref. 28) | 2270 | 13600 | 823 | 2.8 | 16.5 | 1.09 |
High gas permeabilities were observed for the membranes of 2ab and 2ac. The PO2 values of 2ab were in the range of 1700–2900 barrers, which were higher than that of PTBDPA (PO2: 1100 barrers). Copolymer 2ab(1:2) exhibited the highest gas permeability and its PO2 value was 2900 barrers, which was 2.6 times as that of PTBDPA. Similarly, 2ac showed a higher gas permeability than that of PTMSDPA. The PO2 values of 2ac were in the range of 1800–3400 barrers. The higher gas permeability of copolymers may be due to their asymmetrical structure of the repeating unit that generates micro-scale voids. It is obvious that incorporation of trimethylsilyl group or tert-butyl group into poly(diphenylacetylene)s in the way of copolymerization is effective to enhance the gas permeability.
The CO2 and N2 permeabilities of 2ab and 2ac were higher than those of PTBDPA and PTMSDPA, as well as the corresponding oxygen permeabilities. This suggests that the membranes of 2ab and 2ac have large free volumes. Accordingly, the membranes of 2ab and 2ac showed low densities of 0.787–0.902 g cm−3.
The desilylated membranes of 3ab exhibited significantly higher oxygen permeabilities than those of 2ab. The membrane density reduced upon desilylation. This indicates that the spaces occupied by the silyl groups were retained as micro-scale voids after desilylation due to the steric hindrance of tert-butyl groups. It is suggesting that the incorporation of tert-butyl groups prevents the chain packing effectively to enhance the gas permeability. Notably, 3ab(1:2) exhibited extremely high permeability and its PO2 value reached up to 9300 barrers, which was the highest value observed among all synthetic polymers. Contrary to 3ab, the desilylated membranes of 3ac showed lower gas permeabilities than those of the membranes of 2ac. The decrement of gas permeability through desilylation was due to the elimination of spherical bulky trimethylsilyl groups that caused the membrane to become dense. The PO2 values of 3ac were in the range of 980–1080 barrers. These were similar to the PO2 value of 900 barrers for poly(1-phenyl-2-phenylacetylene), which was formed by the desilylation of PTMSDPA.18 The densities of the membranes increased after desilylation. These results indicate that tert-butyl groups play an important role in the generation of micro-voids through membrane desilylation.
Interestingly, the PO2 values of 3ab were significantly higher than those of desilylated poly(TMSDPA–TBDPA) reported in our previous work,18 irrespective of the similarity in chemical structures (Fig. 2). For example, the PO2 of 3ab(1:1) was 6600 barrers, but the PO2 of desilylated poly(TMSDPA–TBDPA) (1:1) was 2700 barrers. The gas permeability increased as the amount of eliminated silyl group increased, when the desilylated polymer had tert-butyl groups.
The oxygen/nitrogen separation factors (PO2/PN2) for all the membranes before and after desilylation were in the range of 1.2–2.5, and the values tended to increase with a decrease in the PO2 value. These findings are consistent with the general observation that the highly gas-permeable polymers typically exhibit low gas separation abilities.
Table 3 showed the data of several gas-permeable polyacetylenes and PIM-1 [a typical polymer in polymers of intrinsic microporosity (PIMs)].28 PTMSP3 has been known as the most gas-permeable polymer, whose PO2 value is as high as 9700 barrers. Indan-based polyacetylenes13,14 show the highest gas permeability among all the existing polymers. The other polyacetylenes containing various aromatic rings also show high gas permeability. PIM-1 (ref. 28) is known to show high gas permeability (PO2 = 2270 barrers). Compared to these highly gas-permeable polymers, the desilylated membranes 3ab(1:2) comparably showed ultrahigh permeability.
Membrane | Ratio | DO2 × 107 | DCO2 × 107 | DN2 × 107 | SO2 × 103 | SCO2 × 103 | SN2 × 103 |
---|---|---|---|---|---|---|---|
a Determined by the “time lag” method at 25 °C; units: cm2 s−1.b Calculated using equation, S = P/D; units: cm3 (STP)/(cm3 × cmHg). | |||||||
2ab | 1:4 | 130 | 160 | 110 | 16.3 | 48 | 9.9 |
1:2 | 160 | 163 | 135 | 18.1 | 59 | 11.6 | |
1:1 | 135 | 160 | 118 | 16.1 | 48 | 9.6 | |
2:1 | 105 | 120 | 70 | 15.7 | 54 | 10.0 | |
2ac | 1:4 | 83 | 90 | 68 | 20.9 | 75 | 12.9 |
1:2 | 155 | 130 | 105 | 17.1 | 67 | 14.3 | |
1:1 | 165 | 140 | 115 | 17.9 | 73 | 14.3 | |
2:1 | 180 | 160 | 130 | 19.5 | 65 | 16.0 | |
3ab | 1:4 | 135 | 180 | 120 | 43.9 | 80 | 33.2 |
1:2 | 340 | 355 | 295 | 27.3 | 60 | 25.2 | |
1:1 | 170 | 180 | 140 | 35.3 | 81 | 33.2 | |
2:1 | 110 | 150 | 91 | 39.5 | 77 | 33.0 | |
3ac | 1:4 | 78 | 68 | 63 | 12.5 | 59 | 7.0 |
1:2 | 80 | 68 | 64 | 12.0 | 58 | 7.1 | |
1:1 | 87 | 70 | 65 | 12.3 | 60 | 7.3 | |
2:1 | 99 | 76 | 70 | 10.9 | 58 | 7.0 |
The membranes of 3ab showed higher gas diffusivity and gas solubility values than those of 2ab. The increase in diffusivity and solubility was due to the increase in the free volume of the membrane. Contrary to 3ab, the membranes of 3ac exhibited lower gas diffusivities and solubilities than those of 2ac. These behaviors were observed for all gases. If the membrane has an affinity to a specific gas, the variation in diffusivity and solubility for a specific gas is different from those for the other gases. Therefore, the changes in gas permeability through desilylation are probably due to the change in free volume rather than the affinity to a specific gas.
This journal is © The Royal Society of Chemistry 2020 |