Yunhua Lu*a,
Jianhua Zhanga,
Guoyong Xiaoa,
Lin Lib,
Mengjie Houb,
Junyi Hua and
Tonghua Wang*b
aSchool of Chemical Engineering, University of Science and Technology Liaoning, Anshan, Liaoning 114051, P. R. China. E-mail: lee.lyh@163.com; Fax: +86 412 5216702; Tel: +86 412 5929952
bSchool of Chemical Engineering, Dalian University of Technology, Dalian, Liaoning 116024, P. R. China. E-mail: wangth@dlut.edu.cn
First published on 5th May 2020
The diamine monomer, 9,9-bis[4-(4-amino-3-hydroxylphenoxy)phenyl] fluorene (bis-AHPPF) was successfully synthesized according to our modified method. A series of hydroxyl-containing poly(ether-imide)s (HPEIs) were prepared by polycondensation of the bis-AHPPF diamine with six kinds of dianhydrides, including 1,2,3,4-cyclobutanetetracarboxylic dianhydride (CBDA), pyromellitic dianhydride (PMDA), 3,3′,4,4′-biphenyl tetracarboxylic diandhydride (BPDA), 3,3′,4,4′-oxydiphthalic anhydride (ODPA), 3,3′,4,4′-benzophenonetetracarboxylic dianhydride (BTDA) and 4,4′-(hexafluoroisopropylidine)diphtalic anhydride (6FDA) followed by thermal imidization. The corresponding thermally rearranged (TR) membranes were obtained by solid state thermal treatment at high temperature under a nitrogen atmosphere. The chemical structure, and physical, thermal and mechanical properties of the HPEI precursors were characterized. The effects of heat treatment temperature and dianhydrides on the gas transport properties of the poly(ether-benzoxazole) (PEBO) membranes were also investigated. It was found that these HPEIs showed excellent thermal and mechanical properties. All the HPEI precursors underwent thermal conversion in a N2 atmosphere with low rearrangement temperatures. The gas permeabilities of the PEBO membranes increased with the increase of thermal treatment temperature. When HPEI–6FDA was treated at 450 °C for 1 h, the H2, CO2, O2 and N2 permeabilities of the membrane reached 239.6, 196.04, 46.41 and 9.25 Barrers coupled with a O2/N2 selectivity of 5.02 and a CO2/N2 selectivity of 21.19. In six TR-PEBOs, PEBO–6FDA exhibited the lowest rearrangement temperature and largest gas permeabilities. Therefore, thermally rearranged membranes from bis-AHPPF-based HPEIs are expected to be promising materials for gas separation.
In recent years, HPI, as the precursor of thermally rearranged (TR) polymers, has been widely concerned and investigated.15 After thermal rearrangement reaction in solid state at 350–450 °C, the benzoxazole structure from HPI was formed, accompanied by the emission of CO2. The obtained TR polymers are a kind of microporous polymer with high fractional free volume (FFV) and narrow cavity size distribution, resulting in high gas permeabilities and outstanding separation selectivities even beyond the 2008 Robeson limit.16–20 Hence, there is a strong incentive for development of new TR polymers with high gas permeability and selectivity. Currently, in order to synthesize TR polymers, two main steps are usually involved: (i) synthesis of HPI precursors using thermal, azeotropic or chemical imidization methods, and (ii) thermal conversion of the HPI precursors into polybenzoxazoles (PBOs) in solid state.21–24 Although the imidization methods usually lead to the final TR polymers with the same chemical structure, the physical and gas separation properties of the TR polymers were very different.25–29 Therefore, the structure and properties of TR polymers could be easily adjusted by molecular structure design and preparation methods to facilitate specific gas separation applications.30–35 According to the reported literatures,25–35 HPI is the most commonly used precursor for the preparation of TR polymers, and most of TR polymers are based on HPI precursors made from 4,4′-(hexafluoroisopropylidene)diphthalic anhydride (6FDA) and 2,2′-bis(3-amino-4-hydroxyphenyl)-hexafluoropropane (APAF) or 3,3′-dihydroxy-4,4′-diamino-biphenyl (HAB). Later, spiro, cardo and triptycene based TR polymers have also been reported in succession.35
Generally speaking, the monomers with rigid backbone, bulky bridging and pendant groups should be preferred to endow TR polymers with high FFV and gas permeabilities. However, the HPIs with rigid structures usually need a relatively higher thermal rearranged temperature (TTR), which is not cost-effective and poor mechanical properties in application. Furthermore, the low-TTR TR polymers containing very flexible backbone generally bring a higher rate of conversion and lower gas permeabilities.36 Therefore, the structure design and synthesis of TR polymers need to consider the balance between chain rigidity and flexibility, and the trade-off relationship between the production cost and the separation performance.
As reported, 9,9-bis(3-amino-4-hydroxyphenyl)fluorene (bisAHPF) is a kind of diamine with rigid and bulky fluorenyl cardo group, which has been used as the hydroxy-functional diamine to prepare the TR polymers.37–39 Cardo moiety with loop shaped structure in polymer main chains is useful to improve the FFV and gas permeabilities of polymeric membranes.40–44 Additionally, fluorenyl cardo group has a large steric hindrance, which is beneficial to restrict the tight stacking of macromolecular chains and increase chain rigidity, thermal properties and FFV. Unfortunately, HPIs from bisAHPF need a higher TTR temperature, resulting in poor mechanical properties as well as processability, so copolymerization with other diamine has been adopted to improve the properties of final TR materials.37–39
In the present study, we report the synthesis and gas transport properties of a series of poly(ether-benzoxazole) (PEBO) membrane prepared from hydroxyl-containing poly(ether-imide)s (HPEIs). The HPEIs were prepared by a polycondensation reaction between 9,9-bis[4-(4-amino-3-hydroxylphenoxy)phenyl]fluorene (bis-AHPPF) and six kinds of dianhydrides, followed by thermal imidization. After subsequently thermally treated in N2 atmosphere, the corresponding PEBOs were obtained for gas separation. Here, 9,9-bis[4-(4-amino-3-hydroxylphenoxy)phenyl]fluorene contains both flexible ether linkage and bulky cardo moiety, which is expected to endow HPEI moderate rigidity to decrease the TTR and maintain a higher gas permeabilities. Finally, the alteration of structure, physical properties as well as gas separation properties of HPEI and PEBO membranes were systematically characterized by numbers of proper analytic techniques. It is believed that this work would provide some valuable insights to design and prepare the gas separation membrane materials for energy development and environmental protection.
Dynamic mechanical properties of HPEIs were tested by DMA 8000 (Perkin Elmer, USA) from 50 to 400 °C at a rate of 10 °C min−1 with 1HZ in air and N2 atmosphere (80 mL min−1). Glass transition temperatures (Tg) of PEBOs were carried out using a Perkin Elmer Instruments DSC 4000 with a heating rate of 20 °C min−1 in nitrogen atmosphere. Two heating–cooling cycles from 50 °C to 400 °C were performed, and Tg was determined based on the second heating cycle. Thermogravimetric-mass spectrometry (TG-MS) was conducted on the Netzsch STA 449F3 (Germany) with a heating rate of 10 °C min−1 and a nitrogen purge of 50 mL min−1 to evaluate thermal stability characteristics as well as the thermal rearrangement, in the temperature range from room temperature to 900 °C.
The densities of HPEIs were measured by the Shimadzu MH-124S Densitometer (Japan). Density for each HPEI sample was measured for at least three times and the average value was used for the FFV calculation. FFV of each polymer was calculated based on the following eqn (1):
(1) |
Wide-angle X-ray diffraction (WAXD) patterns were recorded at room temperature (about 25 °C) by X'Pert Powder X-ray diffractometer (PANalytical, Almelo, Netherlands) to show the changes in intersegmental properties of these polymers. The 2θ value changed from 5° to 70° with copper Kɑ radiation (operating at 40 kV and 40 mA). The average d-spacing values of the HPEI and PEBO were calculated by means of Bragg's law using eqn (2):
nλ = 2dsinθ | (2) |
Mechanical properties (tensile strength, Young modulus, and elongation at break) of HPEI precursors were measured by using the HY-0580 stretching tester (Shanghai Hengyi Precision Instrument Co., Ltd., China) fitted with a 100 N load at room temperature. The samples of 1 cm width and 7 cm length were clamped at both ends with an initial gauge length of 5 cm, and the elongation rate was of 10 mm min−1.
Single gas permeation of PEBO membranes was tested by traditional variable volume-constant pressure method using high purity gases (>99.99%), i.e., H2 (2.89 Å), CO2 (3.3 Å), O2 (3.46 Å) and N2 (3.64 Å). The GC analysis was conducted by GC7890 (Techcomp Ltd.) equipped with a thermal conductivity detector (TCD) and a packed column. For each membrane, the measurements were under taken for more than three samples prepared under the same conditions. The reported permeation data are the averaged value with a measurement precision of 10%. For the details of the test procedure, please refer to our previous report.45 In the study, the feed pressure and testing temperature were maintained at 0.01 or 0.1 MPa and 30 °C, respectively. The gas permeabilities were determined from the eqn (3).
(3) |
αA/B = PA/PB | (4) |
The HPEIs were synthesized from the cardo diamine bis-AHPPF and six kinds of dianhydrides including CBDA, PMDA, BPDA, ODPA, BTDA and 6FDA via a two-step thermal imidization method. After that, most DMAc solvent was removed and the ring-closure reaction was partly completed. The HPEIs are readily prepared with flexible and good mechanical strengths for the further tests. The FTIR spectra for HPEIs, shown in Fig. 2, confirmed the imidization. All HPEIs exhibited the characteristic imide group absorptions at around 1779 and 1717 cm−1 for imide carbonyl symmetrical and asymmetrical stretching, approximately 1388 cm−1 for C–N stretching of imide ring, and around 743 cm−1 for C–N–C ring deformation. In addition, the characteristic broad peak of O–H group appeared at 3000–3600 cm−1. The band around at 1213 cm−1 was the asymmetrical stretching vibration of C–O bonds. The spectra have evidenced the existence of typical imide groups and other functional groups in the molecular structure of HPEI precursors.
Glass transition temperatures (Tg) of HPEIs are determined by DMA 8000 in air or N2, and Fig. 3(a) and (b) displays the tanδ–T curves of HPEIs. The temperature at which the maximum of loss tangent (tanδ) observed is commonly defined as the Tg value by DMA test, as shown in Table 1. As expected, with increasing rigidity of dianhydride monomer, the Tg values are shifted toward higher temperature region. The ether connecting group can increase the mobility of the macromolecular chains, while bulky fluorene moiety hinders the chain motion. Moreover, hydrogen bonding might further increase the interaction between molecular chains to limit the chain movement. As a result, the Tg values of HPEIs are almost above 300 °C. Furthermore, the HPEI–6FDA shows a higher Tg value compared with the reported HPEI (280 °C, DSC) from 6FDA and 2,2-bis(4-(4-amino-3-hydroxyphenoxy)phenyl)hexafluoropropane (6FBAHPP).36 It may be attributed to the stronger rigidity and larger volume of fluorene group than that of hexafluoroisopropyl group.
Samples | Tga (°C) | Td5b (°C) | Td10b (°C) | TTRc (°C) | R700d (%) | Tensile strength (MPa) | Young modulus (GPa) | Elongation at break (%) | |
---|---|---|---|---|---|---|---|---|---|
DMA | |||||||||
N2 | Air | ||||||||
a Tg: glass transition temperature measured by DMA.b Td5 and Td10: 5% and 10% weight loss temperatures in TGA at 10 °C min−1 heating rate under a nitrogen atmosphere, respectively.c TTR: thermal rearrangement temperature obtained from DTG–T curves at the maximum conversion rate.d R700: residual yield in TGA at 700 °C under a nitrogen atmosphere.e Not estimated in tanδ–T curves in N2. | |||||||||
HPEI–CBDA | —e | 330 | 274 | 356 | 372 | 59 | 126.9 ± 2.0 | 4.4 ± 0.2 | 3.6 ± 0.2 |
HPEI–PMDA | —e | 345 | 337 | 377 | 387 | 61 | 99.3 ± 4.0 | 3.8 ± 0.1 | 3.2 ± 0.1 |
HPEI–BPDA | 366 | 343 | 307 | 387 | 403 | 65 | 111.2 ± 3.0 | 4.1 ± 0.2 | 3.6 ± 0.1 |
HPEI–ODPA | 318 | 295 | 296 | 365 | 378 | 60 | 103.2 ± 3.0 | 3.7 ± 0.1 | 3.3 ± 0.3 |
HPEI–BTDA | 335 | 370 | 311 | 379 | 393 | 63 | 86.5 ± 4.0 | 4.5 ± 0.2 | 2.0 ± 0.1 |
HPEI–6FDA | 339 | 330 | 326 | 373 | 371 | 62 | 126.8 ± 3.0 | 3.7 ± 0.1 | 4.3 ± 0.2 |
Using DMA to study the HPEIs not only provides an alternative and accurate method for Tg (α relaxation, glass–rubber transition) measurement, but also offers some other information on thermal behavior. The β and γ relaxations corresponding to the subglass relaxation of the local mobility have been observed in Fig. 3(a) and (b). For HPEIs, because of the further thermal imidization reaction at 200–300 °C, and thermal rearrangement as well as crosslinking above 350 °C, the tanδ–T curves were complex. In Fig. 3(a), because of some small molecules produced by the thermal decomposition reaction, the tanδ peak moves slightly to the low temperature direction. However, the tanδ peak of HPEI–BTDA shifted to high temperature, indicating that the thermal crosslinking reaction took place. After the α relaxation peak of HPEI–ODPA, another lower tanδ loss peak appeared, which might mean that the thermal crosslinking in air reduced the mobility of molecular segments and increased the rigidity of the molecular chain. Due to the testing temperature of 50–400 °C, this phenomenon of other HPEIs is not fully displayed, only some trends can be seen. As shown in Fig. 3(b), thermal oxidation reaction is avoided as much as possible, so the tanδ–T curves measured under nitrogen condition are different from those measured in air. For HPEI–BPDA, HPEI–ODPA and HPEI–6FDA, the Tg values in N2 were higher than those obtained in air because of more complete imidization without oxidative decomposition. The Tg of HPEI–BTDA decreased from 370 °C to 335 °C due to no thermal oxidative crosslinking. Nevertheless, the largest tanδ loss peaks of HPEI–CBDA and HPEI–PMDA didn't appear until 400 °C, so their Tgs were not estimated.
The stress–strain curves of HPEI samples are illustrated in Fig. 4, and the corresponding data are given in Table 1. These HPEI samples showed excellent tensile strength and Young modulus. According to the shape of stress–strain curves, the HPEIs still exhibited the character of brittle materials with lower elongation at break and no yield point. The elongation of these HPEIs was relatively lower than some commercial PI films such as Kapton, although there were flexible ether bonds in the main chain of polymer. The reason may be that the steric resistance of fluorene group increased the rigidity of macromolecular chain and the membrane was not biaxially stretched. Among them, HPEI–CBDA and HPEI–6FDA showed higher tensile strength about 127 MPa, while HPEI–6FDA exhibited the biggest elongation with 4.3%. Excellent mechanical properties can ensure that they can withstand subsequent heat treatment and testing.
As we known, enhancing the fractional free volume (FFV) of polymer was proved to be beneficial to improving the gas permeability of membrane.4 Table 2 summarizes the densities and fractional free volumes (FFVs) of HPEIs. Although the thermal cyclization process was incomplete, we assumed that the imidization degree was 100% to compare the effect of repeat unit structure on FFV. The density data of the samples were measured, and the FFV was calculated from eqn (1). These HPEIs were expected to exhibit higher FFVs because the incorporation of the rigid and bulky cardo moiety into the polymer chain induced loose chain packing and led to an increase in the d-spacing. However, the introduction of ether linkages increased the flexibility of macromolecular chains and reduced the distance between molecular chains as well as FFV. As a result, the FFVs of these HPEIs were not very high. Comparatively, HPEI–6FDA showed the highest FFV due to the hexafluoroisopropyl group with steric hindrance effect.
Polymersa | Density (g cm−3) | Molar mass, M0b (g mol−1) | Molar volume, V0 (cm3 mol−1) | Van der Waals volume, Vw (cm3 mol−1) | Fractional free volume, FFVc | d-Spacing (nm) |
---|---|---|---|---|---|---|
a Thermally cyclized at 250 °C for 15 min.b Estimated by assuming 100% imidization conversion.c Fractional free volume of polymer membranes by Bondi method as in eqn (1). | ||||||
HPEI–CBDA | 1.2423 | 724 | 583.3 | 407.9 | 0.091 | 0.47 |
HPEI–PMDA | 1.3789 | 746 | 541.0 | 379.2 | 0.089 | 0.43 |
HPEI–BPDA | 1.3636 | 822 | 602.8 | 423.5 | 0.087 | 0.42 |
HPEI–ODPA | 1.3810 | 838 | 606.8 | 429.0 | 0.081 | 0.43 |
HPEI–BTDA | 1.3697 | 850 | 620.6 | 435.2 | 0.088 | 0.44 |
HPEI–6FDA | 1.2721 | 972 | 764.1 | 512.0 | 0.129 | 0.55 |
The thermal behavior and rearrangement mechanism of HPEI precursors were studied by TGA-MS in N2 atmosphere, and the Td and TTR observed from Fig. 6 was given in Table 1. As previously reported, the thermal rearrangement of hydroxyl-imide to benzoxazoles ring accompanied the evolution of carbon dioxide (2 mol CO2/HPEI repeating unit). All HPEIs in this study exhibited three weight losses, the first small mass loss around 280 °C was induced by thermal imidization; the second larger weight loss at the range of 325 to 450 °C, was caused by thermal conversion from HPEI to PEBO, where the amount of CO2 evolution reached the maximum value at about 400 °C as confirmed by MS.15 In this paper, the thermal rearranged temperature (TTR) of HPEIs was defined as the temperature at the maximum conversion rate for this polymer, which was closely related to the rigidity of the molecular chain. The TTR of HPEI–6FDA was about 371 °C, lower than that of most precursors, such as 452 °C of HPI(HAB–6FDA), 430 °C of HPI(APAF–6FDA) and 411 °C of HPI(6FBAHPP–6FDA)47 due to the synergistic effect of flexible linkage of –O– and large steric hindrance of fluorene moiety. The third distinct mass loss began at approximately 550 °C, which was caused by decomposition of the polymer backbone. Relatively, HPEI–CBDA showed the lowest thermal stability due to its semialiphatic ring structure although its TTR was 372 °C. In general, all precursors exhibited a high residual weight of 59–65% at 700 °C. These experimental results indicate that the HPEIs with fluorene cardo moieties have been converted to PEBO successfully.
The intersegmental distances of membranes were characterized by wide-angle X-ray diffraction (WAXD). The corresponding XRD patterns of HPEIs and PEBOs are shown in Fig. 7(a) and (b), and the d-spacing values of HPEIs are also listed in Table 2. Actually, the FFV is closely related to the chain packing. The d-spacing results are in agreement with the FFV data in some degree, indicating that the fluorenyl moiety could provide a larger FFV for the polymer precursors. Both HPEIs and PEBOs exhibited broad amorphous peaks, which indicated the amorphous nature of these polymers. From Fig. 7(a), the d-spacing value of HPEI–6FDA is higher than that of other HPEI precursors, which is attributed to the large steric hindrance of hexafluoroisopropyl group to limit the tight packing of molecular chains. In contrast, the d-spacings of PEBO–PMDA, PEBO–BPDA, PEBO–ODPA and PEBO–BTDA increased slightly after the thermal rearrangement process(in Fig. 7(b)). The d-spacing value of PEBO–6FDA increased from 0.55 nm to 0.61 nm, while the d-spacing value of PEBO–CBDA decreased from 0.47 nm to 0.44 nm because of the poor thermal stability of alicyclic structure resulting in the breaking of the macromolecular backbone and the tight intermolecular chains packing. Therefore, these d-spacings may provide an indicator of the amount of available space to penetrate small molecules.
The XPS analysis of PEBO–6FDA is given to illustrate to change of chemical structure, as shown in Fig. 8, which shows the presence of C, N, O and F in the polymer. The fitting curves of C, O and N suggest that the benzoxazole ring structures have been formed from HPEI. Fig. 8(b) shows that there is NC of benzoxazole ring at 287.2 eV. Moreover, according to literatures, 400.6 eV and 399.2 eV have been assigned to –N< in imide ring and –N in benzoxazole ring.37 According to Fig. 8(d), the two peaks at 400.4 eV and 399.1 eV indicate the PEBO–6FDA contain the imide group (–N<) and benzoxazole ring structure (–N). Based on the areas of XPS fitting peaks, the degree of conversion can be calculated about 45.2%, which illustrates that HPEI has been partially converted to PEBO. Hence, thermal treatment time and temperature need to be further adjusted in order to obtain high TR conversion rate and gas permeability.36,48
Fig. 8 XPS spectra of PEBO–6FDA (a)wide scan spectra; (b) fitting curves of C; (c) fitting curves of O; (d) fitting curves of N. |
The thermal properties of PEBOs are characterized and shown in Fig. 9. The Tg values were improved in varying degree and mainly around at 350 °C, while the effect of dianhydride structure on the Tg was very small. After high temperature treatment, thermal rearrangement of intramolecular and crosslinking of intermolecular could be induced, leading to the rigid molecular chain and strong interchain interaction accompanied with low segmental movement ability. The data indicated that these PEBOs exhibited good thermal properties and could be used in high temperature environment.
Samples | Gas permeabilitya/Barrerb | Ideal selectivityc | ||||
---|---|---|---|---|---|---|
H2 | O2 | N2 | CO2 | CO2/N2 | O2/N2 | |
a All permeation results were obtained at 30 °C and 0.1 MPa.b 1 Barrer = 10−10 cm3 (STP) cm cm−2 s−1 cmHg = 3.35 × 10−16 mol m m−2 s−1 Pa.c Ideal selectivities were obtained by the ratio of two gas permeabilities. | ||||||
HPEI–6FDA | 9.46 | 1.47 | 0.36 | 7.12 | 19.78 | 4.08 |
HPEI–6FDA-350 | 67.23 | 9.93 | 2.33 | 49.28 | 21.15 | 4.26 |
HPEI–6FDA-400 | 89.85 | 13.94 | 3.24 | 65.58 | 20.24 | 4.30 |
HPEI–6FDA-450 | 239.6 | 46.41 | 9.25 | 196.04 | 21.19 | 5.02 |
Samples | Permeabilitya/Barrerb | Ideal selectivityc | |||||
---|---|---|---|---|---|---|---|
H2 | O2 | N2 | CO2 | CO2/N2 | O2/N2 | H2/N2 | |
a All permeation results were obtained at 30 °C and 0.01 MPa.b 1 Barrer = 10−10 cm3 (STP)cm cm−2 s−1 cmHg = 3.35 × 10−16 mol m m−2 s−1 Pa.c Ideal selectivities were obtained by the ratio of two gas permeabilities. | |||||||
PEBO–CBDA | 65.08 | 11.53 | 2.33 | 55.64 | 23.88 | 4.95 | 27.9 |
PEBO–PMDA | 99.38 | 18.46 | 3.25 | 87.04 | 26.78 | 5.68 | 30.6 |
PEBO–BPDA | 116.72 | 21.82 | 5.07 | 107.88 | 21.28 | 4.30 | 23.0 |
PEBO–ODPA | 43.06 | 9.43 | 1.20 | 35.31 | 29.42 | 7.86 | 35.9 |
PEBO–BTDA | 78.49 | 16.47 | 2.35 | 68.38 | 29.10 | 7.01 | 33.4 |
PEBO–6FDA | 272.34 | 60.73 | 10.58 | 245.04 | 23.16 | 5.74 | 25.7 |
PEBO–6FDA-450 (ref. 36) | 95.3 | 10.0 | 1.89 | 41.4 | 21.9 | 5.3 | 50.4 |
PBO–6FDA-450 (ref. 37) | 371 | 54.2 | 11.8 | 255 | 21.6 | 4.6 | 31.4 |
PBO–TDA1-460 (ref. 28) | 1547 | 311 | 58 | 1328 | 22.9 | 5.4 | 27 |
PBO-co-PI-6FDA-450 (ref. 49) | 762 | 141 | 34 | 667 | 19.6 | 4.2 | 22 |
As previously described, gas transport properties of TR polymers strongly depended on the thermal treatment protocol. Four gas permeabilities of HPEI–6FDA increased with the increase of treatment temperature. When the treatment temperature was 450 °C, the H2, CO2, O2 and N2 permeabilities of PEBO–6FDA reached 239.6, 196.04, 46.41 and 9.25 Barrers, separately. Meanwhile the reasonable ideal selectivities CO2/N2 of 21.19 and O2/N2 of 5.02 make the TR a more attractive gas separation membrane. The significant increase in gas permeability was ascribed to a higher conversion rate of thermal rearrangement. Moreover, the permeabilities of four kinds of gases followed the order: H2 (2.89 Å) > CO2 (3.30 Å) > O2 (3.46 Å) > N2 (3.64 Å), which was in accordance to their kinetic diameters. Therefore, the thermal treatment protocol can significantly alter the gas separation performance of TR polymers.
According to the TG-MS results, the TTRs of HPEI precursors were mainly around 400 °C, so the degree of thermal rearrangement should be relatively high when the heat treatment temperature was set at 450 °C. As expected according to the XRD curves, PEBO–6FDA exhibited the largest d-spacing value among these PEBOs, mainly due to the steric hindrance structure of hexafluoroisopropane. Therefore, it is distinct that the gas permeabilities order was as follows: PEBO–6FDA > PEBO–BPDA > PEBO–PMDA > PEBO–BTDA > PEBO–CBDA > PEBO–ODPA. Furthermore, it could be noticed that for every TR polymer in this study, four gas permerbilities follows the order: H2 > CO2 > O2 > N2. By comparing the gas selectivities, it was found that the CO2/N2 and O2/N2 ideal selectivities of PEBO–BTDA and PEBO–ODPA were higher than other PEBOs, but their gas permeabilities were very low probably because of intermolecular crosslinking. Integrally, PEBO–6FDA displayed O2 permeability of 60.73 Barrer coupled with an O2/N2 selectivity of 5.74 and CO2 permeability of 245.04 Barrer with a CO2/N2 selectivity of 23.16. The gas permeation properties of PEBO–6FDA are compared to data of previously reported PEBO36 from 6FBAHPPF and 6FDA in Table 4. Clearly, the gas permeabilities and ideal selectivities of PEBO–6FDA from bis-AHPPF membrane were superior to 6FBAHPPF based PEBO. However, compared with some 6FDA-based and triptycene-based PBO without ether linkage,28,37,49 the PEBO–6FDA showed lower gas permeabilities and higher CO2/N2 and O2/N2. The results implied that the bis-AHPPF based PEBO–6FDA exhibited moderate molecular chain rigidity, which was conducive to the balance of gas permeability and selectivity.
In addition, the data in Table 3 were measured at 0.10 MPa, while those in Table 4 were measured at 0.01 MPa. The gas separation tests were conducted with the unsupported membranes. Considering the poor mechanical properties of PEBO membranes after heat treatment, in order to obtain the gas permeability data of six kinds of TR polymers as many as possible, no higher pressure was set. For PEBO–6FDA (450 °C) under 0.01 MPa test pressure, the gas permeabilities of H2, O2, N2 and CO2 increased by 13.7%, 99.7%, 14.4% and 25.0% separately compared to 0.1 MPa. Namely, the gas permeability reduced as the feed pressure increased. Moreover, the selectivities of CO2/N2 and O2/N2 were also improved because the increases of O2 and CO2 were greater than that of N2. This result is consistent with some literature reports.50–52 This can be rationalized by a decrease in gas solubility coefficient with pressure as is typically observed in glassy polymers due to their dual-mode sorption behavior.
An ideal gas separation membrane is expected to have both high permeability and high selectivity. As illustrated in Fig. 10, the O2/N2 separation performance of PEBOs still showed a trade-off relationship between gas permeability and ideal selectivity. Compared to the literatures,36,37,49 PEBO–ODPA, PEBO–BTDA and PEBO–6FDA were near or beyond the 2008 trade-off line. Especially, PEBO–6FDA exhibited much higher gas permeability for O2/N2 because of the bulky cardo and –(CF3)2– moiety in the TR polymer backbone. Therefore, the diamine bis-AHPPF is effective for lowing thermal rearrangement temperature and adjusting the gas permeability and selectivity, and the corresponding PEBO membranes are expected to be applied in the field of gas separation.
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