Taigyu
Joo
a,
Katherine
Mizrahi Rodriguez
b,
Hyunhee
Lee
a,
Durga
Acharya
c,
Cara M.
Doherty
c and
Zachary P.
Smith
*a
aDepartment of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA. E-mail: zpsmith@mit.edu
bDepartment of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA
cThe Commonwealth Scientific and Industrial Research Organization (CSIRO) Manufacturing, Private Bag 10, Clayton South 3169, Victoria, Australia
First published on 26th June 2023
Physical aging is a slow structural relaxation process characteristic of glassy polymers that results in reduced membrane permeabilities. In this study, PIM-1, the archetypal polymer of intrinsic microporosity (PIM), was post-synthetically modified to introduce components that are known to influence physical aging, such as hydrogen bonds and crosslinks. The effects of physical aging were monitored by permeation and sorption experiments, and structural changes were examined by positron annihilation lifetime spectroscopy (PALS) and other characterization techniques. The results suggest that higher initial fractional free volume is the primary factor contributing to higher rates of physical aging and that the introduction of hydrogen bonds and crosslinks reduces the initial free volume of PIM-1. In contrast, structural factors such as hydrogen bonds and crosslinks were the key factors in determining how permselectivity changed with physical aging. This study provides useful structure–property correlations and design principles related to free volume, hydrogen bonds, and crosslinks on physical aging behavior of microporous polymer membranes.
A major thrust of gas separation membrane research in the last four decades has been the development of new polymeric materials.4 Along these lines, membrane performance is evaluated based on the permeability and selectivity of the polymer, and the Robeson upper bound plots, a comprehensive database of polymers tested for gas separation, are commonly used in the field to assess state-of-the-art performance.8–10 Based on Freeman's theory, the overall separation performance of polymeric materials can be improved by increasing backbone stiffness while simultaneously increasing free volume, and such features are the defining characteristics of polymers of intrinsic microporosity (PIMs).11,12 When this type of polymer is cast from solution, polymer chains pack inefficiently to generate some of the highest free volume structures known within the field of gas separation membranes.13
PIMs are attractive materials in the gas separation field because their micropores allow for high gas sorption capacity while their rigid backbone structures hinder diffusion of larger gas penetrants, making them highly diffusion-selective materials especially when considering their high free volume.14 As a result, PIMs typically have orders-of-magnitude higher permeabilities than conventional polymers that are deployed as commercial gas separation membranes.15,16 Ever since the first reports of the PIM concept,17,18 new categories of these materials have been emerging at a rapid pace (e.g., triptycene, Tröger's base, ROMP, and CANAL-based polymers),19–22 along with new functionalizations (e.g., carboxylic acid, amine, and thioamide),23,24 post-synthetic modifications (e.g., crosslinking, thermal rearrangement, and pyrolysis),25–29 and mixed-matrix concepts (e.g., incorporating nanoparticles, MOFs, GO, CNTs, and PAFs).30–35 PIMs show promise because many compositions surpass the Robeson upper bound, yet they have never been deployed in large-scale industrial settings, in part due to challenges with scaling and stability, including phenomena such as plasticization and physical aging.4,13,36,37
Of the two major stability issues, this paper focuses on physical aging behavior of PIMs. Physical aging is the long timescale structural relaxation process of glassy polymers moving towards an equilibrium state that results in changes in membrane property sets over time. This phenomenon is ubiquitous among all glassy materials.38 Mechanistically, kinetically trapped conformations of polymer segments gradually relax towards equilibrium packing structures, thereby reducing the free volume of the polymer.38 Physical aging obeys an exponential relationship between permeability and free volume, and hence, physical aging has the most pronounced effect on permeability right after a polymer is formed into a film;39 however, this process persists throughout the lifetime of a polymer membrane used in the field and results in membranes “aging out”, requiring operators to discard and replace membrane modules.37 Because stable long-term performance is an important factor in commercial operations, more work is required to understand the underlying mechanisms of this phenomenon.
Some of the seminal studies on physical aging demonstrated that this feature is dependent on the amount of excess free volume and segmental mobility.40,41 Generally, polymers with high free volume are expected to age faster since the amount of excess free volume is the driving force for physical aging,42 while polymers with high glass transition temperatures (Tgs) are considered to be more resistant to physical aging since Tg is correlated with chain mobility.38,43,44 For this reason, various crosslinking methods have been studied to mitigate physical aging by intentionally reducing free volume and forming a network of interchain connections that provide rigidity within the polymer matrix.45–47 In this sense, PIMs have the dual attributes of low segmental mobility and high free volume, the former of which is expected to retard physical aging and the latter of which is expected to accelerate it.
Early PIM research anticipated that these polymers would have high physical aging resistance since PIMs generally lack a detectable Tg by standard techniques and contain permanent micropores arising from their backbone configurations (i.e., configurational free volume) that are theoretically unaffected by physical aging.48,49 In terms of Tg, we note that a study using fast scanning calorimetry has determined a Tg of 715 K for PIM-1, which surpasses its degradation temperature of 673 K in an inert atmosphere.50 However, multiple studies have shown that PIMs exhibit physical aging behavior that is often atypical of traditional polymers. For example, Swaidan et al. observed that TPIM-1, a triptycene-based ladder polymer, aged faster and more extensively than PIM-1, although the backbone of TPIM-1 has fewer flexible dioxane moieties and contains triptycene units that incorporate configurational free volume.48 Recently, Lai et al. reported a stark difference in the aging behavior of two different catalytic arene-norbornene annulation (CANAL) polymers, which are microporous polymers consisting of conformationally restricted fused rings.51 The CANAL polymer with 2D contortions showed a slight gain in selectivity and a larger decrease in permeability with time, while the CANAL polymer with 3D contortions showed a high gain in selectivity and a small decrease in permeability with time.51 The results from such studies suggest that the physical aging characteristics that are accepted for conventional polymers do not always translate to the emerging PIM subclass. Therefore, systematic studies of physical aging in PIM materials are required to glean insights into this important yet poorly understood phenomenon.
Recently, our lab demonstrated a solid-state deprotection strategy for PIMs that resulted in simultaneous enhancements of permeability and selectivity relative to pre-protected PIM analogues.29,52 This method, called free volume manipulation (FVM), uses labile functional groups, such as a tert-butoxycarbonyl group (tBOC), to alter physical packing structures and hence transport properties of the deprotected polymers.29,52 By introducing bulky functional groups to the polymer backbone, the intersegmental distances are intentionally widened when the polymer is processed into a solid-state film. Then, after removing these labile functional groups through simple heat treatment in the solid-state, free volume increases. This method was highly effective for amine-functionalized PIM-1 (PIM-NH2).29Fig. 1 shows the FVM approach for PIM-NH2. In short, the archetypal PIM-1 is converted into its amine-functional counterpart, PIM-NH2, which significantly decreases free volume due to hydrogen bonding.29 Next, the amine groups in PIM-NH2 are protected with tBOC groups to yield PIM-tBOC. PIM-tBOC subsequently undergoes thermal treatment to yield free volume manipulated PIM-NH2 (PIM-NH2-FVM), which has slightly larger average free volume element (FVE) diameters along with the potential for light urea crosslinks.29 This approach results in enhancements of both permeability and selectivity for PIM-NH2.29
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Fig. 1 The free volume manipulation (FVM) approach for PIM-NH2 starting with the precursor PIM-1. Note that light crosslinking in PIM-NH2-FVM is represented by a potential urea bond. |
In the context of long-term stability, the effect of FVM on physical aging is difficult to predict. FVM increases FVE size and drives the polymer further from its theoretical chain packing equilibrium, which can potentially accelerate the aging rate. However, it also introduces crosslinks that can reduce translational motions of the polymer segments. In previous comparisons of fresh and aged PIM-NH2 and PIM-NH2-FVM permeability data,29 both polymers showed similar permeability reductions, suggesting that FVM may stabilize the polymer matrix from accelerated physical aging despite introducing the additional free volume.
In this study, we investigate this phenomenon in greater depth, studying the influence of amine functionalization and the subsequent free volume manipulation on archetypal PIM-1 films by monitoring pure-gas transport properties over approximately 10000 hours using non-plasticizing gases (H2, O2, N2, and CH4). In addition to providing a baseline comparison for the aging behaviors of these post-synthetically modified PIMs, this study aims to bridge the guiding principles already established for conventional polymers on the role of free volume, hydrogen bonds, and crosslinks on physical aging behaviors of microporous polymers. By maintaining identical dioxane backbone structures while modifying hydrogen bonding, crosslinking, and free volume, this set of polymers provides a unique system to directly compare the effect of these features on physical aging.
![]() | (1) |
Wide-angle X-ray scattering (WAXS) patterns were collected under 0.08 mbar vacuum using a SAXSLAB machine equipped with a DECTRIS PILATUS3 R 300K detector and Rigaku 002 microfocus X-ray source. All patterns were collected for 1200 s, and the resulting pattern was plotted as intensity I(q) versus scattering wavevector q:
![]() | (2) |
Positron annihilation lifetime spectroscopy (PALS) data were collected using an automated EG&G ORTEC fast–fast coincidence system. A Mylar envelope containing a 22Na radioisotope source was sandwiched between two small stacks of polymer films, each stack approximately 1.5 mm thick. All tests were performed under vacuum (10−6 torr) at room temperature, and a minimum of 5 files with 4.5 × 106 integrated counts were collected for each polymer sample. After each measurement, least squares optimization was performed with the LT v9 program using a four-component (para-positronium, free positron, and ortho-positronium) fitted model.54 In the model, the para-positronium lifetime was fixed to τ1 = 0.125 ns and free positron (τ2) and two ortho-positronium lifetimes (τ3 and τ4) were fitted, indicating bimodal free volume distributions, which typically result in better statistical fitting for high free volume glassy polymers.55 Intensities (Ii) for all of these components were also determined.56 The PAScual software was adapted to calculate pore size distributions,57 and the Tao–Eldrup equation was used to calculate the average FVE size using the obtained ortho-positronium lifetimes:56,58
![]() | (3) |
![]() | (4) |
Pure-gas permeabilities of four gases (H2, CH4, N2, and O2) were tested for each aging sample using a constant volume–variable pressure automated permeation testing apparatus (Maxwell Robotics). All samples were masked with epoxy glue on brass supports to ensure no leakage from upstream to downstream. Further details of the testing setup can be found elsewhere.20,29,52 Before any permeation test, the entire apparatus was held under vacuum for 8 h. When changing to a different testing gas, the upstream was flushed with high pressure He, and the entire apparatus was held under vacuum between 0.5 and 1 h depending on the prior gas tested. All permeation tests for physical aging curves were performed at 35 °C with an upstream pressure of 15 psia and a downstream pressure <9.5 torr. For the variable temperature permeation study, the testing conditions were kept similar to those in the previous description, but the tests were performed at 35, 45, 55, and 65 °C.
Permeability (P) was calculated using the following equation:
![]() | (5) |
![]() | (6) |
Pure-gas sorption isotherms of CH4, N2, and O2 were measured at 35 °C using an automated pressure decay sorption testing apparatus (Maxwell Robotics). All connections in the apparatus were sealed using VCR gaskets to limit uncertainty from leaks. For each sorption test, at least 0.1 g of polymer films were loaded into a 3 cm3 sample cell. At the beginning of the sorption measurement, the entire apparatus was degassed under full vacuum for 8 h. When changing to a different testing gas, the apparatus was flushed with high pressure He and held under vacuum for 3 h. The charge volume was held at each testing pressure for 0.3 h before dosing the gas into the sample chamber. Once the testing gas was dosed, the sample chamber was allowed to equilibrate at the testing pressure for 2.5, 2, and 1 h for CH4, N2, and O2, respectively. Each sorption isotherm was collected up to 700 psia and fitted using the dual-mode sorption (DMS) model, which is commonly used to describe sorption in glassy polymers:65
![]() | (7) |
At each testing pressure, the amount of gas sorbed by the sample was calculated by mass balance using the pressure in the charge chamber and the equilibrated pressure after the charge gas was dosed into the sample chamber. The pure-gas sorption coefficients were then calculated by dividing the gas concentration in the polymer by the testing pressure:
![]() | (8) |
Polymer | PIM-1 | PIM-NH2 | PIM-NH2-FVM |
---|---|---|---|
a Light urea crosslinks were not considered in the calculation. | |||
Thickness (μm) | 37.6 ± 0.9 | 51.3 ± 1.1 | 51.2 ± 2.0 |
Density (g cm−3) | 1.21 ± 0.06 | 1.28 ± 0.02 | 1.25 ± 0.02 |
FFVgroupa | 0.23 ± 0.04 | 0.16 ± 0.01 | 0.18 ± 0.01 |
FFVPALS | 0.255 ± 0.005 | 0.215 ± 0.004 | 0.213 ± 0.006 |
Drying conditions | Vacuum, 130 °C, 12 h | Vacuum, 130 °C, 12 h | Vacuum, 130 °C, 12 h |
Post-treatment conditions | n/a | Vacuum, 250 °C, 27 h | Vacuum, 250 °C, 27 h |
Fig. 2 depicts a graphical comparison of the pure-gas permeabilities of H2, O2, N2, and CH4 for the three PIM polymers as a function of time to approximately 10000 h. All data points in Fig. 2 are normalized to the first data point for easier comparison of trends among polymers, but comparisons of aging behavior on an absolute scale are shown in Fig. S1† and the tabulated values are in Table S4† for reference. As shown in Table S4,† the permeability and selectivity of fresh films are reasonably similar compared to the previously reported values.29 Given the need to understand uncertainty and reproducibility for membrane-based gas separation,77 at least three total samples from different casting batches were tested up to 1000 h, and the results are shown in Fig. S5 and 6† for comparison. The general trends remained the same within the tested 1000 h, confirming the reproducibility of our results shown in Fig. 2.
Physical aging of conventional polymer membranes manifests itself in permeability loss since polymers lose free volume as polymer chains relax toward their equilibrium packing structure.38 As shown in Fig. 2, all three PIM polymers showed this traditionally observed permeability loss with aging time, suggesting that neither the introduction of secondary interactions from amine groups nor the introduction of light crosslinks mitigates free volume reduction. The extent of permeability reduction (CH4 > N2 > O2 > H2) exactly followed the order of kinetic gas diameters (CH4: 3.80 Å; N2: 3.64 Å; O2: 3.46 Å; H2: 2.89 Å), indicating that the dependence of physical aging rate monitored via permeability correlated directly with the sizes of penetrants. Such a dependence is seen in many other studies in the literature,47,78 and it is attributed to the strong effect of free volume loss on diffusivity, as will be further discussed later. Among the three polymers tested, in general, PIM-NH2-FVM showed the largest permeability decrease, resulting in a 75% decrease for the largest gas considered, CH4, followed by PIM-NH2 (70%) and PIM-1 (50%), respectively. Interestingly, the extent of permeability decreases for the polymers considered switched order for the smallest gas considered, H2, as shown in Fig. 2a. In this case, PIM-1 had a 26% decrease from its initial permeability to the final measured permeability at approximately 10000 h, while PIM-NH2 and PIM-NH2-FVM showed a 17% and a 9% decrease, respectively, from their initial hydrogen permeability.
To further elucidate these findings, the permeability data in Fig. 2 have been fitted to the following equation:79,80
P = P0t−βP | (9) |
Regarding the observed change in the order of aging rates when testing H2 for our samples as shown in Fig. 2a, we note that previous studies have proposed that small gases such as H2 may have unique transport behavior relative to larger gases due to small, interconnected void spaces within the membrane matrix.81 We further note that the switch is also readily observed in Fig. 3. The higher relative change in permeability for H2 in PIM-1 compared to PIM-NH2 and PIM-NH2-FVM is simply a result of H2 surveying a broader portion of the free volume distribution in PIM-1 compared to other gas molecules. From a simulation study of PIM-1 by Li et al.,78 the effective FFV of PIM-1 had a strong dependence on the size of the probe molecules surveying its accessible free volume. PIM-1 had an FFV of 0.255 when surveyed with an H2 molecule (Connolly radius of 1.45 Å), while it had an FFV of 0.222 when surveyed with a CO2 molecule (Connolly radius of 1.65 Å).78 In the case of the PIMs studied in this work, PIM-1 had the largest FFV, and the addition of polar functional groups such as amines as well as thermal treatment reduced the amount of free volume inside the polymer matrix for PIM-NH2 and PIM-NH2-FVM, as seen from the FFV values in Table 1. Hence, a more significant effect of aging on the smallest penetrant is observed for PIM-1. Additionally, the stronger influence of free volume loss on diffusivity dominates with increasing gas size for the post-synthetically modified counterparts.
Fig. 4 shows the ideal selectivity of two gas pairs, H2/CH4 and O2/N2, monitored as a function of time. Analogous to the relative permeability aging plots, the selectivities were normalized to the first data point for easier comparison, and the selectivities on an absolute scale are shown in Fig. S2.† The H2/CH4 and O2/N2 selectivities increased for all polymers with aging time. This result is a typical permeability and selectivity trade-off response of physical aging since the reduction of free volume in polymer membranes affects larger molecules more significantly.38 When compared across the samples, PIM-NH2-FVM showed the highest gain in selectivities for both gas pairs throughout the aging period, resulting in a 260% increase for H2/CH4, followed by 180% for PIM-NH2 and 50% for PIM-1. Fig. 5 shows the comparison of selectivity gain and permeability loss with aging compared to other PIMs in the literature that reported aging data with a minimum of 100 days of aging. It is important to note that direct comparisons or correlations cannot be made because all data have different aging times and thicknesses, but a few interesting observations can be gleaned. First, PIMs that have hydrogen bonds without crosslinks (the blue data points in Fig. 5) did not have a particularly distinguishing gain in selectivity or loss in permeability with aging compared to other PIMs. This finding suggests the high sensitivity of the aging rate constant we observed for PIM-NH2 in Fig. 3 may not be a generalizable feature for PIMs with hydrogen bonds. Introducing hydrogen bonds to polymer backbone structures may only tune the free volume structures of PIMs without giving a distinctive aging attribute, at least for non-condensable gases. Further analysis should be made for condensable gases such as CO2 since polar functional groups that induce hydrogen bonds significantly affect gas transport of condensable gases.65 Second, while there are limited aging data for crosslinked PIMs in the literature, crosslinked PIMs generally gained much higher selectivities with aging compared to non-crosslinked PIMs. In fact, the smallest gain in H2/CH4 selectivity among the crosslinked PIMs was 143%, and this was the ninth highest gain among all PIMs considered (N = 58). Given these findings, the high sensitivity of aging rate constants we observed for PIM-NH2-FVM in Fig. 3 may be a generalizable feature of crosslinked PIMs.
![]() | ||
Fig. 5 Comparison of long-term physical aging effects on (a) H2/CH4 and (b) O2/N2 separation for various PIMs reported in the literature.13,19,89,94–105 The star symbols are PIMs in this study, and only polymer films with a minimum of 100 days of aging are considered. The dotted orange line is a parity line, representing equal permeability loss and selectivity gain. |
What is particularly interesting about PIM-NH2-FVM is that it showed the steepest slope from the origin of the H2/CH4 plot even among the crosslinked PIMs in the literature, highlighting its remarkably large boost in selectivity without losing much permeability to hydrogen. This result suggests that there is unique stability towards smaller gas molecules and increasing molecular screening of large gas molecules with aging. We hypothesize that this observation is a result of the FVM method creating a larger number of small FVE pathways for small gas molecules such as hydrogen. From our previous report on PALS data, applying FVM to PIM-NH2 resulted in a 19% increase in the intensity related to the smaller FVE (I3) along with the narrowing of the FVE distribution,29 indicating an increase in the number of small FVEs and a reduction of larger FVEs, which heavily impacts the diffusion of larger gas molecules. Thus, PIM-NH2-FVM exhibited a significant permeability reduction for larger gas molecules while still permitting rapid and selective diffusion of small gas molecules such as hydrogen.
Pi = DiSi | (10) |
This model states that permeation of penetrants through a polymer membrane is governed by both thermodynamic factors (i.e., sorption of penetrants into the polymer matrix) and kinetic factors (i.e., diffusion of penetrants through the polymer matrix). By using the ideal gas selectivity equation in eqn (6), diffusion and sorption selectivity can also be decoupled as follows:
![]() | (11) |
As shown in Fig. 6b, the sorption coefficients did not significantly change compared to permeability for all gases and polymers. The changes in sorption coefficients throughout the 2230 h aging period were less than −4% for PIM-1 and PIM-NH2-FVM for all gases. While PIM-NH2 showed a larger decrease among the three polymers, the changes were still small compared to the permeability changes shown in Fig. 6a. As shown in Fig. S8–10,† sorption isotherms did not change significantly even at high pressures for all polymers, and this result demonstrates that a decrease in sorption is not a significant factor regardless of the type of functional groups and additional crosslinks that PIMs contain. Relatively small changes in sorption coefficients have also been observed for CO2 in PIM-1 from a detailed physical aging study by Bernardo et al.,79 even though CO2 has relatively higher sorption compared to the gases tested in this study. Thus, we believe our findings are generalizable to various gases with PIMs.
In contrast to the sorption coefficients, the effective diffusivity decreased significantly with aging, as shown in Fig. 6c. This finding suggests that the mechanism for aging of these PIMs is driven by changes to the packing structure of polymer segments. As expected, changes in both permeability and diffusivity followed identical trends, correlating closely with the size of penetrants, as shown in Fig. 6a and c. The densification of the polymer matrix impacts the diffusion of larger gas penetrants more significantly compared to smaller gas penetrants, and this finding confirms our assertions in Section 3.1 that physical aging monitored by permeability has a large dependence on the kinetic gas diameter due to the diffusion selective nature of PIMs. Hence, the change in diffusion selectivity had a much larger contribution to the permselectivity, as shown in Fig. 6d, and H2/CH4 separation had a much larger gain in selectivity compared to O2/N2 due to the larger difference in penetrant sizes (0.91 Å difference for H2/CH4versus 0.18 Å difference for O2/N2), as shown in Fig. 4.
According to the Brandt model, the activation energy of diffusion, ED, is directly proportional to the square of the penetrant diameter (d2):
ED = cd2 − f | (12) |
![]() | (13) |
To investigate the changes in energetics of gas transport, variable-temperature permeation tests were performed to obtain the activation energy of permeation, Ep:20
P = P0e−Ep/RT | (14) |
![]() | ||
Fig. 8 Comparison of changes in activation energy of permeation (Ep) for PIM-NH2 and PIM-NH2-FVM samples upon aging. The samples were aged for 710 h. |
The changes in the packing structure of the PIMs considered in this study were investigated using wide-angle X-ray scattering (WAXS). Fig. 9a presents the WAXS patterns for both fresh and aged PIM samples, where the dotted lines indicate the fresh films. All patterns show four distinct peaks, and these peaks clearly resemble the WAXS patterns observed in our previous study.29 A study by McDermott et al. showed that the three peaks in the high-q region, highlighted by the gray background in Fig. 9a, represent characteristic distances of spiro centers on different chains, while the larger peak in the low-q region is closely related to the microporosity of PIMs.85,86 While the locations of the low-q peaks were nearly unchanged for the PIMs studied in this work, the three characteristic peaks in the high-q region showed non-negligible changes, which provides quantitative insights into polymer densification during the aging period. A magnified version of the WAXS patterns in the high-q region is shown in Fig. 9b, and Table S13† presents the d-spacing, which are the average interchain distances that were calculated from these three peaks.
As shown in Fig. 9c, the average interchain distances decreased for all polymers with aging. Interestingly, PIM-NH2 had a comparable reduction for all peaks compared to PIM-1, and PIM-NH2-FVM had the largest reduction for all three peaks. While these are very small changes (∼1–2%) and the characteristic spiro center distances do not directly inform the actual free volume sizes in PIMs, we notice a few correlations that agree with the analysis in Fig. 4 and 6. First, the comparable d-spacing reductions for PIM-NH2 and PIM-NH2-FVM with PIM-1 further support our assertion that neither the introduction of secondary interactions from amine groups nor the introduction of light crosslinks mitigates volume contraction. Even if the chain mobilities decrease due to reduced free volume from hydrogen bonding and crosslinks, the polymer packing structures still evolve towards their equilibrium conformations at an appreciable rate within the tested time frame. Thus, permeability reductions were observed for all polymers. Second, the reduction order for peak 3 (P3), which is associated with the smallest d-spacing of around 3.8 Å, correlates with the order of selectivity gains in Fig. 4. This result suggests that d-spacing in the range of gas penetrant size has the largest effect on selectivity, a result that would be consistent with PIMs obeying the sorption–diffusion model, similar to other reports in the literature.24,29,87
Given the thickness of our films for this study, we wanted to investigate ultra-long term aging behavior of our samples. To this end, the free volume changes of the PIM polymers with aging time were investigated using positron annihilation lifetime spectroscopy (PALS), which is able to accurately observe small free volume changes.40,88–92 During a PALS experiment, positrons (e+) are naturally emitted from a radioactive source. These positrons “pick off” electrons in FVEs, forming a transient semi-stable particle ortho-positronium (o-PS) that is subsequently annihilated in the polymer matrix. The lifetimes of the o-PS atoms are correlated with average FVE sizes by using the Tao–Eldrup relationship, and FVE distributions can also be obtained by analyzing the lifetimes and the relative intensities of the model parameters.93 Two o-PS lifetimes (τ3 and τ4) were obtained from PALS for the samples in this work, indicating the presence of a bimodal distribution within the PIM films. The total FFV for a bimodal FVE distribution is the sum of FFV calculated from each bimodal peak as shown in eqn (4). Thus, the amount of free volume contributed by each average FVE diameter (di) can be approximated using the following equation:59,63
![]() | (15) |
Tables 2 and S14† summarize the PALS parameters obtained for the samples from our previous study29 that have been aged for approximately 20000 h (833 days). Fig. 10a–c show the comparison of the average FVE size distributions (FSDs) obtained for fresh and aged samples. It is noted that our samples have the same chemistry and underwent the same drying conditions as the previous study, but earlier samples had been aged under atmospheric conditions instead of in a desiccator. As shown in Table 2 and Fig. 10a–c, PIM-1 showed the largest average FVE size reduction of −25.6 ± 5.2% and −3.6 ± 0.4% for the small and large FVEs, respectively, compared to PIM-NH2 (−16.6 ± 4.3% and −3.0 ± 0.6%) and PIM-NH2-FVM (−17.5 ± 4.5% and −1.4 ± 0.7%) over this relatively long aging period. The notably larger changes in both FVE sizes for PIM-1 agree with our analysis in Section 3.1 in that PIM-1 had the largest permeability reduction for only H2 but a smaller permeability reduction for larger gases. This interesting finding is related to H2 being able to survey a broader portion of free volume distribution due to its small size. Remarkably, the reduction orders for both d3 and d4 were strongly correlated with the order of the corresponding initial FFVPALS,τi, as shown in Fig. 10d and e. More detailed experiments are required to investigate the correlation between free volume and rates of free volume reduction, but the comparison of FSDs with long aging times suggests that the total extent of structural change is most strongly correlated with the initial amount of free volume and not with amines or light crosslinks. This finding matches known trends for conventional glassy polymers,40,84 suggesting that the same mechanistic and theoretical phenomena for aging apply to PIMs.
Aging timeb (h) | PIM-1 | PIM-NH2 | PIM-NH2-FVM | |
---|---|---|---|---|
19![]() |
21![]() |
19![]() |
||
a Errors were calculated based on the population standard deviations. b The presented time is the aging time at the start of PALS experiments. c PALS data for fresh samples are from a previous study.29 | ||||
Freshc | d 3 (Å) | 6.4 ± 0.3 | 6.2 ± 0.2 | 6.3 ± 0.2 |
d 4 (Å) | 11.25 ± 0.04 | 10.13 ± 0.05 | 10.14 ± 0.06 | |
FFVPALS,τ3 | 0.014 ± 0.002 | 0.012 ± 0.001 | 0.015 ± 0.002 | |
FFVPALS,τ4 | 0.240 ± 0.005 | 0.203 ± 0.004 | 0.199 ± 0.005 | |
Aged | d 3 (Å) | 4.76 ± 0.25 | 5.17 ± 0.21 | 5.20 ± 0.23 |
d 4 (Å) | 10.84 ± 0.03 | 9.83 ± 0.03 | 10.00 ± 0.04 | |
FFVPALS,τ3 | 0.006 ± 0.001 | 0.007 ± 0.001 | 0.008 ± 0.001 | |
FFVPALS,τ4 | 0.181 ± 0.003 | 0.199 ± 0.003 | 0.178 ± 0.004 |
![]() | ||
Fig. 10 Comparison of change in bimodal FVE size distribution (FSD) for (a) PIM-1 (b) PIM-NH2, and (c) PIM-NH2-FVM. The FVEs of fresh films from the previous study29 are plotted as dotted lines, and samples that have been aged for approximately 20![]() |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ta01680c |
This journal is © The Royal Society of Chemistry 2023 |