Preetom Sarkar†
ab,
Aruna Kumar Mohanty†a,
Parthasarathi Bandyopadhyaya,
Santanu Chattopadhyayb and
Susanta Banerjee*a
aMaterial Science Centre, Indian Institute of Technology, Kharagpur – 721302, India. E-mail: susanta@matsc.iitkgp.ernet.in; Tel: +91-3222-283972
bRubber Technology Centre, Indian Institute of Technology, Kharagpur – 721302, India
First published on 15th January 2014
A series of new semifluorinated sulfonated polyimide copolymers (DHNHXX) were prepared from 1,4,5,8-naphthalenetetracarboxylic dianhydride (NTDA), 4,4′-diaminostilbene-2,2′-disulfonic acid (DSDSA) and 1,4-bis-[{2′-trifluoromethyl-4′-(4′′-aminophenyl)phenoxy}] benzene (HQA). The degree of sulfonation of DHNHXX was varied by changing the molar ratio of the sulfonated diamine, DSDSA to the non-sulfonated diamine, HQA. The flexible DHNHXX membranes showed high thermal stability (desulfonation temperature above 270 °C) and good mechanical properties. The oxidative stability of DHNHXX improved with increasing the fluorine content. DHNHXX showed anisotropic dimensional changes, and good water stability (did not dissolve for up to 415 h), higher than many other sulfonated polyimides. Transmission electron microscopy (TEM) analysis revealed cluster-like microstructures for the DHNHXX membranes, suggesting good phase-separated morphology. DHNH70 with IEC = 2.10 meq. g−1 exhibited high proton conductivity, with a maximum up to 129 mS cm−1 at 90 °C in water.
It has been observed that the sulfonated six-membered ring (naphthalenic) polyimides exhibit superior chemical and thermal stabilities and mechanical strength over analogous five-membered ring polyimides because of their strain-free ring structures.7,8 Mercier and coworkers5 first synthesized various sulfonated copolyimides from naphthalene-1,4,5,8-tetracarboxylic dianhydride (NTDA), 2,2′-bendizine sulfonic acid (BDSA) and common nonsulfonated diamine monomers. However, these SPIs from BDSA exhibited poor water stability. Consequently, Okamoto’s group synthesized SPIs using relatively flexible sulfonated diamines such as 4,4′-diaminodiphenyl ether-2,2′-disulfonic acid (ODADS), 4,4′-bis(4-aminophenoxy)biphenyl-3,3′-disulfonic acid (BAPBDS) and various non-sulfonated diamines which showed much better water stability at comparable ion exchange capacity (IEC) values.9,10 Similarly, McGrath et al.11 also reported the synthesis of SPIs with improved water stability based on a novel sulfonated diamine, 3,3′-disulfonic acid-bis[4-(3-aminophenoxy)phenyl]sulfone (SA-DADPS), containing flexible sulfone and ether linkages. Both groups independently observed that increasing the flexibility of the backbone structure of SPIs resulted in enhanced water stability. Okamoto and his coworkers also reported 2,2′-bis(3-sulfopropoxy)benzidine (2,2′-BSPB), 3,3′-bis(3-sulfopropoxy)benzidine (3,3′-BSPB) and 2,2′-bis (4-sulfobutoxy)benzidine (2,2′-BSBB)-based side chain-type SPIs which showed higher proton conductivities and better water stability than main-chain type SPIs.12,13 They attributed the improvement in stability and conductivity to the relatively higher basicity of sulfonated diamines and the well-separated micro-phase structures, respectively. However, the proton conductivity of the side chain-type SPIs bearing pendant sulfoalkoxy groups decreased largely at high temperature and low humidity due to the relatively easy cleavage of the sulfoalkoxy groups.14 It has also been reported that the structure of non-sulfonated diamines plays a vital role in tuning the solubility, water uptake, proton conductivity and the water stability of SPIs along with the structure of sulfonated diamines. Litt’s group15,16 has reported the influence of inherently developed chain spacing due to some angled and/or bulky non-sulfonated diamine moieties in SPIs in improving the dimensional stability and proton conductivity, particularly at high temperature and low relative humidity (RH). Miyatake et al.17 and Sun et al.18 also reported the improvement of the oxidative stability due to the hydrophobic trifluoromethyl group in the SPIs along with interchain spaces for water molecules in aiding the proton transport mechanism.
In a previous article,8 we reported fluorinated SPIs, DQNXX {for NTDA–DSDSA/QA(m/(1¬m))} from the commercially available sulfonated diamine, 4,4′-diaminostilbene-2,2′-disulfonic acid (DSDSA) and non-sulfonated diamine, 4,4′-bis [3′-trifluoromethyl-4′(4-aminobenzoxy)benzyl]biphenyl (QA), bearing trifluoromethyl (–CF3) groups. The DQNXX membranes exhibited high proton conductivity, good phase-separated morphology, low water uptake and improved water stability. However, it is felt necessary for further improvement of the PEM properties of the DQNXX membranes with a high degree of sulfonation (≤80 mol% of disulfonation). Hence, more stable polymer systems need to be explored. Consequently, in continuation of our research into PEMs, an attempt has been made to increase the proton conductivity at a low degree of sulfonation through the use of a low molecular weight and comparatively flexible fluorinated diamine, 1,4-bis-[{2′-trifluoromethyl 4′-(4′′-aminophenyl)phenoxy}] benzene (HQA) in place of QA in DQNXX. Accordingly, this work describes the synthesis and characterization of new SPIs, DHNHXX based on HQA. The properties of the synthesized materials, such as their thermal and oxidative stability, mechanical strength, water uptake behavior and proton conductivity have been investigated in detail and compared with other polymers.
:
50)} is described as an example. First, 0.340244 g (0.0918 mmol) of DSDSA, 10 mL of m-cresol and 0.2044 g (0.28 mL) of TEA were added into a dried 250 mL, three-necked round-bottomed flask equipped with a condenser and N2 inlet. The mixture was then heated to 80 °C and stirred under N2 until DSDSA was dissolved. Thereafter, 0.533257 g (0.0918 mmol) of HQA, 0.492692 g (0.1837 mmol) of NTDA and 0.44871 g of BA were added successively, followed by the addition of ∼10 mL of m-cresol. The mixture was stirred at 80 °C for 4 h, at 180 °C for 16 h and at 200 °C for 3 h, respectively. After cooling to room temperature, 3 mL of m-cresol was added to dilute the highly viscous solution. After completion of the reaction, the viscous polymer solution was slowly poured into excess isopropyl alcohol under constant stirring. The fibrous precipitate was collected by filtration. The fibrous polymer was further washed thoroughly by methanol to remove any residual solvent and impurities. Finally, fibre-like polymer was collected after drying at 120 °C under vacuum overnight. Films were prepared from the polymer solutions in DMAC (15% w/v) by pouring them in to Petri dishes and heating sequentially at different temperature (at 80 °C (12 h), 100 °C, 120 °C, 140 °C and 160 °C each for 2 h) for slow removal of the solvent. The acidification of the membranes was performed by immersing them in 1.5 M H2SO4 at room temperature for three days. Except for DHNH40, transparent, light brown and flexible membranes were obtained from the polymers. The thicknesses of the membranes (in the range ∼40–60 μm) were measured as the average of the ten different measurements of the same membrane sample using a Mitutoyo Digimatic micrometer with an accuracy of 0.001 mm, and in each case the standard deviation was within 3 μm of the average thickness of the membrane.
NMR data of the acid form: 1H-NMR (DMSO-d6): δ (ppm) 8.83–8.61 (H5, H6); 8.30 (H1); 8.13–8.07 (H9, H10); 7.92–7.83 (H2, H3, H8); 7.59–7.50 (H4, H7); 7.38–7.28 (H11, H12).
The ion exchange capacities (IECs) of the DHNHXX membranes were determined by the back-titration method as reported elsewhere.20 The membrane in acid form (0.2 g) was converted to the sodium form by immersing the membrane in 50 mL of 1.0 M NaCl aqueous solution for 48 h. The released proton was then titrated with standard 0.01 M NaOH aqueous solution using phenolphthalein as the indicator. The water absorption and dimensional stability of the membranes were tested at the desired temperature from the water uptake ratio and swelling ratio, which was defined as the change in weight and dimension (diameter or thickness) of the membranes after soaking in water for 5 h divided by the weight and dimensions of the dry samples. The oxidative stability of the DHNHXX membranes was evaluated by recording the elapsed time in which the membranes (10 mm × 10 mm) started to break into pieces (τ1) and dissolved completely (τ2) under occasional stirring after immersion in Fenton's reagent (2 ppm FeSO4 in 3% H2O2) at 80 °C. The water stability was investigated by measuring the elapsed time in which a membrane lost its mechanical properties (brittle or bending at the corners) after its immersion into water at 80 °C.
The proton conductivity (σ, S cm−1) in the plane direction of the DHNHXX membranes (1 cm × 2 cm) was calculated using σ = l/wdR (l (= 0.8 cm) is the distance between the electrodes, and w and d are the width and thickness of the membrane, respectively). The resistance value (R) was measured over the frequency range of 100 Hz to 2 MHz by the two-point probe method using AC impedance spectroscopy (HIOKI 3532-50 LCR Hi-TESTER). The prehydrated membranes were clamped across the pair of platinum electrodes in a home-made Teflon conductivity cell, as reported elsewhere.20,21 Conductivity measurements under fully hydrated conditions were then carried out with the cell immersed in deionized water by increasing the temperature from 30 to 90 °C at a heating rate of 1–2 °C min−1.
| Polymer | DSDSA (mol%) | ηinha (dL g−1) | DSb | |
|---|---|---|---|---|
| Theoretical | NMR | |||
| a Inherent viscosity of the DHNHXX polymers in NMP at 30 °C; polymer concentration 0.5 g dL−1.b Degree of sulfonation: the theoretical value is calculated from the monomer feed ratio; the NMR value corresponds to the experimentally determined value from the content of the DSDSA moiety in the polymer. | ||||
| DHNH40 | 40 | 1.48 | 0.4 | 0.38 |
| DHNH50 | 50 | 2.17 | 0.5 | 0.46 |
| DHNH60 | 60 | 1.88 | 0.6 | 0.60 |
| DHNH70 | 70 | 1.97 | 0.7 | 0.66 |
The solubility behavior of the polymers (both in the TEA salt and acid form) at room temperature was tested (as 10% (w/v)) in various common organic solvents, and the results are shown in Table 2. The DHNHXX (acid form) polymers were soluble in polar aprotic solvents such as DMSO, DMAc, DMF, NMP and pyridine, but insoluble in THF or acetone. The DHNXX (TEA salt form) polymers with XX > 40 showed good solubility in m-cresol, but not in their proton form. This might be due to the intensive polymer chain packing in their proton form. Though the polymers were prepared in m-cresol, after isolation by precipitation and drying, DHNXX with XX > 70 (i.e. DHN80) was mostly in the form of an insoluble mass or was sparingly soluble in m-cresol. Similarly, DHNXX with XX < 50 was not completely soluble and formed a suspension of particles. This behavior can be explained on the basis of π–π interactions of planar NTDA moieties.22 Increasing the content of the ionic DSDSA comonomer above XX = 40 improves the solubility of DHNXX. However, after reaching XX = 70, a further increase of the ionic DSDSA moieties might have resulted in higher ordering in the microstructure which complementarily facilitated the increased π–π interactions of planar NTDA moieties, ultimately leading to aggregates. The overall good solubility of DHNHXX, XX = 40–70, was due to the combined effects of flexible vinyl and ether (–O–) linkages which form a different intrasegmental configuration, and the bulky trifluoromethyl (–CF3) groups in the backbone, which disrupt the regularity of the molecular chains and hinder the dense chain packing.
| Polymer | NMP | DMAc | DMF | DMSO | Py | THF | m-Cresol |
|---|---|---|---|---|---|---|---|
| a Data in parentheses refer to the TEA salt form, +: soluble, ±: partially soluble, − : insoluble. | |||||||
| DHNH40 | ±(±) | ±(±) | ±(±) | ±(±) | ±(±) | −(−) | ±(±) |
| DHNH50 | +(+) | +(+) | +(+) | +(+) | +(+) | −(−) | +(+) |
| DHNH60 | +(+) | +(+) | +(+) | +(+) | +(+) | −(−) | −(+) |
| DHNH70 | +(+) | ±(+) | ±(+) | +(+) | +(+) | −(−) | −(±) |
The chemical structure of DHNHXX was confirmed by both FTIR and NMR spectroscopy. Fig. 1 shows the FTIR spectra of the DHNHXX polymers as a function of DS. The spectra showed strong absorption bands at around 1712 cm−1 and 1674 cm−1 due to the stretching vibrations of the carbonyl groups of the naphthalimide ring, while the band at around 1349 cm−1 appeared due to the C–N asymmetric stretching. These bands clearly indicate the formation of imide rings. The bands at 1024 cm−1 and 1081 cm−1 were due to the symmetric and asymmetric stretching of the sulfonic acid groups. The intensities of the peaks at 1024 cm−1 and 1081 cm−1 increased with the degree of disulfonation. The representative 1H NMR spectrum of DHNH60 is presented in Fig. 2. The spectral signals can be assigned to all of the magnetically different protons of the polymer repeat unit. No residual amine, amide or carboxylic protons were observed, indicating the imidisation reaction was complete. After acid treatment, the peak related to triethylammonium protons at δ (ppm) = 1.14 and 3.07 disappeared. Extra peaks due to free aromatic amine or free carboxylic acid in moiety were not found. This confirmed that the salt form of the SPI copolymer was successfully converted into the corresponding acid form without the degradation of the polymer backbone. The 1H NMR spectra were also used to calculate the copolymer composition, similar to the method used in our previous article20 (Table 1). The area under the broad signal due to the protons of the naphthalimide moiety (δ (ppm) = 8.83–8.61) was taken as the integral value = 1 and was used for the integration of the remaining signals. The copolymer composition calculated from the integrals of the signal regions I–III (Fig. 2) was in good agreement with the feed ratio.
The mechanical properties of the DHNHXX membranes were measured in both dry and wet conditions. For the wet conditions, the membranes were immersed in DI water at room temperature for 24 h prior to the measurements. The results are summarised in Table 3. The reason for the low value of the tensile strength for the DHNH40 membrane is viewed with scepticism, and might be attributed to the low quality of the film (opaque due to particle formation in the solution) and the low molecular weight of the formed polymers due to their phase-out (precipitation) during the polymerisation reaction. However, it should be noted that the remaining membranes showed comparable tensile strengths and much larger Young's moduli compared to many other reported six-membered SPIs.18,23 In the dry state the membranes showed tensile strengths in the range of 66–88 MPa and Young's moduli in the range of 1.74–2.36 GPa. The comparatively high elongation at break (14–49%) of the DHNHXX polymers with respect to the polymers reported by Sun et al.18 (Table 3), despite having similar non-sulfonated segments of the polymer structure, might be due to the flexible vinyl linkage of the sulfonated diamine, DSDSA, used in the preparation of DHNHXX. As is commonly experienced in aromatic PEMs, the elongation at break for the DHNHXX membranes (Fig. 4a) were much lower than that of the Nafion® 117 membrane (288%). In wet conditions (Fig. 4b), the membranes also showed good mechanical properties with tensile strengths of 28–48 MPa, elongation of 4–23% and Young's moduli of 1.20–1.56 GPa. Similar to the regular observed trend in PEMs, the tensile strength of the DHNHXX membranes decreased with increasing DS. It was also observed that the Young's moduli of the membranes did not show a regular trend with the increasing degree of sulfonation.
| Polymer | TSa (MPa) | Yb (GPa) | EBc (%) | Reference | |||
|---|---|---|---|---|---|---|---|
| Dry | Wet | Dry | Wet | Dry | Wet | ||
| a Tensile strength at a strain rate of 5% min−1, 65 ± 2% RH and 30 °C.b Young's modulus.c Elongation at break. | |||||||
| DHNH40 | 44 | 28 | 1.23 | 1.20 | 6.6 | 3.6 | This paper |
| DHNH50 | 88 | 73 | 1.74 | 1.55 | 48.5 | 23.1 | This paper |
| DHNH60 | 68 | 61 | 2.36 | 1.56 | 20.8 | 12.5 | This paper |
| DHNH70 | 66 | 48 | 2.17 | 1.38 | 13.7 | 7.8 | This paper |
NTDA–BABSA/6FBAB (3 : 1) |
73 | — | 1.85 | — | 10.3 | — | 18 |
NTDA–BABSA/6FAPB (3 : 1) |
75 | — | 2.06 | — | 9.5 | — | 18 |
NTDA–BABSA/BAPB (3 : 1) |
70 | — | 1.89 | — | 9.7 | — | 18 |
| Nafion® 117 | 22 | ND | 0.16 | ND | 288 | ND | This paper |
The oxidative and water stability of the PEMs are critical aspects as the fuel cell operates under humidified and oxidative conditions. As shown in Table 4, the DHNHXX membranes showed fairly good oxidative stability which decreased with the increasing degree of sulfonation. Thus, as expected, the DHNH40 membrane showed the highest oxidative stability (τ2 = 4.6 h) and DHNH70 showed the lowest oxidative stability (τ2 = 2.9 h) in the series. Nevertheless, these oxidative stability values are better than those of many other reported sulfonated polyimides.18,24 The high oxidative stability of the DHNHXX membranes is due to the presence of hydrophobic trifluoromethyl groups which could protect the polymer main chain from being attacked by water molecules containing highly oxidizing radical species.13,17 In addition, although displaying a relatively high fluorine content, the DHNHXX membranes displayed lower oxidative stability in comparison to our previously reported DQNXX membranes.8 This might be due to the comparatively slightly higher water absorption due to the higher IEC of the DHNHXX membranes (relatively lower molecular weight of HQA with respect to QA in the co-SPIs) and the relatively greater flexible backbone structure resulting in higher entanglement and more free space.
| Polymer | IECW,Theo. (meq. g−1)a | Thickness (μm) | Oxidative stabilityb (h) | Water stabilityc (h) | Reference | |
|---|---|---|---|---|---|---|
| τ1 | τ2 | |||||
| a IECW,Theo. = (1000/MWrepeat unit) × DSTheo. × 2, where DSTheo. is calculated from the monomer feed ratio.b The time expended for the membrane to begin to break (τ1), or the complete dissolution (τ2) in Fenton's reagent (2 ppm FeSO4 in 3% H2O2) at 80 °C.c Measured as the time in which the membrane lost its mechanical properties in hot water (80 °C).d Completely dissolved.e Started to dissolve.f Reported for Fenton's reagent (30 ppm FeSO4 in 30% H2O2) at 30 °C.g Measured at 100 °C. | ||||||
| DHNH40 | 1.10 | 121 | 4.6 | 20.5 | >450 | This paper |
| DHNH50 | 1.41 | 61 | 3.9 | 14.7 | >450 | This paper |
| DHNH60 | 1.75 | 61 | 3.4 | 11.2 | >450 | This paper |
| DHNH70 | 2.10 | 39 | 2.9 | 6.3 | ∼417 | This paper |
| DQN60 | 1.67 | 51 | 3 | 20 | >400 | 8 |
| DQN70 | 2.03 | 45 | 1.2 | 9 | >400 | 8 |
| DQN80 | 2.42 | 50 | 0.8 | 4.5 | ∼120d | 8 |
NTDA–BAPBPDS/ODA (2 : 1) |
1.99 | 27 | 0.95 | 1.35e | 390 | 24 |
NTDA–BAPBPDS/BAPB (3 : 1) |
2.02 | 40 | 1.42 | 1.33e | 360 | 24 |
NTDA–BABSA/6FBAB (3 : 1) |
1.87 | 50–60 | 47f | 76f | 191g | 18 |
NTDA–BABSA/6FAPB (3 : 1) |
1.91 | 50–60 | 37f | 47f | 237g | 18 |
NTDA–BABSA/BAPB (3 : 1) |
1.95 | 50–60 | 29f | 49f | 290g | 18 |
The water stability of the DHNHXX membranes was studied in de-ionised water at 80 °C. The stability was characterized by the elapsed time by which the hydrated membranes lost their mechanical strength. The results of the water stability are listed in Table 4 and compared with the results of other SPIs. The DHNH70 membrane with the highest IEC in the series exhibited fair water stability, as it did not dissolve until the membrane was soaked in hot water for ∼415 h in relation to that of our previously reported DQN80 membrane, which dissolved in 120 h, and various other SPIs.8,18,24 This suggested that in addition to the validated profound effect of various sulfonated diamines, the structure of the non-sulfonated diamine can influence the water stability of SPI membranes. According to the general trend, for a particular series of polymers with varying DS, the stability of the membranes should decrease with the increase of the IEC (high water uptake). However, it is noticed that despite having higher IEC and water uptake, the DHNHXX membranes showed comparable water stability over DQNXX. It has been reported that a flexible chain can undergo relaxation more easily than rigid chains.6 Thus, the non-sulfonated diamine HQA with three benzene rings linked with ether bonds imparted greater flexibility to DHNHXX in comparison to the flexibility contribution of QA for DQNXX. Thus, the adverse effect of high IEC by high water uptake for DHNHXX (in comparison to DQNXX) was offset by the favorable effect of its flexible structure. It may be further noted that the increased fluorine content in DHNHXX compared to DQNXX did not bring significant change in the water stability (the DHNH70 membrane lost mechanical strength after 415 h). This might be due to the selective increased hydrophobicity of the non-sulfonated segment (due to the higher fluorine content) of the DHNHXX, while the hydrolysis degradation would generally take place in the sulfonated segment of the copolymer structure. In addition to the IEC and flexibility of SPIs, the basicity of the sulfonated and non-sulfonated diamine moieties greatly influences their water stability. The water stability is mainly determined by the electronic density of imido rings which is strongly dependent on the basicity of diamine moieties as previously mentioned. The greater the positive character of the imido carbonyl, the poorer the water stability (i.e. faster loss of mechanical strength). This indicates that in the present comparison (up to 450 h testing) between DHNHXX and DQNXX polymers, the effect of the basicity of the non-sulfonated diamine was found to be redundant, whereby both systems used the same common sulfonated diamine, DSDSA.
| Polymer | IECW (meq. g−1) | Dimensional change | WUWb (%) | λc [H2O/SO3−] | σ (mS cm−1) | Reference | |||||
|---|---|---|---|---|---|---|---|---|---|---|---|
| Theo. | Titr. | NMRa | Δl | Δt | 30 °C | 80 °C | 90 °C | ||||
| a IECW,NMR = (1000/MWrepeat unit) × DSNMR × 2, where DSNMR corresponds to the molar content of DSDSA units in the polymer structure determined from the 1H NMR spectra.b WUW (%) = [(Wwet − Wdry)/Wdry × 100], where Wwet and Wdry are the weights of the wet and dry membranes, respectively (measurements were at 30 °C).c λ = WUW (%)/(100 × IECW,Theo. × MW,H2O), where MW,H2O = 18 g mol−1. | |||||||||||
| DHNH40 | 1.10 | 1.02 | 1.04 | 0.01 | 0.03 | 15.23 | 7.71 | 5 | 10 | 12 | This paper |
| DHNH50 | 1.41 | 1.32 | 1.30 | 0.02 | 0.06 | 20.57 | 8.09 | 10 | 28 | 31 | This paper |
| DHNH60 | 1.75 | 1.63 | 1.75 | 0.04 | 0.17 | 26.29 | 8.36 | 28 | 60 | 66 | This paper |
| DHNH70 | 2.10 | 1.98 | 1.98 | 0.05 | 0.20 | 33.61 | 8.88 | 46 | 99 | 129 | This paper |
| DQN70 | 2.03 | 1.91 | ND | 0.02 | 0.11 | 29.73 | 8.2 | 23 | 40 | ND | 8 |
| DQN80 | 2.42 | 2.31 | ND | 0.03 | 0.12 | 35.61 | 8.2 | 55 | 81 | ND | 8 |
| Nafion® 117 | 0.91 | 0.90 | NA | 0.11 | 0.19 | 19 | 11.4 | 60 | 135 | 150 | This paper |
It is well known that the phase-separated morphology holds a close relation with the proton conductivity of the PEMs. Hence, the microstructure of the DHNHXX membranes stained with Ag+ was investigated by TEM. Thus, the dark regions, as shown in Fig. 5, refer to hydrophilic ionic clusters (due to the aggregation of sulfonated groups) and the brighter regions correspond to hydrophobic segments, giving a clear indication of the phase-separated morphology of the DHNHXX membranes. This morphological feature is in contrast to the homogeneous nature without clear phase-separated morphology reported for many other main chain-type SPIs.9 From the TEM micrograph it is clearly observed that the DHNH50 membrane consists of ionic clusters in a uniform distribution with average sizes of 27–30 nm. When the DS was 0.6 (DHNH60), it showed uniform distribution of a large amount of medium-sized ionic clusters (33–40 nm), along with a certain amount of smaller (20–25 nm) and larger (40–45 nm) ionic clusters. On increasing the DS further to 0.7 (DHNH70), a largely aggregated cluster morphology was observed with widely varied cluster sizes, with large amounts in the range 35–40 nm with certain small size clusters (17–24 nm) and larger ionic clusters (50–55 nm). These widely varied sizes of ionic clusters in the TEM micrograph was quite similar to many reported in the literature.25 At low DS (DHNH50), hydrophilic ionic clusters were exhibited as isolated domains in the system. However, with an increase in DS (DHNHXX, XX ≥ 60), the individual isolated clusters come close to each other and form clearer connectivity with clusters in close proximity for better proton transport. Although the phase-separated morphology was observed in both the DHNHXX polymers and our previously reported DQNXX polymers,8 the distribution of hydrophilic domains (ionic clusters) was significantly better in the former compared to the latter. Also, the variation in sizes of the clusters was very wide in the DQNXX polymers. If the above mentioned observation is true, since the size of the clusters varies in the presence of absorbed water (under different humid conditions), it might be considered that the increased flexibility and the proportion of hydrophobic trifluoromethyl groups in the nonsulfonated diamine moieties of the DHNHXX polymers would result in relatively increased uniformity in the sizes and distribution of clusters in the hydrophobic domains. It is also important to note that the microstructure obtained was similar to the reported microstructure of side chain-type SPIs,18,25 where well phase-separated morphology is generally expected. It is anticipated that the presence of pendent hydrophobic trifluoromethyl groups rendered the formation of this kind of phase-separated morphology responsible for improved proton conductivity.
In keeping with the common trend of PEMs, water uptake for the DHNHXX membranes gradually increased with the increasing IECW values (Table 5) and was in the range of 15–34%. Nevertheless, the maximum water uptake value (34%) for the DHNHXX polymers with the highest DS (DHNH70) was rather low as compared to many other reported fluorinated and non-fluorinated SPIs,6,18 and the value further decreased with an increase in the fluorine content (hydrophobic trifluoromethyl groups) in the DHNHXX polymer series. Hence, the presence of trifluoromethyl groups in the polymer structure can be envisaged as hindrance to excessive dimensional changes under humidified conditions, while helping to maintain acceptable mechanical properties for the membranes. Again, the water uptake values among the SPI membranes with different IECw values is often evaluated in terms of the number of water molecules absorbed per sulfonic acid group or the hydration number (λ).26 In this study, the λ values were calculated using the theoretical IECw values which were calculated from the molar ratio in the feed. Although the WU values increased with increasing IECw, λ remained more or less constant after reaching a certain value (λ ∼ 8), as shown in Table 5. This may be attributed to the higher rigidity of the aromatic SPI chains and the strong ionic interaction among the sulfonic acid groups, which restricted the free volume for water absorption beyond a certain limit.
Table 5 lists the water swelling values for the DHNHXX membranes, as they showed anisotropic character due to the relatively larger dimensional change in thickness than in the plane direction. The anisotropic degree of membrane swelling, Δt/Δl, was in the range of 2.8–4.6, indicating significant anisotropic membrane swelling. It is expected that the lower dimensional change in the plane direction of the membrane is favorable for the high quality fabrication of membrane electrode assemblies for application under the humid conditions of fuel cells. The anisotropic membrane swelling of DHNHXX membranes is considered to be due to the favourable orientation of polymer chains in the plane direction. The rigid structure of the DHNHXX SPIs seemed to facilitate the alignment in the plane direction. The increased swelling (in both the plane and thickness directions) of the DHNHXX membranes in comparison to the DQNXX membranes might be due to the relatively reduced rigidity of the backbone structure and the higher probability of entanglement resulting from the flexible phenyl ether linkages of the HQA moieties in the co-SPIs.
Fig. 8 shows the temperature dependence of the proton conductivity for the DHNHXX and Nafion® 117 membranes in deionized water. The proton conductivity of membranes showed Arrhenius-type (σ = A
exp(−Ea/RT), where σ = proton conductivity (mS cm−1); A = pre-exponential factor; R = universal gas constant (8.314 J mol−1 K−1); T = absolute temperature (K)) temperature dependence. With the rise in temperature, the proton conductivity of all of the membranes increased; DHNH70 exhibited proton conductivity comparable to the level of conductivity of Nafion® 117 at high temperature. The activation energies, Ea, of the proton conductivity were in the range 13.8–18.46 kJ mol−1 for DHNHXX (i.e. for XX = 40, Ea = 14.97 kJ mol−1; for XX = 50, Ea = 18.46 kJ mol−1; for XX = 60, Ea = 13.80 kJ mol−1 and for XX = 70, Ea = 15.21 kJ mol−1). Under similar laboratory conditions for Nafion® 117 the value was 13.63 kJ mol−1, whereas the literature reports activation energies for Nafion® 117 between 7 and 14 kJ mol−1.30 This implied that the activation energies for DHNHXX were close to the activation energies of Nafion® 117. This suggests that the DHNHXX membranes may involve similar kinds of proton conduction mechanisms.
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| Fig. 8 Arrhenius temperature dependence of the proton conductivity (σ) of the DHNHXX and Nafion® 117 membranes. | ||
Footnote |
| † Authors made equal contribution. |
| This journal is © The Royal Society of Chemistry 2014 |