Henghui
Huang
a,
Shaoyi
Xu
ab,
Li
Zhang
c,
Jiantao
Fan
*ab,
Hui
Li
*a and
Haijiang
Wang
c
aDepartment of Materials Science and Engineering, Southern University of Science and Technology, Shenzhen 518055, Guangdong, China
bAcademy for Advanced Interdisciplinary Studies, Southern University of Science and Technology, Shenzhen, 518055, China
cDepartment of Mechanical and Energy Engineering, Southern University of Science and Technology, Shenzhen, 518055, China
First published on 11th November 2020
Nanomaterials with a uniform size, large surface area, high adsorption capacity, and excellent dispersion are critical to proton conduction and cell performance when functionalized and incorporated into a proton exchange membrane. We designed and fabricated a novel composite PEM based on vinylphosphonic acid-functionalized mesoporous silica nanoparticles (VPA-MSNs), with the aim of improving the cell performance and proton conductivity of a perfluorosulfonic acid (PFSA) membrane under low relative humidity (RH) conditions. The experimental results show that the VPA-MSN(–NH2)/PFSA composite membrane provides a proton conductivity of up to 23.2 mS cm−1 at 30% RH and up to 9.6 mS cm−1 at 10% RH, which are respectively 3.2 and 8.6 times higher than those of a pristine PFSA membrane, and 5.6 and 10.4 times higher than those of a commercial Nafion membrane. In addition, the VPA-MSN(–NH2)/PFSA composite membrane exhibits superior fuel cell performance and low ohmic resistance at low relative humidity. Improvements in water absorption/retention, proton conductivity, and single-cell performance resulted from these effectively hydrophilic surfaces and mass transfer pathways, as the mesoporous structure and abundant functional groups in the membrane enhanced the connectivity of the hydrophilic zone, forming new proton transport channels. The incorporation of VPA-MSNs into the PFSA matrix also enhanced the water retention properties and mechanical strength, and adjusted the organic–inorganic interface and hydrophilic ionic domains inside the membranes simultaneously. The results indicate that this new type of VPA-MSN(–NH2)/PFSA composite membrane is promising for developing PEMs that tolerate variations in humidity.
To enhance a membrane's water retention and adjust its water content, materials with high water sorption and low water release have been introduced into PEMs. Inorganic nanosized fillers such as SiO2, ZrO2, and TiO2 have abundant hydrophilic groups that retain a large number of water molecules through hydrogen bonding, ensuring that the PEM has a sufficiently high water content;4 therefore they have broad applications under low humidity operating conditions. However, the poor dispersion and low proton conductivity limited SiO2 nanoparticle application in high performance PEMs.5
The high surface free energy of SiO2 nanoparticles is the main reason for their poor dispersion. A strategy using electrostatic repulsion or steric hindrance has shown the potential to address these problems through functionalizing their surface, effectively preventing particle agglomeration and improving their dispersibility.6 In another approach, when more and stronger carrier sites (conducting groups), which are crucial determiners of proton transfer, were introduced into the surface of nanoparticles, proton conductivity was enhanced. To date, various SiO2-based materials with various functional groups have been incorporated into membranes to improve the proton conduction and cell performance of proton exchange membranes under low humidity and high temperature conditions. Amiinu et al. prepared a Nafion hybrid membrane including silica functionalized with imidazole groups using the sol–gel method.7 They claimed that the synthesized membrane had better thermo-mechanical properties and proton conductivity in a non-humidified environment. Kamol et al. prepared composite membranes by dispersing fluorinated polyoxadiazole oligomer (ODF)-functionalized silica nanoparticles in a Nafion matrix. A physical crosslinking effect and better water retention were observed due to the inclusion of these functionalized nanoparticles.8 Wang et al. prepared a type of bio-inspired Nafion membrane (Bio-Nafion) composed of biofunctional SiO2 (Bio-SiO2) nanofibers and a Nafion matrix; their results showed that the introduction of Bio-SiO2 nanofibers into composite membranes significantly improved water uptake, dimensional stability, and proton conductivity at low relative humidity.6 Sangaraju et al. synthesized new sulfonated silica (SSA) using tetraethyl orthosilicate and chlorosulfuric acid through calcination, which was used as a filler to create Nafion–SSA composite membranes for use in PEMFCs under low relative humidity (RH) conditions. High water uptake and ion exchange capacity values were observed, and the Nafion–SSA composite membrane showed better proton conductivity than recast Nafion.9 Zhao et al. investigated the effects of the –NH2 group and the –PO3H2 group in submicrospheres of silica as a filler for a Nafion membrane. Their work showed that –PO3H2 groups will perform well at low relative humidity. They mentioned that the lack of hydration can be resolved by adding a large number of –PO3H2 groups to the filler.10 The presence of silica in a Nafion matrix can help to overcome the limitations of Nafion by improving proton conductivity at elevated temperature and low RH due to the excellent water retention capacity of silica,11 which has significantly improved fuel cell performance. Table 1 shows a summary of silica application in Nafion membranes.
Embedded nano-material | Proton conductivity (mS cm−1) | Water uptake (%) | Reference |
---|---|---|---|
Amino acid functionalized SiO2 nanofiber | 140.4 (20 °C, 100RH), 242.4 (80 °C, 100RH), in-plane | 47.6% (10 wt%, 20 °C) | 7 |
Amino-acid functionalized hollow mesoporous silica microspheres | 119 (30 °C, 100RH), 210 (80 °C, 100RH), in-plane | 41.2% (4 wt%, 30 °C) | 12 |
Sulfonated silica | 111 (100% RH, 80 °C), 84 (100% RH, 30 °C), through-plane | 24.9% (5 wt%, 25 °C) | 9 |
Fluorinated polyoxadiazole oligomer (ODF)-functionalized silica nanoparticles | 65 (100% RH, 80 °C), 4.0 (15%, 80 °C), through-plane | 48.2% (5 wt%, 25 °C) | 8 |
Silica functionalized with imidazole groups | 105 (100% RH, 80 °C), 0.65 (anhydrous condition, 80 °C), through-plane | — | 13 |
The –NH2 group and the –PO3H2 group in submicrospheres of silica | 207(100% RH, 80 °C), 15 mS (40% RH, 80 °C), through-plane | 41.2% (5 wt%, 25 °C) | 10 |
Phosphonic acid-functionalized mesoporous silica nanoparticles | 136 (90% RH, 80 °C), 19.6 (30% RH, 80 °C), 9.2 (10% RH, 80 °C), through-plane | 49.5 (10 wt%, 25 °C) | This study |
Among these potentially promising water-retentive materials for PEM applications at low RH, phosphonic acid-based materials meet the requirements. Phosphoric acid groups act not only as proton donors but also as proton acceptors, and they possess a relatively high dielectric constant and hydration energy,14 so phosphonic acid-based materials have higher water absorption and retention capacity,15 as well as the ability to transport protons at low humidity; hence, phosphonic acid-functionalized SiO2 nanoparticles may have better water-retention capacity and proton conductivity than unmodified ones. When phosphoric acid groups with the same type of electric charge were introduced into the surface of nanoparticles, the mutual repulsion among nanoparticles and between the nanoparticles and the PFSA molecular chain was enhanced,16 endowing them with excellent dispersion performance in a PFSA membrane.
The specific surface area and size of nanoparticles incorporated into a proton exchange membrane are critical to the number of proton conduction sites and proton conduction paths.17 Mesoporous materials have larger specific surface areas because their nanoparticles contain many micropores with diameters in the range of 2–50 nm. The size of synthesized nanoparticles is closely related to their precursors and surfactants. When precursors possess abundant ionic groups, they repel each other, making it difficult for nano-microspheres to agglomerate and thereby keeping the prepared nanoparticles small.18 The size and amount of micropores have a significant impact on the water-retention of composite membranes, the water in micropores has a lower saturated vapor pressure value (according to the Kelvin equation) and therefore materials with smaller pores have higher water retention.
We therefore designed and synthesized mesoporous silica nanoparticles (MSNs) with different functional groups and micropores, to study the types and number of functional groups as well as how the sizes and number of their mesopores influenced the nanoparticles' dispersion, water retention, mechanical properties, proton conduction, and single-cell performance of the composite membrane. Abundant water-sorption groups, numerous smaller size pores, and excellent dispersion ensured that the prepared VPA-MSN(–NH2)/PFSA composite membranes had better proton conductivity and single-cell performance than an unmodified PFSA membrane, and lower impedance under low-humidity conditions. The experimental results show that the prepared VPA-MSN(–NH2)/PFSA composite membrane in this paper has great potential for application at low relative humidity.
The membranes' water uptake was calculated from the weight difference between the dry membrane and the wet membrane (eqn (2.1)), and their swelling ratio was tested by measuring changes in the length and thickness in dry and wet states (eqn (2.2)). The dry and wet membranes were prepared as previously reported.22
(2.1) |
(2.2) |
Water release testing was conducted on the PFSA membrane and VPA-MSN(–NH2)/PFSA composite membranes at 60 °C and 10% RH. The membranes were weighed (W) at various test times, and the water retention ratio was calculated with eqn (2.3):
(2.3) |
The mechanical properties of the PEMs were studied using the ASTM D882-02 standard test method. Membrane samples were die-cut into dumbbell-shaped specimens (40 mm × 5 mm gauge area), and then the specimens were tested with an Instron 5866 universal tester, using a tensile rate of 10 mm min−1 and at 25 ± 1 °C.23
(2.4) |
An 885 Fuel Cell Potentiostat (Scribner Associates) was used to evaluate MEAs containing various PEMs: the PFSA, Gore 740, and PFSA/PEIMPA composite membranes. The operating temperature of the single-cell system was controlled by using a temperature control system, and the RH of the feed gas was controlled by using a humidifier. The feed gases (hydrogen and air) had stoichiometries of 1.3 and 2.0, respectively. The cell voltage at various current densities (scanned from 0 to 2 A cm−2) was tested, yielding polarization curves and power density curves. Before testing, the MEA needed to be activated at a high current density until the cell performance stabilized.24
The EIS of the MEAs was carried out using a frequency analyzer after the polarization curves were obtained. The scanning frequency of the EIS measurements was 106 to 0.1 Hz at a current density of 1.0 A cm−2.
Fig. 1 Procedure for synthesizing the MSNs with –OH or –NH2 groups and the phosphonic acid-functionalized MSNs. |
The structure of MNS(–OH), MSN(–NH2) and VPA-MSN(–NH2) was characterized using Raman spectra. As shown in Fig. 2(a), the peaks at 966 cm−1 and 2940 cm−1, which indicate the stretching vibrations of –NH– and –NH2, are weaker for PEIMPA than for MNS(–NH2), indicating that most of the amino groups were reacted and replaced. The peaks at 657 cm−1 and 820 cm−1 represent the bending vibrations of P–O, and the peak at 1060 cm−1 represents the bending vibration of PO bonds, indicating that –PO3H2 groups were introduced into MNS(–NH2), some of the –NH2 groups were functionalized as phosphonic acid, and the phosphonic acid-functionalized MSNs were appropriately synthesized.
Fig. S1(a and b)† illustrates the 13C NMR spectrum of MSN(–NH2) and VPA-MSN(–NH2), and Fig. S2(a–c)† shows the 13C NMR spectrum of the MSN(–NH2), and a mixture of MSN(–NH2) and VPA at the beginning of the reaction and after 6 hours of reaction (the 12 hour reaction product mentioned in Section 2.3 is not used for the NMR test because of the poor solubility of final products for the NMR test). Compared with those for only the mixture of MSN(–NH2) and VPA, the intensities of the peaks at 131.2 and 137.4 ppm (assigned to CH2CH) have obviously decreased and new peaks have appeared at 58.7 and 41.2 ppm (assigned to –CH2–CH–NH–), implying that the –NH2 groups have reacted with the CC bonds, and CC bonds were converted to –C–C– bonds. Moreover, the peak at 41.2 ppm (assigned to –CH2–PO3H2) has appeared for obtained VPA-MSN(–NH2), indicating that the –PO3H2 groups were introduced. Besides, compared with the 1H NMR spectrum of MSN(–NH2) and the VPA-MSN(–NH2), the results show the –NH2 content decreased and new –PO3H2 appeared. Therefore, the 1H NMR, 13C NMR and Raman spectra demonstrated that the reaction between nucleophile NH2 and a double bond is successful and the prepared VPA-MSN(–NH2) was obtained.
Fig. 3 The zeta potential of the MSNs with various functional groups, dispersed in an ethanol–water solution. |
The particle size and distribution of the MSNs with –OH, –NH2, and –PO3H2 groups were determined by dynamic light scattering (DLS). The effective diameter and polydispersity of the MSNs are presented in Fig. 4(a and b). The MSNs with –PO3H2 groups were smaller and had a more uniform distribution than those with –OH. The size of the MSNs with –PO3H2 groups was also observed using scanning electron microscopy (SEM) and transmission electron microscopy (TEM), and the surface morphology of the nanospheres was clearly observed. As can be seen in the SEM and TEM images (Fig. 3(c and d)), the diameter of most microspheres was in the range of 30–80 nm, and the nanoparticles' distribution was uniform.
Fig. 4 Effective diameter and polydispersity of (a) MSN(–OH) and (b) VPA-MSN(–NH2); (c) SEM and (d) TEM images of VPA-MSN(–NH2). |
Because of their excellent dispersion and small size, the VPA-MSN(–NH2) nanoparticles had a larger adsorption capacity and specific surface area.25 The nitrogen adsorption–desorption isotherms for the MSNs are shown in Fig. 5. Based on the BJH theory, we tested and calculated the Brunauer–Emmet–Teller (BET) surface area, adsorption capacity, total pore volume, and mean pore diameter of the MSNs (see Table 1). The MSN(–OH) had a BET surface area of 329.66 m2 g−1, compared with up to 1092.4 m2 g−1 for the VPA-MSN(–NH2). It is known that functional groups exist mainly on the surface of nanospheres, so MSNs possess more active sites for functionalization or proton transfer when the particles have a larger specific surface area. The volume adsorbed in the nitrogen adsorption–desorption isotherm of the MSN nanometer microspheres increased sharply at a relative pressure (p/p0) of approximately 0.50, indicating capillary condensation in the microspheres' uniform structure. Although the pore size distributions (Fig. 4(c and d)) and mean pore diameters (Table 2) were similar for MSN(–OH) and VPA-MSN(–NH2), the proportion of micropores (less than 2 nm) in MSN(–NH2) was greater than that in MSN(–OH), indicating that the presence of the amino groups enhanced the dispersion of the template agent (CTAB).
Fig. 5 (a) BET adsorption isotherms (N2) and (b) pore size distributions of MSN(–OH) and VPA-MSN(–NH2). |
Sample | BET s.a. (m2 g−1) | V m (cm3(STP) g−1) | Total pore volume (p/p0 = 0.990) | Mean pore diameter (nm) |
---|---|---|---|---|
MSN | 329.66 | 75.741 | 0.5816 | 7.0573 |
VPA-MSN(–NH2) | 1092.4 | 250.99 | 2.4787 | 6.0762 |
The cross-sectional and surface SEM images of MSN(–OH)/PFSA and VPA-MSN(–NH2)/PFSA are shown in Fig. 6. The VPA-MSN(–NH2)/PFSA composite membranes were smaller and had excellent dispersion. The nanoparticles were uniformly distributed inside the membrane, no defects or particle aggregates were detected on the surface or in the cross-section, and they were slightly larger than pristine nanoparticles. But when the MSN(–OH) was incorporated into the composite membrane, it showed particle aggregates in the cross-sectional and surface SEM images. The EDS mapping for the surface and cross-section of MSN(–OH)/PFSA and VPA-MSN(–NH2)/PFSA composite membranes also showed that the additive (VPA-MSN(–NH2)) was uniformly distributed throughout the membrane (see Fig. 7). The incorporated particles' large size and uneven dispersion weakened the membrane's water retention performance and lengthened the proton conduction paths, hampering proton conductivity and failing to improve the PEM's single-cell performance.26
Fig. 6 SEM images of the VPA-MSN(–NH2)/PFSA composite membrane: (a) surface, and (b) cross-section. SEM images of the MSN(–OH)/PFSA composite membrane: (c) surface and (d) cross-section. |
Fig. 7 EDS mapping for the surface of the (a) VPA-MSN(–NH2)/PFSA composite membrane and (b) MSN(–OH)/PFSA, and (c and d) cross-section of the VPA-MSN(–NH2)/PFSA composite membrane. |
Fig. 8 Mechanical properties of the PFSA membrane, Gore 740 membrane, and VPA-MSN(–NH2)/PFSA composite membranes with various contents. |
The dimensional stability of the membranes was characterized using their swelling ratios. As seen in Table 3, the swelling ratios of the PFSA membrane and Gore 740 membrane were 3.54% and 2.86%. In comparison, the values for the MSN(–OH)/PFSA and VPA-MSN(–NH2)/PFSA composite membranes with various contents were higher than that for the Gore 740 membrane but lower than that for the PFSA. This was because on the one hand, more water molecules were absorbed by the hydrophilic groups, increasing the PEM's swelling ratio, and on the other hand, the PFSA matrix was fixed by nanoparticles with rigid structures.28
Sample | Water uptake (%) | Water contact angle (°) | Swelling ratio (%) |
---|---|---|---|
PFSA | 38.9 ± 1.2 | 76.2 ± 1.16 | 3.54 ± 0.16 |
Gore 740 | 37.6 ± 0.8 | 84.23 ± 1.29 | 2.68 ± 0.12 |
2MSN(–OH)/PFSA | 41.2 ± 1.3 | 69.26 ± 0.86 | 3.12 ± 0.23 |
2MSN(–NH2)/PFSA | 43.2 ± 0.6 | 67.25 ± 1.37 | 2.57 ± 0.09 |
1VPA-MSN(–NH2)/PFSA | 42.3 ± 1.7 | 71.53 ± 0.54 | 3.34 ± 0.24 |
2VPA-MSN(–NH2)/PFSA | 45.5 ± 1.3 | 68.45 ± 0.97 | 3.06 ± 0.34 |
5VPA-MSN(–NH2)/PFSA | 48.7 ± 2.1 | 64.23 ± 1.15 | 2.95 ± 0.27 |
Our findings demonstrated that the MSN(–NH2) was effective for simultaneously improving the mechanical strength and dimensional stability of the composite membranes, guaranteeing them under practical fuel cell operating conditions.
The water uptake of the PFSA and VPA-MSN(–NH2)/PFSA composite membranes under 10–100% RH conditions and immersion in water is exhibited in Fig. 9(a). The water absorption ratio of various membranes demonstrated that the VPA-MSN(–NH2) and MSN(–OH) added into composite membranes can effectively improve the water sorption of the membrane across the entire humidity range, and the water uptake of the VPA-MSN(–NH2)/PFSA composite membrane is significantly higher than that of PFSA at lower RH. Further, the composite membranes of the VPA-MSN(–NH2)/PFSA with a higher content (i.e., with more –PO3H2 groups) also have higher water uptake, indicating that the water molecules were adsorbed by a larger number of –PO3H2 groups and numerous smaller pores.
Water retention was characterized using the water release ratios of the membranes at low RH. Fig. 9(b) presents the water retention at 10% RH and various test times. The first stage was characterized by high water release via the evaporation of free water, while the second stage saw more moderate water release through the slower evaporation of bound water. Hence, the incorporation of MSN(–NH2)/PFSA or VPA-MSN(–NH2)/PFSA significantly reduced the composite membranes' water release ratios in these initial stages. In the first stage, the rate of water loss was mainly related to the hydration energy of the existing groups within the membrane; the decreasing slope of the water release curve and the decrease in the rate of water loss indicated that the –NH2 and –PO3H2 groups had a stronger affinity for water than the –OH groups. In the second stage, the abundant mesopores and micropores in the added materials were key factors affecting the water content in the equilibrium state, because they could store and retain more water. According to the Kelvin equation, the saturated vapor pressure of water is significantly reduced in smaller channels, which is why the composite membranes remained wet at a low RH.30
The surface hydrophilicity of the VPA-MSN(–NH2)/PFSA composite membrane was also enhanced (as measured from the membranes' water contact angles; see Table 2) because more hydrophilic groups had been introduced into the composite membrane. The membranes with higher surface hydrophilicity could effectively decrease the interfacial resistance to water and proton transfer in the membrane.
Fig. 10 Proton conductivity of the PFSA membrane and VPA-MSN(–NH2)/PFSA composite membranes with 1, 2, and 5 wt% contents at various RHs and 80 °C. |
From the temperature-dependence of proton conductivity, the activation energy (Ea) for proton conductivity was calculated using the Arrhenius equation, and the values are presented in Fig. 11(a and b). At 80% RH, the Ea for the PFSA membrane was 11.74 kJ mol−1 and Gore 740 membrane was 12.89 kJ mol−1. The incorporation of VPA-MSN and MNN with –NH2 or –OH groups slightly increased the Ea of the composite membrane to 13.76 kJ mol−1 and 16.56 kJ mol−1, implying that the Grotthuss mechanism predominated in proton transport. This is because sulfonic acid groups are more susceptible to proton ionization than phosphate groups. Under low humidity conditions (RH = 20%), compared with PFSA (25.18 kJ mol−1) and Gore 740 membranes (26.56 kJ mol−1) with a high energy barrier, the VPA-MSN(–NH2)/PFSA membranes had a low conductivity barrier, and the Ea values for the 1VPA-MSN(–NH2)/PFSA, 2VPA-MSN(–NH2)/PFSA, and 5VPA-MSN(–NH2)/PFSA composite membranes were 21.38, 20.35, and 18.78 kJ mol−1, respectively. This implies that the VPA-MSN(–NH2) efficiently helped the membrane transmit protons, and that its high VPA-MSN(–NH2) loading made the 5VPA-MSN(–NH2)/PFSA composite membrane more favorable for proton transfer due to its low energy barrier. These experimental results indicated that the PFSA membrane had stronger humidity dependence, and the proton-conduction Ea increased from 11.74 kJ mol−1 to 25.18 kJ mol−1 when the RH dropped from 80% to 20%. The addition of VPA-MSN(–NH2) effectively reduced the humidity dependence of the PEMs: for the 5VPA-MSN(–NH2)/PFSA composite membrane, the proton conduction Ea only increased from 14.47 to 18.78 kJ mol−1. The lower proton-conduction energy barrier and enhanced proton conductivity of VPA-MSN(–NH2)/PFSA occurred mainly because VPA-MSN(–NH2) adsorbed and retained water molecules, increased the number of carriers for proton conduction and favored the Grotthuss mechanism transport pathway.
Fig. 11 Arrhenius plot of the activation energy for proton conductivity at (a) 80% RH and (b) 20% RH for the PFSA membrane, Gore 740 membrane and VPA-MSN(–NH2)/PFSA composite membranes. |
Improving the connectivity of the hydrophilic zone in the composite membrane is the key approach for enhancing proton conductivity. This hydrophilic region is formed by microphase separation of the ionomer, so we investigated the microphase separation in the VPA-MSN(–NH2)/PFSA composite membranes using SAXS.33 The results for the PFSA membrane and VPA-MSN(–NH2)/PFSA composite membranes with various contents are presented in Fig. 12, which shows a change in the spacing of the hydrophilic zone after the introduction of VPA-MSN(–NH2) and MSN(–OH). The q values (scattering vector) of PFSA, MSN(–OH)/PFSA, 1VPA-MSN(–NH2)/PFSA, 2VPA-MSN(–NH2)/PFSA and 5VPA-MSN(–NH2)/PFSA were 1.29, 1.72, 2.24, 2.78 and 3.56 nm−1, respectively. The Bragg spacing d, which refers to the distance between two water clusters, can be calculated using d = 2π/q. The d value shifted from 5.04 to 1.77 nm after 5 wt% VPA-MSN(–NH2) was incorporated into the PFSA. Less space between water clusters meant that the VPA-MSN(–NH2)/PFSA composite membrane network connected adjacent hydrophilic domains within the PFSA matrix, thereby enhancing the continuity of the proton channels. Fig. 12 also shows that the scattering peaks of the VPA-MSN(–NH2)/PFSA composite membrane are wider than those for the PFSA membrane. The reason for these results is that a part of separated hydrophilic areas merged into a large hydrophilic area, and therefore the size of the hydrophilic zone was not uniform and the boundary between hydrophilic and hydrophobic domains did not appear clearly, as well as the addition of the VPA-MSN into the PFSA matrix reduced their phase separation. Therefore the small q value of the VPA-MSN(–NH2)/PFSA membrane was attributed to the formation of large ionic clusters and enhancement of the continuity of hydrophilic domains, and the broader SAXS profile was attributed to the low phase separation and the hydrophilic zones with various sizes. Although the phase separation of the membrane was decreased, the ion conductivity increased with the VPA-MSN(–NH2) content because of the large ionic domains and a large number of ion-conducting functional groups.
Fig. 13 H2 crossover current density of Gore 740, PFSA MNS(–OH)/PFSA and VPA-MSN(–NH2)/PFSA composite membranes in LSV tests. |
Fig. 15 The cell voltages of MEAs based on Gore 740, PFSA, and VPA-MSN(–NH2)/PFSA composite membranes at 100, 80, 50, 20, and 0% RH (current density = 1 A cm−2). |
To further understand the effect that incorporating VPA-MSN(–NH2) and MSN(–OH) had on resistance to proton transport, Fig. 16 shows the EIS analyses of the MEAs based on VPA-MSN(–NH2)/PFSA and MSN(–OH)/PFSA composite membranes with various contents at 80%, 50%, 20%, and 0% RH. The results indicated that the cell voltage at 1 A cm2 is consistent with EIS of the MEA; as more VPA-MSN(–NH2) was incorporated, the composite membrane was better able to retain its lower resistance when the RH dropped from 80% to 0%, and the MEA with more VPA-MSN(–NH2) maintained a higher cell voltage at low RH. This was because these composite membranes had better water-retention ability, so a wetter state was maintained even at low or no RH, resulting in lower resistance to proton transport. In this way, more connected proton transport channels were preserved in the composite membrane than in the PFSA membrane, improving proton conduction and single-cell performance at lower RHs.
Fig. 16 EIS of PFSA and VPA-MSN(–NH2)/PFSA composite membranes at (a) 80% RH, (b) 50% RH, (c) 20% RH, and (d) 0% RH (current density = 1 A cm−2). |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0se01339k |
This journal is © The Royal Society of Chemistry 2021 |