Novel Polymeric Composite TPPS/s-PEEK Membranes for Low Relative Humidity PEFC

Composite membranes based on different wt percentages of meso-tetrakis-(4-sulfonatophenyl)porphyrin (TPPS) embedded in a medium sulfonation degree (50%) sulfonated poly(etheretherketone) (s-PEEK) were investigated. The successful introduction of porphyrin into the membranes and the characterization of its different species into the membrane ionic domains were carried out by spectroscopic techniques. Moreover, the effect of TPPS arrangement was investigated in terms of water retention, proton conductivity and fuel cell performance at low relative humidity (RH). It was found that the introduction of this porphyrin induces a variation of the chemical-physical parameters, such as ion exchange capacity (IEC), water up-take (Wup %) λ and proton concentration ([H+]), attributable to the interactions that occur between the sulfonic groups of the polymer and the nitrogen sites of TPPS. The TPPS, in its J-aggregated form, actively participates in the proton conduction mechanism, also maintaining the adequate water content in more drastic conditions (80 °C and 50% RH). A maximum power density value of 462 mW cm−2 was obtained for the s-PEEK membrane, with a 0.77 wt % content of TPPS. This evidence suggests that the presence of J-aggregates in the proton conduction channels maintains a good hydration, even if a drastic reduction of the RH of the reactant gases occurs, preventing the membrane from a dry-out effect.


Introduction
The pressing international demand of greenhouse gases emissions reduction is implemented by the development of renewable and clean energy. In this scenario, the polymer electrolyte fuel cells (PEFCs) play a key role for energy production [1,2]. In fact, their high efficiency, energy density and environmental harmlessness, make them promising devices for clean energy generation.
The key component of PEFC is a polyelectrolyte membrane based on functionalized polymer, able to transfer protons from the anode to cathode compartments. Even if Nafion ® is the most commonly used membrane, due to its high proton conductivity, some disadvantages, such as water uptake, methanol permeability and cost, have oriented research to the study of alternative polymers. Poly-ether-ether-ketone (PEEK) is a low cost thermoplastic, widely used in the space-flight, petroleum, chemical and medical industrial fields, due to its heat and corrosion resistant properties [3][4][5]. Moreover, a wide range of literature has shown that functionalized PEEK containing sulfonic groups is suitable for PEFC applications [6,7]. The sulfonic groups are introduced in the main chain of the polymer via a direct sulfonation reaction, and the degree of functionalization produces polymer membranes Table 1. Identification labels for membranes under investigation and relative 5,10,15,20-meso-tetrakis (4-sulfonatophenyl)porphyrin (TPPS) content.

UV-Vis Extinction and Fluorescence Emission spectroscopies
The UV-vis extinction spectra were recorded for the three DMAc composite membranes at 25 • C on an Agilent mod. 8453 diode array spectrophotometer. The membranes were stabilized at room conditions before measuring. Fluorescence emission spectra were acquired on a Jobin Yvon-Spex Fluoromax 4 spectrofluorimeter. Emission spectra were not corrected for the absorbance of the samples.

Thickness Measurements
The thickness of the membranes was measured with a Mitutoyo digital thickness gauge (mod. Absolute). The samples, before the measurement, were equilibrates at room temperature and humidity. The thickness was measured as an average value of at least 20 points taken on the surface of each membrane and corresponds to a value of about 45 µm.

Ion Exchange Capacity
The ion exchange capacity (IEC, meq g −1 ) was calculated through acid base titration of the membrane, performed with an automatic titrator (Metrohm Mod. Titrino 751 GPD) as reported elsewhere [51]. The IEC of the titrated membrane is therefore given by Equation (1) IEC = V · M/m dry (1) where V is the titrant volume (mL), M is the concentration of the titrant (mol·L −1 ) and m dry is the dry mass of the sample (g).

Water Uptake, λ Parameter and Proton Concentration
The water uptake (W up %) was determined as percentage by calculating the difference in weight between the wet and the dry sample according to Equation (2) W up % = [(m wet − m dry )/m dry ] × 100 (2) where m wet and m dry are the wet and the dry mass (g) of the membrane sample, respectively. The dry mass was determined by weighing the sample after drying in an oven for 2 h at 80 • C under vacuum (1000 mbar); the wet mass was determined by weighing the sample after immersion in H 2 O for 24 h at 30 • C and for 2 h at 80 • C.
The λ parameter, expressed as the ratio moles H 2 O/moles-SO 3 H was calculated through the water uptake and IEC values ratio.
The proton concentration, expressed in M, is calculated as follows (Equation (3)): where V wet is the wet volume, expressed in cm 3 .

In-plane Proton Conductivity and Effective Mobility
The proton conductivity (σ, S cm −1 ) in the longitudinal direction was measured with the four probes method, using a commercial cell (Bekktech) and a potentiostat-galvanostat (AMEL mod. 2049), as reported elsewhere [14]. Proton conductivity was obtained at 30 • C and 80 • C and full humidification levels (100% RH), by applying Equation (4).
where R is the electrical resistance (Ω), L = 0.425 cm the fixed distance between the two platinum electrodes, W the width (cm), and T the thickness of the sample (cm). The activation energy was calculated by the Arrhenius law, from conductivity results carried out at 100% RH. The effective proton mobility µ (cm 2 V −1 s −1 ) was calculated as follows (Equation (5)): where [H + ] is the proton concentration and F is the Faraday constant (96,485 C mol −1 )

Fuel Cell Tests
Homemade electrodes were prepared by spraying the catalytic ink onto a commercial gas diffusion layer Sigracet-24BC (SGL group), following a standardized procedure [31]. A Pt loading of 0.5 mg cm −2 for both the anode and the cathode side was used. Membrane and electrodes were directly assembled in a single cell, tightened at 10 Nm, to obtain membrane-electrodes assemblies (MEAs).
The cell tests were performed in a 25 cm 2 cell, connected to a commercial test station (Fuel Cell Technologies). The different membranes developed were characterized by feeding humidified H 2 to the anode and humidified air to the cathode at the temperature of 80 • C, at the absolute gas pressure of 3.0 bar and at the values of RH of 50%, 75% and 100%. The gas flows were set at 1.5 and 2 times the stoichiometry at the working current for hydrogen and air, respectively. For each measurement, the open circuit voltage (OCV) values of the membranes were also measured. The cell resistance (R cell ) was measured at OCV with an Agilent milliohmmeter by a static method at a frequency of 1 kHz.

Spectroscopic Characterizations
Taking advantage of the favorable spectroscopic properties of porphyrins, the different preparation steps and the final composite membranes with different TPPS content were characterized by UV-Vis extinction and fluorescence emission techniques. Porphyrins exhibit in the visible region (400-700 nm) a very intense Soret band with a high molar extinction coefficient (ε ≈ 10 5 M −1 cm −1 ) and a pattern of weaker Q-bands at longer wavelengths (ε ≈ 10 4 M −1 cm −1 ). These latter are extremely diagnostic for the determination of structural changes and/or coordination on the macrocyclic ring. A change from D 2h to D 4h -symmetry leads to a simplification of the Q bands pattern with the concomitant reduction from four to two Q-bands [52]. For this class of compounds, fluorescence emission is evidenced by the presence of a typical double shaped band in the 600-800 nm range, originating from the Q (0,0) and Q (0,1) transitions. To characterize the re-casting steps, extinction spectra were recorded on the porphyrin TPPS and s-PEEK dispersion in DMAc, instantaneously after the addition of the filler and, in the sol phase (80 • C, 90 min.), before the stratification of the membranes by Doctor-Blade technique. Figure 1 shows the extinction spectra for 0.77 wt % TPPS sample taken as reference. Two distinct Soret bands centered at 420 nm and 445 nm are clearly detectable in the initial dispersion (black line), and ascribable to the porphyrin free base and its diacid form in DMAc, respectively. Moreover, a high baseline background, due to scattering of the dispersion, together with a broad band at about 500 nm are evident. According to the literature, the latter is ascribable to porphyrin J-aggregates in presence of s-PEEK polymer [31]. The thermal treatment of the sample, required for the membrane preparation, induces the solubilization of the filler, as confirmed by the decrease of baseline in the extinction spectrum ( Figure 1, red line), and the substantial disappearing of the J-aggregate band. Furthermore, the Soret band of the free base TPPS evidences an increase in intensity and a bathochromic shift (∆λ = +4 nm). Therefore, high temperature treatment causes the disaggregation of preformed porphyrin aggregates and the inclusion of the porphyrin free base in the polymeric matrix, as confirmed by the red shift of the Soret band, ascribable to the location of the porphyrin in a different microenvironment, with respect to the initial sample. In accordance with the data reported in the literature, this aspect is crucial for the formation of aggregates driven by weak intermolecular forces throughout the evaporation process and for a re-organization at nanoscale of the polymeric ionic domains [31]. Figure 2 displays the extinction spectra of the final composite membranes obtained with different wt % TPPS. Depending on the load of TPPS, a different distribution of the porphyrin free base, its diacid form and the J-aggregate is evident from the relative bands at 422, 445 and 496 nm, respectively. In particular, for the sample s-PEEK-0.77, the extinction spectrum seems almost attributable to porphyrin J-aggregates. treatment causes the disaggregation of preformed porphyrin aggregates and the inclusion of the porphyrin free base in the polymeric matrix, as confirmed by the red shift of the Soret band, ascribable to the location of the porphyrin in a different microenvironment, with respect to the initial sample. In accordance with the data reported in the literature, this aspect is crucial for the formation of aggregates driven by weak intermolecular forces throughout the evaporation process and for a reorganization at nanoscale of the polymeric ionic domains [31].   Indeed, the presence of a residual amount of monomeric TPPS in s-PEEK-0.77 composite membrane is confirmed by fluorescence emission spectra. According to the literature [31], the emission spectrum (inset of Figure 3, dashed line) shows, in the range 600-800 nm, the two band profile ascribable to the diacid porphyrin embedded in the polymeric matrix, together with a contribution from J-aggregate emission. Moreover, to confirm the location of the porphyrin species into the s-PEEK ionic domains and the proton exchange process, s-PEEK-0.77 composite membrane was dipped into alkaline solution (NaOH 1 M). The corresponding extinction spectrum ( Figure 3, solid black line) shows the complete disappearance of the J-aggregate band, and the exclusive presence of the Soret band centered at 424 nm, accompanied by four Q-bands at 524, 562, 598, 652, due to TPPS in its monomeric free base form. The corresponding emission spectrum (inset of Figure  3, solid black line) confirms the nature of the fluorophore embedded in the membrane. Porphyrin disaggregation in alkaline conditions has already been described for similar systems, with only a slight difference in the band positions with respect to the present system [31]. Indeed, this latter discrepancy could be due to the location of the porphyrin in a different microenvironment, due to the changed sulfonation degree for the two compared membranes. Indeed, the presence of a residual amount of monomeric TPPS in s-PEEK-0.77 composite membrane is confirmed by fluorescence emission spectra. According to the literature [31], the emission spectrum (inset of Figure 3, dashed line) shows, in the range 600-800 nm, the two band profile ascribable to the diacid porphyrin embedded in the polymeric matrix, together with a contribution from J-aggregate emission. Moreover, to confirm the location of the porphyrin species into the s-PEEK ionic domains and the proton exchange process, s-PEEK-0.77 composite membrane was dipped into alkaline solution (NaOH 1 M). The corresponding extinction spectrum (Figure 3, solid black line) shows the complete disappearance of the J-aggregate band, and the exclusive presence of the Soret band centered at 424 nm, accompanied by four Q-bands at 524, 562, 598, 652, due to TPPS in its monomeric free base form. The corresponding emission spectrum (inset of Figure 3, solid black line) confirms the nature of the fluorophore embedded in the membrane. Porphyrin disaggregation in alkaline conditions has already been described for similar systems, with only a slight difference in the band positions with respect to the present system [31]. Indeed, this latter discrepancy could be due to the location of the porphyrin in a different microenvironment, due to the changed sulfonation degree for the two compared membranes. due to TPPS in its monomeric free base form. The corresponding emission spectrum (inset of Figure  3, solid black line) confirms the nature of the fluorophore embedded in the membrane. Porphyrin disaggregation in alkaline conditions has already been described for similar systems, with only a slight difference in the band positions with respect to the present system [31]. Indeed, this latter discrepancy could be due to the location of the porphyrin in a different microenvironment, due to the changed sulfonation degree for the two compared membranes.

IEC, Wup, λ and Proton Concentration
Chemical-physical characterizations, such as IEC, W up % and λ, were carried out to understand how the different arrangements of TPPS could affect the main properties of the polymeric matrix. Regarding the IEC data, addition of TPPS to the s-PEEK is expected to increase the ion exchange capacity, due to the presence of sulfonic groups as substituents of the porphyrin structure. Moreover, it is known that interactions between the nitrogen atoms of porphyrin and the sulfonic groups of s-PEEK occur [25,31], so a reduction of ion exchange capacity is expected in the composite membranes, due to the lower availability of the exchangeable protons. Consequently, the measured IEC values should be considered as a compromise between the free proton ions, those involved in the interactions between the sulfonic groups of the polymer and TPPS and those responsible for TPPS stacking in the J-aggregates. As reported in Table 2, the introduction of TPPS increases the IEC of the s-PEEK-0.35 composite membrane respect the recast one. This behavior is attributable to the increase of the number of free protons available for ion exchange, due to the presence of the diacid porphyrin, as the predominant species into the polymer matrix. In s-PEEK-0.77, the TPPS distribution is mainly in J aggregates form (see Figure 2), and a reduction of IEC is expected with respect to 0.35 wt % load, due to the formation of a supramolecular network that involves the sulfonated groups of both the polymer and the porphyrin. An extra addition of TPPS up to 1.5 wt % causes a further reduction of IEC down to the recast value, since a higher number of SO 3 H groups of s-PEEK is involved in the hydrogen bonding with the porphyrin N-sites. The ability of functional groups to retain water molecules is quantified by measuring the water uptake (W up %) and calculating the λ parameter, as shown in Table 2. As expected, the W up % increases by increasing temperature and, over the entire investigated temperature range, presenting a maximum value for the s-PEEK-0.77 membrane. Additionally, the λ parameter, in accordance with the W up %, increases by increasing temperature and the amount of TPPS introduced. At 30 • C, the variation of λ follows the same trend as W up %, and most of the water is present as loosely bound water (λ ≤ 10) [53]. At 80 • C, higher λ values are found. In particular, for the samples s-PEEK-0.77 and s-PEEK-1.5, values of 22 and 14, respectively, are obtained. This finding indicates that water is present as a second phase, which mainly contributes to the proton conduction mechanism. This effect could be correlated with the introduction of porphyrin into the membranes, thereby inducing a re-arrangement of the polymeric structure, as also revealed by SEM characterization. In fact, as reported in the Supplementary Material, Figure S1, different morphologies can be found, depending on the porphyrin loads. These results are in accordance with morphological and structural studies previously reported for similar systems [31]. Regarding the proton concentration, in this case, the data are also in agreement with the trend of water uptake and λ, presenting a maximum value for the membrane with porphyrin in J-aggregate form (s-PEEK-0.77). The proton mobility expresses the ability of the proton carriers to move into hydrated polymeric channels, and it is strictly related to the proton conductivity mechanism. From Figure 4, it is evident that the proton mobility is higher for the membrane with 0.77 wt % TPPS, than the other composite and recast membranes for both the investigated temperatures. In addition, the same trend reported for proton concentration, meaning that all the protons present in the second hydration phase (λ > 10) are involved in the conduction mechanism.
Polymers 2020, 12, x FOR PEER REVIEW 8 of 14 the proton conductivity mechanism. From Figure 4, it is evident that the proton mobility is higher for the membrane with 0.77 wt % TPPS, than the other composite and recast membranes for both the investigated temperatures. In addition, the same trend reported for proton concentration, meaning that all the protons present in the second hydration phase (λ > 10) are involved in the conduction mechanism.

Electrochemical Characterizations
Another fundamental property of polymeric membranes is the proton conductivity, closely related to the chemical-physical parameters above discussed. The proton conductivity data, as a function of TPPS loading at two different temperatures (30 °C and 80 °C) are reported in Figure 5a,b. In general, the conductivity increases by increasing the temperature from 30 to 80 °C for all the investigated samples. Moreover, for both the temperatures, a maximum in conductivity can be found for s-PEEK-0.77, in accordance with the other chemical-physical values, especially water uptake, proton concentration, mobility and λ. The data were compared to λ values to highlight the importance of the bonding among protons, water and functional groups. The same trend was found for conductivity and λ at both the temperatures, meaning that the ratio of water per sulfonic group plays a key role in the conduction mechanism.

Electrochemical Characterizations
Another fundamental property of polymeric membranes is the proton conductivity, closely related to the chemical-physical parameters above discussed. The proton conductivity data, as a function of TPPS loading at two different temperatures (30 • C and 80 • C) are reported in Figure 5a,b. In general, the conductivity increases by increasing the temperature from 30 to 80 • C for all the investigated samples. Moreover, for both the temperatures, a maximum in conductivity can be found for s-PEEK-0.77, in accordance with the other chemical-physical values, especially water uptake, proton concentration, mobility and λ. The data were compared to λ values to highlight the importance of the bonding among protons, water and functional groups. The same trend was found for conductivity and λ at both the temperatures, meaning that the ratio of water per sulfonic group plays a key role in the conduction mechanism. for s-PEEK-0.77, in accordance with the other chemical-physical values, especially water uptake, proton concentration, mobility and λ. The data were compared to λ values to highlight the importance of the bonding among protons, water and functional groups. The same trend was found for conductivity and λ at both the temperatures, meaning that the ratio of water per sulfonic group plays a key role in the conduction mechanism. Proton conductivity across the membrane can occur mainly by the Grotthuss and the vehicular mechanism. According to the Grotthuss mechanism, protons are transferred from one functional group to another, in a succession of hydrogen bond making and breaking; this "proton jump" determines the reorganization of the surrounding environment, usually with the orientation of the Proton conductivity across the membrane can occur mainly by the Grotthuss and the vehicular mechanism. According to the Grotthuss mechanism, protons are transferred from one functional group to another, in a succession of hydrogen bond making and breaking; this "proton jump" determines the reorganization of the surrounding environment, usually with the orientation of the dipoles of the solvent, and therefore the formation of a proton diffusion path. According to the vehicular mechanism, the proton migration requires the translational movement of larger species, which therefore serve as diffusion vehicles. For example, in an aqueous environment, protons are transported by water molecules. The activation energy is a fundamental tool to better understand which mechanism is predominant during proton conduction. Several papers report activation energy in the range 14-40 kJ mol −1 for Grotthuss mechanism and lower than 14 kJ mol −1 for the vehicular one [54,55]. Since proton conductivity shows an Arrhenius behavior, the activation energy can be roughly calculated for the developed membranes and it is reported in Table 3. Table 3. Activation energy for the developed membranes.
All the data reported so far point to the fact that porphyrins are strongly bound to the functional groups of the polymer, and their amount and reorganization in the polymeric matrix directly affect the proton conduction mechanism. Furthermore, J-aggregates seem to be actively involved in the proton conduction mechanism [31]. All the characterizations above described give us indications on the real applicability of the membranes in a PEFC device. To evaluate their performance and make a comparison among the different porphyrin loaded membranes, the electrochemical characterization in terms of I-V curves was carried out. In Figure 6a the polarization curves of the four membranes obtained at 80 • C and 100% RH are compared. It is evident that s-PEEK-0.77 has the best performance among the investigated composite membranes, in accordance with the chemical-physical parameters, such as proton concentration and mobility, λ and conductivity values. Furthermore, its performance is comparable to the s-PEEK-0 recast membrane. As reported in Table 4, all the investigated samples showed a good OCV value, of about 1 V, comparable or slightly higher than that obtained from s-PEEK recast membrane. This means that the introduction of TPPS increases the OCV value indicating a more dense and compact structural arrangement of the composite membranes, with respect to that obtained by the pristine polymer. In general, the cell resistance of composite membranes is higher than recast one and among the composites the 0.77 wt % amount produces a minor increase (Table 4). In addition, the current density recorded at 0.6 V, typically referred to the ohmic region, highlights that the TPPS load plays a key role in the electrochemical performance.
was carried out. In Figure 6a the polarization curves of the four membranes obtained at 80 °C and 100% RH are compared. It is evident that s-PEEK-0.77 has the best performance among the investigated composite membranes, in accordance with the chemical-physical parameters, such as proton concentration and mobility, λ and conductivity values. Furthermore, its performance is comparable to the s-PEEK-0 recast membrane. As reported in Table 4, all the investigated samples showed a good OCV value, of about 1 V, comparable or slightly higher than that obtained from s-PEEK recast membrane. This means that the introduction of TPPS increases the OCV value indicating a more dense and compact structural arrangement of the composite membranes, with respect to that obtained by the pristine polymer. In general, the cell resistance of composite membranes is higher than recast one and among the composites the 0.77 wt % amount produces a minor increase (Table  4). In addition, the current density recorded at 0.6 V, typically referred to the ohmic region, highlights that the TPPS load plays a key role in the electrochemical performance.   Figure 6b, the effect of the decrease of relative humidity is shown, also highlighting in this case a contribution due to the porphyrin in the structure. In fact, at 100% RH, when the polymer is completely hydrated, the presence of TPPS into the polymeric matrix affects less the proton conduction mechanism. On the contrary, at lower RH, the different porphyrin load and their peculiar arrangement in J-aggregates participate within the membrane conduction channels. As expected, the reduction of humidity level down to 75% RH produces a decrease of the performance and an increase of the cell resistance for all the investigated membranes (Table 4). In particular, s-PEEK-0.77 sample provided the best performance among the three composite membranes, and was comparable to the recast one. As discussed above, this fact could be explained by the participation of porphyrins in the proton conduction mechanism, by making the membrane more hydrated, as can be seen from the data of W up % and λ. This result is in line with data already reported for similar systems. Indeed, previous investigations demonstrated that the physical-chemical properties of TPPS 0.77 wt % sample are related to a good balance between porphyrins in their monomeric and aggregated species. In particular, the extra sulfonated groups of the porphyrin free base enhance the proton membrane conductivity, while an improvement of the mechanical properties is ascribed to the polymer structural re-arrangement, due to the presence of the aggregates [31]. The contribution of TPPS to membrane hydration is still visible when the operative conditions were shifted toward low RH (50%) Figure 7 shows a comparison of the I-V and power density curves for the s-PEEK-0 and s-PEEK-0.77 membranes. For samples containing 0.35 and 1.5 wt % of TPPS, the polarization curves were not recorded, due to poor performance in such drastic conditions. The curves evidence that the reduction of gas humidification affects the electrochemical performance. Indeed, the performance of the s-PEEK-0.77 membrane remains quite unaltered with respect to the 75% RH ones, and it is significantly higher than that of the recast. This effect is due to the different hydration of the membrane, as a consequence of the presence of porphyrin. In particular, the J-aggregate in the composite membrane not only participates in the proton conduction, but also helps to maintain a higher level of hydration. On the contrary, a reduction of RH from 75% down to 50% drastically reduces the performance of the recast membrane, due to the dehydration of the polymer.
conductivity, while an improvement of the mechanical properties is ascribed to the polymer structural re-arrangement, due to the presence of the aggregates [31]. The contribution of TPPS to membrane hydration is still visible when the operative conditions were shifted toward low RH (50%) Figure 7 shows a comparison of the I-V and power density curves for the s-PEEK-0 and s-PEEK-0.77 membranes. For samples containing 0.35 and 1.5 wt % of TPPS, the polarization curves were not recorded, due to poor performance in such drastic conditions. The curves evidence that the reduction of gas humidification affects the electrochemical performance. Indeed, the performance of the s-PEEK-0.77 membrane remains quite unaltered with respect to the 75% RH ones, and it is significantly higher than that of the recast. This effect is due to the different hydration of the membrane, as a consequence of the presence of porphyrin. In particular, the J-aggregate in the composite membrane not only participates in the proton conduction, but also helps to maintain a higher level of hydration. On the contrary, a reduction of RH from 75% down to 50% drastically reduces the performance of the recast membrane, due to the dehydration of the polymer. The power density curves indicate that s-PEEK-0.77 composite membrane reaches a maximum value of 462 mW cm −2 , against a value of 358 mW cm −2 obtained with the s-PEEK-0 sample. It is notable how the presence of J-aggregates in the proton conduction channels keeps the membrane hydrated, preventing the membrane from dry-out effect, even if a drastic reduction of the RH of the reactant gases occurs.

Conclusions
Ion exchange composite membranes based on polyetheretherketone sulfonate (s-PEEK) with a medium DS (50%) and containing different wt percentages (0-1.5 wt %) of porphyrin (TPPS) as a filler have been developed for use as components in polymer electrolyte fuel cells. The successful introduction of the organic macrocycle into the membranes and the characterization of the different species were carried out by spectroscopic techniques.
A complete chemical-physical and electrochemical characterization was performed in order to investigate the effect of TPPS on the properties of the membranes. It was found that the TPPS, in its J-aggregate form, actively participates in the proton conduction mechanism maintaining the adequate water content, even in more drastic conditions of 80 • C and 50% RH. In fact, the introduction of this porphyrin induces a variation of the chemical-physical parameters such as IEC, W up %, λ and [H + ], attributable to the interactions that occur between the sulfonic groups of the polymer and the nitrogen atoms of TPPS.
A maximum in proton conductivity can be found for membrane with 0.77 wt % TPPS loading, in accordance with the other chemical physical characterizations. Moreover, the lowest activation energy (21 kJ mol −1 ) found for this sample points to a conduction mechanism mainly ruled by the Grotthuss model.
The electrochemical characterization in terms of I-V curves highlights the fact that s-PEEK-0.77 has the best performance among the investigated composite membranes, especially when operating in a more drastic conditions (i.e., 50% RH). A maximum power density value of 462 mW cm −2 for the s-PEEK-0.77 was obtained. This finding points to the active role of J-aggregates in the proton conduction channels, keeping the membrane hydrated and preventing the membrane from dry-out effect, even if a drastic reduction of the RH of the reactant gases occurs.