Prabal
Sapkota
a,
Sean
Lim
b and
Kondo-Francois
Aguey-Zinsou
*c
aMERLin, School of Chemical Engineering, The University of New South Wales, Sydney, NSW 2052, Australia
bElectron Microscope Unit, University of New South Wales, Sydney, NSW 2052, Australia
cMERLin, School of Chemistry, University of Sydney, NSW 2006, Australia. E-mail: f.aguey@sydney.edu.au
First published on 15th February 2023
This work reports on the synthesis of a platinum (Pt)–tin (Sn) catalyst supported on Vulcan carbon (VC) for the superior electrooxidation of molecular hydrogen at the anode and electroreduction of molecular oxygen at the cathode of a proton exchange membrane fuel cell. The synthesis was done by using the polyol process. The resulting electrocatalyst with a Pt/Sn mass ratio of 3 (PtSn/VC(3)) demonstrated superior electrocatalytic activity of 3- and 1.4-fold over Pt/VC (synthesized as a reference catalyst) for the reduction of oxygen and oxidation of hydrogen, respectively. The developed PtSn/VC(3) catalyst also demonstrated a greater mass activity of 373 mA mgPt−1, i.e. a 2.4-fold improvement compared to Pt/VC for oxygen reduction. The superiority of PtSn/VC(3) was further confirmed upon operation in a self-breathing fuel cell. A maximum power density of 96 mW cm−2 was observed, i.e. a 45% improvement in terms of power density as compared to Pt/VC. In addition, this new PtSn/VC(3) catalyst demonstrated remarkable stability under accelerated stress test where a fuel cell performance degradation of 9% was observed after 60000 fuel cell cycles with a 85% of maximum power density retention.
Sustainability spotlightThis works addresses the SDG 7 by advancing technologies in the form of better electrocatalysts and fuel cells architectures that can help to ensure the access to affordable, reliable, and sustainable energy and modern energy for all. |
To reduce the amount of Pt in fuel cells two main approaches have emerged along: (1) the alloying of Pt with other elements with the aim to enhance the catalytic activity for ORR with the assumption that alloying leads to an increase in catalytic active sites;2,5 and (2) the development of non-platinum based catalysts. Pt-alloys that have been reported include transition metals such as copper (Cu), nickel (Ni), cobalt (Co) and iron (Fe)4 and the following trend of increasing electrocatalytic activities Pt < Pt3Ti < Pt3V < Pt3Ni < Pt3Fe ≈ Pt3Co has been reported.4,6–8 In this case, the activity of Pt3Co exceeded that of Pt by 3-fold (at 0.9 V vs. SHE 0.1 M HClO4).
Non-platinum based catalysts, mainly include carbon based catalysts: such as carbon (C)/nitrogen (N) composites,9 C/N/Fe4,10 and Fe/Ni/N-graphene.4,11 These catalysts have shown good electrocatalytic activity, for example FeNC, displayed an ORR activity of 2.5 mA cm−2 (at the half wave potential E1/2 = 0.76 V vs. SHE, 0.05 M H2SO4).12
When Pt is alloyed with transition metals, it is expected that the Pt–Pt bond distance is reduced, and this would lead to a decrease in the chemisorption energy of the adsorbates (e.g. O˙ and HO˙) at the active sites and thus improved catalytic activity.13 Alloying Pt with other elements of different atomic sizes (e.g. Co, Fe) are found to increase the surface roughness, and as a result increase the catalytic surface area.14 A weaker adsorption of intercedes species (e.g. HO˙, HOO˙ and O˙) has also been reported as a result of the downshift in the d-band center of Pt upon alloying, and this leads to improved ORR.4,6,13,14 In addition, due to a weaker adsorption of the intermediary species (i.e. O˙, HO˙ and HOO˙) at the catalytic site, the surface of Pt based alloys is less prone to the formation of an oxide layer.2,15
Apart from Pt, other noble metals such as Pd alloyed with Pt, Ru and Ir have also been investigated for ORR. For example, bimetallic Pd0.33Pt0.66 and trimetallic PtPdCu have been found to surpass the performance of Pt by 1.7-fold (at E1/2 = 0.84 V vs. SHE, 0.1 M HClO4) and 4.7-fold (at E1/2 = 0.94 V vs. SHE, 0.1 M HClO4), respectively.16,17
Although Pt plays a crucial role at both the anode and cathode of PEMFCs, considerably less work has been reported on HOR in comparison to ORR. Among the few reports, Pd was alloyed with noble metals such as Ru, Ir 2,18and PdIr showed enhanced electroactivity over Pt by a factor 1.8 (at 0.20 V vs. SHE, 0.5 M H2SO4).18 Similarly, Pt alloyed with Cu showed a 2.4 fold increase in HOR activity compared to Pt (at 0.2 V vs. SHE, 0.1 HClO4)4 and PtP2 (platinum phosphide)/PNC (phosphorous and nitrogen doped carbon) showed a 1.47 fold (0.2 V vs. SHE, 0.1 HClO4) enhancement over Pt/C.19
Despite the excellent performances of some of the alternative Pt alloy catalysts for both the oxidation of hydrogen and the reduction of oxygen, very few of these catalysts have been tested under real fuel cell environments. Accordingly, it is difficult to assess the potential of these catalysts as an alternative to Pt.13 To date, the focus of PEMFCs research has been mainly on vehicular applications. However, the need for better power sources for portable and miniature applications cannot be overlooked. The amount of Pt used in small fuel cell stacks of low power rating is higher (i.e. 0.5 mg cm−2) in comparison to stacks for commercial vehicular application (i.e. 0.25–0.35 mg cm−2);20 and this is driven by the lower operating temperature of small stacks of a few 100 W and the slow reaction kinetics at low temperatures. The need to reduce the amount of Pt in small stacks is thus important.
Herein, we report on a single-step method to make a very active and durable platinum–tin on Vulcan Carbon (VC), noted as PtSn/VC(3) ORR and HOR electrocatalyst.4,21 The catalyst contains a minimum amount of Pt (20 wt%) and is suitable for both the anode and cathode of a PEMFC. Sn has been found to be effective in the decomposition of water and the electrooxidation of ethanol and methanol in fuel cells to produce H+.22–24 Accordingly, we assumed that the addition of Sn to Pt would facilitate the oxidation of H2 as Pt–Sn and PtSnO2 have been reported to be highly active in methanol and ethanol oxidation.25,26 Through theoretical studies, the addition of Sn to Pt was also reported to increase the number of ‘H˙’ adsorption sites and decrease the energy for hydrogen adsorption at active sites (0.5 eV for Pt compared to 0.38 eV for a thin layer of Sn deposited on the surface of Pt).27 In addition to facilitating the oxidation of H2, Sn was also reported to facilitate O2 reduction, for example the introduction of Sn to Pt was found to facilitate the adsorption of O2 at a lower potential (0.45 V vs. SHE) than Pt (0.8 V vs. SHE).28 The formation of SnO2 during ORR is finally assumed to prevent the oxidation of Pt. The latter helps to minimize Pt dissolution and increases the number of active sites for O2 adsorption.24,29 Alloying Sn with Pt was thus expected to enhance its electrocatalytic activity as well as lead to synergistic effects for both HOR and ORR. Accordingly, this work reports on a new catalyst suitable for both ORR and HOR and its performance in a self-breathing PEMFC. To the best of our knowledge, this is among the first attempts to do so. In addition, an accelerated stress test of PtSn/VC(3) revealed a remarkably low fuel cell performance degradation of 9% over 60000 cycles.
For making the fuel cell, 24 mg of as-synthesized catalyst was added to a vial. 125 μL of Milli Q water, 100 μL Nafion 10% in water and 500 μL of 2-propanol were added. The final volume was adjusted by adding 1.5 mL of 2-propanol. The mixture was sonicated for 5 min and left to stir overnight at room temperature.
X-Ray Diffraction (XRD) was performed by using a Philips X'pert Multipurpose XRD system operated at 40 mA and 45 kV and equipped with a monochromated Cu Kα radiation (λ = 1.541 Å). Diffraction patterns were recorded between 15 to 80°. X-Ray Photoelectron Spectroscopy (XPS) was performed by using a Thermo ESCALAB250Xi XPS system operated at 160 W and equipped with a mono-chromated Al K-α (1486.68 eV) X-ray source.
The amount of Pt and Sn in the as-synthesized catalysts was determined by inductively coupled plasma-optical emission spectrometry (ICP-OES) by using an Optima7300DV (PerkinElmer, USA). For this, the materials were digested in acid (3HCl + 1HNO3).
Cyclic Voltammetry (CV) and Linear Sweep Voltammetry (LSV) were performed by using a VMP3-Biologic potentiostat. The potentiostat was connected to a Rotating Disk Electrode (Basi RDE 2) having a 3 electrodes electrochemical cell. Ag/AgCl saturated with 3 M NaCl was used as the reference electrode and a Pt wire as the counter electrode. Freshly prepared 0.1 M HClO4 was used as electrolyte. The catalyst activity reported was determined by subtracting the background measurement and iR correction.
Fuel cell testing was done by using a self-breathing single PEMFC as described in Fig. 1.31 The anode had a mixed serpentine flow field (Fig. 1a), and the opening at the air cathode was 35% of the active area of the cell (Fig. 1c), ∼2 cm2. A silicon gasket was used for sealing (Fig. 1d). Full detailed design of the self-breathing PEMFC can be found in a ref. 31.
Fig. 1 Photo of the self-breathing PEMFC showing the (a) anode, (b) open cathode, (c) MEA, (d) silicon sealing gasket. |
An Accelerated Stress Test (AST) was performed by modifying the protocol proposed by the US DOE and other research groups.32–35 In brief, polarization curves were run between the Open Circuit Voltage (OCV) and 0.4 V, and between each cycle, the potential was held for 3 s at the OCV and 0.4 V. The total number of cycles were 60000 at room temperature (25 °C) with H2 humidified at 20% RH at the anode. Although various AST protocols have been proposed to analyze the durability of Pt/C under fuel cells.32–34,36 Most of these protocols rely on testing under N2 at the cathode for 30000.32 However, higher fuel cell degradation was reported when N2 was replaced by O2/air.33 Testing under O2/air also replicates a more realistic fuel cell environment. In addition, all current testing protocols have been designed for the scenario of vehicular application,32 and do not address the operating conditions of stationary and portable applications. As per our knowledge, there has not been any research in the past where the performance of Pt or Pt alloy catalysts has been observed under AST at low temperature and humidity. So, this work is among the first of its kind to determine the performance of catalysts under self-breathing operation for an extended period. This ensures the practicality of the platinum–tin alloy catalyst reported here.
Characterization of PtSn/VC(3) by TEM revealed particles with an average size of 2 ± 0.3 nm uniformly dispersed on VC as shown Fig. 2. The particles had a d spacing of 0.231 nm and this would correspond to Pt3Sn (111) (Fig. 2c). The d spacing of Pt was 0.223 mm in line with previous reports.39 Increase in d spacing upon alloying Pt with Sn has been reported due to the larger atomic size of Sn(158 pm) as compared to Pt (138 pm).27,40,41
Further, STEM and elemental mapping of PtSn/VC(3) showed an uniform distribution of Pt and Sn ‘co-located’ on the VC support. This suggests that Pt3Sn particles have been synthesized on VC at a Pt/Sn mass ratio of 3 (Fig. S1†).
The XRD of the as-synthesized PtSn/VC(3) is shown Fig. 3. The diffraction peaks are assigned to cubic Pt3Sn. In particular, the diffraction peaks at 38.8 and 65.5° were assigned to Pt3Sn (111) and Pt3Sn (220), respectively. These peak positions are shifted slightly towards lower diffraction angles in comparison to Pt/VC synthesized in a similar manner (Fig. 3). This is in line with previous reports where a slight shift of the peaks towards lower diffraction angles is reported for PtSn/C materials.42,43 Such a shift towards lower diffraction angles suggests the formation of defects due to the formation of vacancies and dislocation as a result of alloying.44 It is noteworthy, that the observed Pt3Sn phase is in line with the Pt–Sn phase diagram (Fig. S2†) where Pt3Sn is formed at a 25% Sn and 75% Pt composition. A small diffraction peak is observed at 33.3° indicating the presence of Sn and this is assumed to be due to some Sn particles directly forming at the surface of VC.45 There is a possibility that isolated Pt particles would also have formed but their diffraction peaks would overlap with the peaks of Pt3Sn.46 The diffraction peaks at 39.8 and 67.5° are assigned to cubic Pt (111) and Pt (220), respectively. Further characterization of the as-synthesized PtSn/VC(3) by XPS is shown Fig. 4. The binding energies of Pt 4f, i.e. 71.8 and 75.1 eV are shifted by 0.7 and 0.4 eV, respectively compared to the Pt/VC (Fig. 4a and S3†). This shift to higher binding energies can be attributed to a transfer of electron from Sn to Pt as expected upon the formation of a Pt–Sn bond.47–50 Sn/SnO2 peaks were not observed by XPS and this could be due to the overlapping of these peaks (485.8–486.7 eV) with the Pt3Sn peaks (487.2 eV).51,52
Alloying also increases the d vacancy and lowers the Fermi level of Pt.49,50 Similarly, the binding energies 487.2 and 495.7 eV in the Sn 3d spectrum could be assigned to the formation of a Pt3Sn alloy.47,53 Accordingly, the XPS results are in agreement with the observations made by XRD and confirmed that no isolated Pt particles were formed at the surface of VC.
Under saturated H2, the HUPD was very pronounced in the range 0.05–0.3 V and the CV profile displayed much larger currents due to the occurring HOR. This increase in current density for PtSn/VC(3) in comparison to Pt/VC clearly indicates that PtSn/VC(3) is a good HOR catalyst (Fig. 5 and S4a†). The enhanced HOR performance of PtSn/VC(3) can be explained by considering the theoretical reports predicting that alloying Sn with Pt would result in a decrease in the adsorption energy of H2 at the Pt–Sn surface by ∼0.12 eV in comparison to Pt. Alloying is also assumed to provide more active sites for H2 adsorption owing to the “uneven surface” formed upon alloying Pt with Sn because of Sn larger atomic size (158 pm) as compared to Pt (138 pm).27 This better HOR performance of the PtSn/VC(3) was further confirmed by LSV (Fig. 5b), where hydrogen oxidation at PtSn/VC(3) started at a marginally lower potential (∼13 mV vs. SHE) than on Pt/VC. The broader LSV peak in the case of PtSn/VC(3) could be due to accumulation of hydrogen at the working electrode,58 in agreement with previous observations.59,60
It has been predicted by theoretical calculations that when Sn is alloyed with Pt, the ‘O˙’ hydrogenation reaction (O˙ + H˙ → OH˙) would occur with a lower activation barrier of 0.66 eV for Pt3Sn as compared to the 0.77 eV for Pt.61 This would facilitate the formation of H2O during ORR.
The influence of Sn/Pt ratios on the morphology of the Pt–Sn particles was further investigated by TEM (Fig. S8–S9†). In all the materials, the Pt–Sn particles were well dispersed on VC and the particle size increased from 1.5 ± 0.3 to 3.5 ± 0.5 nm with higher amounts of Sn (Fig. S9†). This can be explained by the faster reduction of Pt in comparison to the Sn precursor, and the associated nucleation and growth mode. Indeed, increasing amounts of SnCl2 would result in a prolonged generation of Sn nuclei and eventually leads to further particle growth.69Table 1 summarizes the composition of the catalysts and their average particle size.
Catalyst | wt% of metals | at% of metals | Average particle size (nm) | ||
---|---|---|---|---|---|
Pt | Sn | Pt | Sn | ||
Pt/VC | 19.6 | 0 | 100 | 0 | 1.5 ± 0.3 |
PtSn/VC(3) | 19.4 | 6.8 | 83 | 17 | 2 ± 0.3 |
PtSn/VC(1.5) | 19.8 | 13.9 | 62 | 38 | 2.5 ± 0.5 |
PtSn/VC(1) | 19.6 | 19.8 | 52 | 48 | 3.5 ± 0.5 |
Fig. 7 Activity comparison at various Sn/Pt ratios, (a) HOR activity @ 0.2 V vs. SHE, (b) ORR activity @ 0.85 V vs. SHE. These values were determined from LSV (Fig. S10 and 11†) in 0.1 M HClO4 under saturated (a) H2 and (b) O2, at a scan rate of 10 mV s−1 @1600 rpm. The catalyst loading was 50 μg cm−2. |
PtSn/VC(3) also showed better performance in terms of mass activity (373 mA mgPt−1) for ORR, which is higher than Pt/VC (153 mA mgPt−1) (Fig. S14†). The number of electrons involved during ORR was found to be 3.92 for PtSn/VC(3) and this indicates that the ORR could occur along the four-electron path (Fig. S15 and 16†). The ORR can follow a four-electron path that leads to the formation of H2O (reaction 1) or a two-electron path leading to the formation of H2O2 (reaction 2). H2O2 has a detrimental effect on the proton conducting membrane, because it leads to its oxidation and thus premature degradation. Upon the two-electron path, the fuel cell potential also decreases to 0.68 V, which is almost half of the potential (1.23 V) of the four-electron path.4,71
O2 + 4H+ + 4e− → 2H2O (E° = 1.23 V) | (1) |
O2 + 2H+ + 2e− → H2O2 (E° = 0.68 V) | (2) |
The best performing PtSn/VC(3) was further analyzed for stability by conducting an accelerated stress test (AST) within the self-breathing PEMFC. The resulting polarization curves up to 60000 cycles are shown Fig. 9a. The performance loss after 60000 cycles was only 9% (at 150 mA cm−2), while one-third of the loss occurred during the first 10000 cycles. 85% of the maximum power density was retained after 60000 cycles (Fig. 9b).
The decrease in the performance (4.3%) in the low current density region (<50 mA cm−2) was expected owing to the normally occurring initial ‘loss’ in catalytic active sites.34 However, at high current (>100 mA cm−2) mass transfer losses (mainly O2 and H2O) have been reported to limit performance.34 Accordingly, the performance degradation of 9% (at 150 mA cm−2) observed at higher current density is assumed to be due to an initial ‘loss’ in catalytic active sites in addition to some mass transport limitations.34
A stable performance under AST proves the capability of these PtSn/VC(3) catalysts to be operated under abrupt load conditions. The maximum power density after 60000 cycles decreased by 15% in comparison to the first cycle. In a recent work, a performance degradation of 15% after 30000 cycles was reported with the PtCu/VC catalyst.72 This work cannot be directly compared with other ASTs done at 80 °C, 100% RH and N2 at the cathode due to the unique nature of self-breathing operation, however, ASTs on conventional PEMFCs operated with H2, air at 80 °C and 80% RH with a Pt Ketjenblack catalyst showed a degradation of 6% after 10000 cycles at 100 mA cm−2.35 A higher performance degradation of 12% (at 100 mA cm−2 after 10000 cycles 35and 20% (at 220 mA cm−2 was also reported after 1000 cycles for Pt/C in conventional PEMFCs.73 The results reported here are thus superior to earlier reports in the literature.35,73 A performance degradation of 50 mV for PtSn/VC(3) after 60000 cycles is remarkable as a maximum degradation of 30 mV is the target set by the US Department of Energy after 30000 cycles.32
It is thus apparent that alloying Pt with Sn leads to superior electrocatalytic activity for the electrooxidation of molecular hydrogen and the electroreduction of molecular oxygen at the anode and cathode of the fuel cell, respectively. The electrocatalytic activity and mass activity improved by 2 and 2.5-fold, respectively, against Pt. This improved performance over Pt/VC is assumed to be due to a change in binding energy of intermediate species such as HO˙, HOO˙ and O˙ on the PtSn/VC(3) surface. Alloying is also assumed to lead to an increase in the d-vacancy of Pt and, as such, an enhanced catalytic activity.
Successful application of these catalysts at both the anode and cathode of the self-breathing PEMFC demonstrates their appropriateness at the MEA of a PEMFC. There are very few instances in the literature where Pt-alloys were successfully used at the anode and the cathode of PEMFCs, among which a MEA developed with a Pt7Cu demonstrated a power density of 45.16 mW cm−2. This corresponds to 1.4-fold output power increment over Pt operated under similar conditions.4 Future work would aim at understanding the degradation mechanism under fuel cell operation.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2su00129b |
This journal is © The Royal Society of Chemistry 2023 |