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  • 1
    Online Resource
    Online Resource
    The Electrochemical Society ; 2018
    In:  ECS Transactions Vol. 86, No. 13 ( 2018-07-23), p. 469-474
    In: ECS Transactions, The Electrochemical Society, Vol. 86, No. 13 ( 2018-07-23), p. 469-474
    Type of Medium: Online Resource
    ISSN: 1938-6737 , 1938-5862
    Language: English
    Publisher: The Electrochemical Society
    Publication Date: 2018
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  • 2
    Online Resource
    Online Resource
    The Electrochemical Society ; 2019
    In:  ECS Transactions Vol. 92, No. 8 ( 2019-07-03), p. 515-522
    In: ECS Transactions, The Electrochemical Society, Vol. 92, No. 8 ( 2019-07-03), p. 515-522
    Type of Medium: Online Resource
    ISSN: 1938-6737 , 1938-5862
    Language: English
    Publisher: The Electrochemical Society
    Publication Date: 2019
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  • 3
    In: ECS Transactions, The Electrochemical Society, Vol. 104, No. 9 ( 2021-10-01), p. 17-23
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2021
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  • 4
    Online Resource
    Online Resource
    The Electrochemical Society ; 2022
    In:  ECS Meeting Abstracts Vol. MA2022-02, No. 64 ( 2022-10-09), p. 2377-2377
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2022-02, No. 64 ( 2022-10-09), p. 2377-2377
    Abstract: PEFCs have been attracted as one of the clean and efficient energy conversion systems. Platinum nanoparticles are commonly used as cathode catalysts in Polymer electrolyte fuel cells (PEFCs) due to their high activity for oxygen reduction reaction (ORR). However, platinum is rare and expensive, therefore it needs to improve the mass activity and durability for widespread fuel cells. Recently, ionic liquids (ILs) have been studied to enhance the ORR activity of platinum catalysts 1) . We try to improve the catalytic activity of Pt/C catalysts by using Ionic Liquids (ILs). RTILs are salts that melt at temperatures below 100 o C and generally consist of bulky cations and anions. It has been studied in a wide range of fields, including the energy sector because of its highly conductive and nonvolatile. Recently, it has been reported that ILs layer enhance the ORR catalytic activity on Pt surface, due to the suppress the coverage of OH ad from water molecules 1) . However, the correlation between increased ORR activity and the structure of the ionic liquid has not been clarified. In this study, we focused on ILs quaternary phosphonium cations and a bis(trifluoromethylsulfonyl)amide (TFSA) anion. The phosphonium cations based ILs have been reported to have higher thermal stability than imidazolium or ammonium cations 2) . In addition, the phosphonium ILs show higher electrochemical stability, conductivity, and hydrophobicity than the ammonium ILs. The ORR activity was analyzed using the rotating disk electrode (RDE) method 3) . Commercially available 20 wt% Pt/C (Cabot, Vulcan XC-72R 🄬 ) catalyst was used for bare Pt/C modified electrodes. The Pt/C electrodes were modified with phosphonium ILs (PXXXY + TFSA - [alkyl chain X= 4 Y= 1, 12, 16]). The thickness of the ILs layer was calculated by using the BET surface area of carbon supports. The electrochemical measurements were conducted under Ar or O 2 saturated conditions, respectively. Electrochemical surface area (ECSA) was estimated from hydrogen adsorption wave in cyclic voltammograms (CVs). Mass activity (MA) and surface area specific activity (SA) of ORR at 0.9 V on Pt nanoparticles were calculated from the Koutecky-Levich equation. The ILs layer enhanced ORR activity. However, ORR activity decreased when the ILs layer was excessively thick. These results suggest that the ORR activity decreases in a thicker ILs layer due to increased resistance to oxygen mass transport or proton conductivity. Moreover, the ORR activity of the ILs modified Pt/C catalyst increased as the asymmetric part alkyl chains of the ILs became longer. Our previous reports show that as the size -is larger, both the molar volume and oxygen solubility increases. Our results show that these physicochemical properties originating from the structure of the cation affect ORR activities. [Reference] 1) Gui-Rong Zhang, et al ., ACS Catal. , 8 , 8244-8254 (2018). 2) K. Tsunashima and M. Sugiya, Electrochem. Commun ., 9 , 2353, (2007). 3) H. A. Gasteiger, S. S. Kocha, B. Sompalli, F. T. Wagner, Appl. Catal. B Environ . 56 , 9. (2005).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2022
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  • 5
    Online Resource
    Online Resource
    The Electrochemical Society ; 2019
    In:  ECS Meeting Abstracts Vol. MA2019-02, No. 35 ( 2019-09-01), p. 1562-1562
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2019-02, No. 35 ( 2019-09-01), p. 1562-1562
    Abstract: Polymer Electrolyte Fuel Cells (PEFCs) are expected to be used for automobiles and various applications because of their high power density and low environmental load. To spread PEFCs, improving cell performance is required. One of the factors that lowers cell performance is proton transport resistance in catalyst layers (CLs) which depends on CLs structure. Typical CLs are constructed by carbon supported Pt nanoparticles covered with ionomer thin films. Ionomer thin films have two important roles. First, ionomer thin films work as a binder between carbon black particles. Second, ionomer thin films provide path way for protons, so that proton transport resistance decreases with increasing ionomer carbon ratio (I/C). Oxygen transport resistance is another reason to lower cell performance. In CLs, oxygen transport involves the transport in micro porous media and the permeation through ionomer thin film, thus oxygen transport resistance increases with increasing I/C. To improve cell performance, both protons and oxygen transport resistance need to be low by the optimization of CLs structure. In this study, to analyze the relationship between cathode CLs structure and proton transport property, three-dimensional catalyst layer model is constructed considering carbon black aggregate and ionomer thickness distribution. Mass transport is calculated based on multi-block model considering proton diffusion, oxygen diffusion, water diffusion, and electrical conduction (1). And cathode reaction is calculated by Butler-Volmer equation. Inoue et al. analyzed the relationship between cell performance and CLs structure using the same model. They reported that oxygen transport resistance tends to be dominant for cell performance. However, they didn’t consider ionomer thickness dependence on proton transport property. In our previous study, we analyzed thickness dependence on proton transport properties of ionomer thin films using molecular dynamics (MD) simulations (2). Ionomer thin film was modeled as Nafion and water molecules adsorbed on flat carbon surface. The thickness of films was changed systematically from four nm to ten nm by changing the number of Nafion chains. Diffusion coefficient of protons was calculated with different ionomer thicknesses. It was found that at low water content, proton diffusion coefficients show a peak at the ionomer thickness of around seven nm. In this study, to analyze proton transport phenomena in detail, information about the relationship between ionomer thickness and diffusion coefficient of protons obtained from MD simulations has been introduced to the multi-block model as a correction term. It was found that gradient of I-V curve decreases with increasing I/C considering the correction term. This results suggest that the contribution of proton transport resistance increases considering nanoscale phenomena. In the future work, we will analyze mass transport properties in CLs such as the details of the overvoltage and current density distribution to investigate the relationship between CLs structure and proton transport properties. Acknowledgment This research was supported by the New Energy and Industrial Technology Development Organization (NEDO) of Japan and the Promotion of Science (JSPS) KAKENHI Grant no. 18H01364. We used the integrated supercomputation system at the Institute of Fluid Science. References 1. G. Inoue, N. Ishide, Y. Matsukuma, and M. Minemoto, ECS Trans. , 50(2) , 461 (2012). 2. K. Kobayashi, T. Mabuchi, G. Inoue, and T. Tokumasu, ECS Trans. , 86(13) , 469 (2048).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2019
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  • 6
    Online Resource
    Online Resource
    The Electrochemical Society ; 2019
    In:  ECS Meeting Abstracts Vol. MA2019-02, No. 33 ( 2019-09-01), p. 1458-1458
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2019-02, No. 33 ( 2019-09-01), p. 1458-1458
    Abstract: Introduction Recently, formic acid is expected as one of the energy career for renewable energy. Especially, direct formic acid fuel cells (DFAFCs) which use formic acid as fuel, have received considerable attention since they can generate higher power density than the other direct liquid fuel cells [1]. However, CO 2 gas is generated in the anode reaction when DFAFCs are operating. If CO 2 bubbles stay in the anode gas diffusion layer (GDL) the mass transport resistance in GDL increases and the power generation performance of DFAFCs decreases with the lapse of time. In this study, we have investigated the effect of CO 2 bubble distribution on power generation performance by visualizing the CO 2 bubble distribution in DFAFCs during power generation using X-ray CT. Experimental A single cell with 1 cm 2 of active area was used. We used NR-212 as proton exchange membrane, PEM. Pd/C was used for anode catalyst and Pt/C was used for cathode catalyst. Moreover, two types of GDL with different structures of carbon paper and carbon cloth were used. The voltage sweep was performed at a sweep rate of -5 mV / sec until the cell voltage turned from the open circuit voltage to 0 V, and the cell voltage and current density during the sweep were recorded. A three-dimensional measurement X-ray CT apparatus (TDM-1000H-Ⅱ (2K), Yamato Scientific) was used for visualizing CO 2 bubble distribution in DFAFCs. It took 15 minutes to visualize and the spatial resolution was 2.7 μm. Results and discussion From the measurement of the power generation characteristics, it was found that the maximum current density is higher with carbon cloth GDL than with carbon paper GDL, despite the lower open circuit voltage. In addition, using carbon paper GDL, the gradient of polarization curve became steep in the high current density region. These phenomena are generally considered to be caused by mass transport, and in this experiment it is thought that this is probably due to the effect of bubbles in the anode GDL. Therefore, in order to investigate the influence of bubbles in the anode GDL, visualization was performed. Fig. 1 shows the CO 2 bubble distribution in the anode GDL at high current density operation using each GDL. These figures are three-dimensional representation of the bubble distribution in the anode GDL averaged over 15 minutes of visualization time. Furthermore, these are top views seen from the vertically upward direction of the GDL plane, the white part indicates that bubbles exist. As shown in Fig. 1, using carbon paper GDL, bubbles were present under most of the rib and also present under the channel, which was thought to cause the power generation performance degradation due to the mass transport. On the other hand, with the carbon cloth GDL, there were almost no bubbles under the channel, and bubbles and voids were concentrated under the rib. It is considered that in the carbon cloth, the bubbles were concentrated in part and the discharge path of the bubbles was formed, so that the bubbles were efficiently discharged and the power generation performance did not decrease even in the high current density region. Reference 1) Y. Zhu, Z. Khan, R.I. Masel, Journal of Power Sources , 139, 15-20 (2005) Figure 1
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2019
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  • 7
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2022-02, No. 42 ( 2022-10-09), p. 1541-1541
    Abstract: Polymer electrolyte fuel cells (PEFCs) are expected as one of the clean, highly effective energy conversion systems, and have been actively studied. Pt nanoparticles on carbon supports (Pt/C) are commonly used as a cathode catalyst for PEFCs, because of the high activity on oxygen reduction reaction (ORR). However, its durability in long term driving and high mass activity for ORR have not sufficiently fulfilled at the present. More improvements of Pt/C catalyst for ORR activity and the durability are required for the spread of PEFCs To improve the activity and durability of Pt/C, ionic liquids (ILs) modified catalysts, called Pt/C-Solid catalysis with an IL layer (SCILL) catalysts, have recently attracted much attention [1]. ILs are liquid salts around room temperature, which have high ionic conductivity and electrochemical stability. We focused on hydrophobic ionic liquids with quaternary phosphonium cations [2] . Quaternary phosphonium cations ionic liquids have higher ionic conductivity and hydrophobicity than quaternary ammonium ionic liquids with the same structure and the same counter ions. Because of interference in the oxygen reduction reaction on platinum by water, increasing the hydrophobicity of the surface is expected to improve the activity on Pt/C catalysis. Hence, by using the quaternary phosphonium cations ILs for Pt/C-SCILL catalysts, it promises to improve the ORR activities for the catalyst. On the other hand, proton conduction and oxygen permeation rate are also important factors for ORR activity enhancement. In this study, we report the ORR activity for Pt/C-SCILL catalysts with ILs composed of highly hydrophobic cations and hydrophobic anions. Quaternary phosphonium based ILs (PXXXY+TFSA-[alkyl chain X= 4 Y= 1, 12, 16]) were used for Pt/C-SCILL modified electrodes. Commercially available 20 wt% or 30 wt% Pt/C (Cabot, Vulcan XC-72R 🄬 ) catalyst was used for bare Pt/C modified electrodes. The ultrasonicated Pt/C catalyst suspension was dropped on the mirror polished glassy carbon disk electrodes. Pt/C-SCILL modified electrodes were prepared by recasting the ILs-2-propanol solution on the bare Pt/C modified electrodes or adding ILs to the catalyst suspension. Moreover, the mixture of the ILs and bis(trifluoromethanesulfonyl)imide (HTFSA) were also examined. The thickness of the ILs layer was calculated relative to the BET surface area of the carbon support. A platinum wire and a reversible hydrogen electrode (RHE) were used as the counter and reference electrodes, respectively. CV and LSV were carried out in 0.1 M HClO4 solution under Ar (CV) or O 2 (LSV) atmosphere, respectively. The Pt/C-SCILL catalyst was prepared by recasting (thin layers, ~0.4 nm) or mixing (thick layers, 1nm~) methods. In the case of the thin layer (~0.4 nm) of ILs, the ORR activity increased as the size of the cations increased. However, for the thicker (1 nm ~) ILs layers, the ORR activity was lower than for the bare Pt/C catalysts. It seems that the aprotic ILs interfered with the proton supply, making the four-electron reduction reaction of oxygen less likely to occur. Therefore, we attempted to supply protons to the thick ILs layer by mixing an ionic liquid with a proton source. HTFSA was dissolved in P444(12)TFSA, which showed relatively good ORR activity in thin film studies. The Pt/C-SCILL catalyst was prepared by adding the mixture with a catalyst dispersion. This proton mixing Pt/C-SCILL catalyst showed a significant improvement in ORR activity compared to bare Pt/C catalyst. References [1] S. Silvia et al. , Adv. Energy Sustainability Res. , 2 , 2000062 (2021). [2] K. Tsunashima and M. Sugiya, Electrochem. Commun ., 9 , 2353 (2007).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2022
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  • 8
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2022-02, No. 64 ( 2022-10-09), p. 2393-2393
    Abstract: Ionic liquids (ILs) have characteristic physicochemical properties such as high thermal stability, low volatility, low melting point, and flame resistance. Moreover, ILs exhibit also excellent electrochemical properties represented by a wide potential window.[1] Hence, they have a great potential for electrochemical applications such as electrolytes for batteries, capacitors, fuel-cells and so on. Phosphonium ILs have unique physical characters such as lower viscosity and higher ionic conductivity compared with corresponding structured ammonium ILs.[2] Recently, we have evaluated the diffusion coefficient and the solubility of oxygen molecules in phosphonium ILs and have clarified that such oxygen behaviors strongly depends on the chemical structure of cation rather than that of anions. In the present study, we demonstrated the proton effect for the ORR in phosphonium ILs using rotating ring disk electrode (RRDE) technique.[3] Tetraalkyl-phosphonium(PXXXY + and bis(trifluoromethane sulfone) imide (TFSA - )) ILs were used for electrolytes. Cyclic voltammetry (CV) and convective voltammogram were performed using a three electrode cell at 25 o C. The RRDE constructed a glassy carbon (GC) or platinum (Pt) disk, and Pt ring electrodes were used as the working electrodes. The ring current was measured at a potential of 1.0 V vs. Ag/Ag + reference electrode, where the intermediate oxidation reaction enough attached to diffusion limit. In the non-protonic media, ORR currents were observed from –0.6 V on GC disk electrode and –0.5 V on Pt disk electrode respectively, which were corresponding to the one-electron reduction reaction in ORR. On the other hand, the on-set potential of ORR in protonic media was higher than that in non-protonic media on both electrodes. Such potential shifts were strongly appeared on the Pt disk electrode than that on the GC disk electrode. Moreover, the diffusion limiting current was observed on Pt disk electrode at higher potential region in protonic media, and the current increased with increasing H-TFSA content. Therefore, the limiting current originated from not the transport of oxygen molecules, but that of proton, while the ring current oppositely decreased with increasing H-TFSA content. The ring current originated from intermediate formed on Pt disk electrode was smaller than that on GC disk electrode. These results indicated that the number of electrons in ORR increased by the existence of proton, and the effect of proton was promoted on Pt surface better than the GC surface. [1] A. Khan, C. Zhao, ACS sustainable Chem. Eng. 4 , 506 (2016) [2] K. Tsunashima, and M. Sugiya, Electrochemistry Communications, 9, 2353- 2358(2007) [3] M. Hildera, et al, Electrochimica Acta, 202, 100-109(2016).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2022
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  • 9
    Online Resource
    Online Resource
    The Electrochemical Society ; 2019
    In:  Journal of The Electrochemical Society Vol. 166, No. 13 ( 2019), p. D564-D568
    In: Journal of The Electrochemical Society, The Electrochemical Society, Vol. 166, No. 13 ( 2019), p. D564-D568
    Type of Medium: Online Resource
    ISSN: 0013-4651 , 1945-7111
    RVK:
    Language: English
    Publisher: The Electrochemical Society
    Publication Date: 2019
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  • 10
    Online Resource
    Online Resource
    The Electrochemical Society ; 2020
    In:  Journal of The Electrochemical Society Vol. 167, No. 13 ( 2020-01-10), p. 134502-
    In: Journal of The Electrochemical Society, The Electrochemical Society, Vol. 167, No. 13 ( 2020-01-10), p. 134502-
    Abstract: Direct formic acid fuel cells (DFAFCs) have received considerable attention because they can generate a higher power density compared to other direct liquid fuel cells. However, when generated CO 2 bubbles are retained in the anode’s porous transport layer (PTL), the performance of the DFAFCs deteriorates. The gas–liquid two-phase flow behavior within a PTL is not clear; therefore, in this work the power-generation characteristics of DFAFCs using two types of PTL, carbon paper and carbon cloth, were investigated. It was found that the maximum current density was approximately 60 mA cm −2 higher with the carbon cloth than with the carbon paper. The CO 2 bubble distribution in the anode’s PTLs was visualized by X-ray computed tomography and discuss the effects of the bubbles on the power-generation performance of DFAFCs. We found that interstices in a carbon-cloth PTL provided pathways for bubble migration and release to the channel, so that the bubbles did not deteriorate the power output. Bubble accumulation in a carbon-paper PTL led to a drop in power output, confirming that the structure of the PTL and the CO 2 bubbles affect the power-generation characteristics.
    Type of Medium: Online Resource
    ISSN: 0013-4651 , 1945-7111
    RVK:
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2020
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