Ramanujam Kannanab,
Hye-Ri Jangb,
Eun-Sil Yoob,
Hong-Ki Leec and
Dong Jin Yoo*ab
aR&D Education Center for Specialized Graduate School of Hydrogen and Fuel Cells Engineering, Chonbuk National University, Jeollabuk-do 561-756, Korea. E-mail: djyoo@jbnu.ac.kr
bGraduate School, Department of Energy Storage/Conversion Engineering, Hydrogen and Fuel Cell Research Center, Chonbuk National University, Jeollabuk-do 561-756, Korea
cHydrogen Fuel Cell Parts and Applied Technology Regional Innovation Center, Woosuk University, Jeollabuk-do 565-902, Korea
First published on 7th April 2015
The development of an efficient catalyst for proton exchange membrane fuel cells is presently a challenging and pressing need. Enhanced activity is expected to occur if the interactions between the catalytic metal and the support are improved. Herein, we report the eco-friendly green solid state synthesis of palladium quantum dots@carbon on mixed valence cerium oxide nanoparticles/reduced graphene oxide hybrid (PdQD@C–CeOx/RGO) nanocomposites. We also detail their notable performance in the electrocatalysis of ethylene glycol and water in alkaline medium. The palladium nanoparticles, which are 2–5 nm in size, are formed in a fast manner. In terms of catalytic activity, the low-quantity palladium nanoparticle (5 wt%)@carbon–cerium oxide/reduced graphene oxide on the electrode exhibits the highest forward anodic peak current density (10 mA cm−2) compared with the Pd/CeOx and Pd/RGO nanocomposite electrodes. The cerium oxide/reduced graphene oxide functions as both the support and in assisting the electrooxidation reactions towards removal of poisonous intermediates formed during the electrooxidation of ethylene glycol. This work could provide new insights into the simple fabrication of high-performance catalytic electrodes for fuel cell applications.
As a result, attempts have been made to find an alternative to methanol. Ethylene glycol (EG) has been suggested as an alternative energy carrier for fuel cells due to its high energy density, higher boiling point, low vapour pressure, non-toxicity, extensive availability from renewable sources, and its relatively effortless transport and storage.11,12
Recently, nanostructured metal catalysts have found extensive application in fuel cell electrocatalysis. The development of an active electrocatalytic system is challenging. Recent studies have found that platinum (Pt) is one of most effective catalysts for direct alcohol fuel cells (DAFCs).13–15 However, platinum's high cost, limited availability, and propensity to generate intermediate poisonous compounds during the electrooxidation process represent serious drawbacks. Therefore, reducing the dependence on Pt by developing a Pt-free catalyst would likely be advantageous. Palladium (Pd) and Pd-based catalysts have been considered as suitable catalysts for DAFCs and could be used as a potential substitute for Pt. In addition, Pd is comparatively inexpensive and more abundant compared to Pt. Pd and Pt also exhibit almost identical electrocatalytic performance towards DAFCs.13–16
Supported metal catalysts exhibit enhanced catalytic activity and stability compared to unsupported catalyst. Typically, the support material provides an improved physical surface for the metal catalyst, resulting in an improved surface area that allows for the maximum number of catalytic centres to be available for the reaction.17–20 Traditionally, different types of conductive carbon black (Vulcan XC, Ketjen Black, and Denka Black) have been used as the support material for noble metals in electrochemical reactions.4,20 To improve the electrical conductivity and surface area, carbon nanotubes, carbon nanofibers, and graphene have been used as support materials.4,15,20,21
Graphene is a thin, nanostructured material with sp2-hybridized carbon atoms arranged in a honeycomb lattice. Recently, graphene-based materials have attracted considerable attention in energy fields due to their multitude of beneficial properties such as high surface area, high electrical conductivity, and good thermal and mechanical stability. These unique properties have facilitated the use of graphene in energy storage and conversion applications. In the recent past, graphene-based materials have been used as the support material for precious metal nanoparticles in the fields of energy conversion (especially for fuel cell electrocatalysis).4,20,21 Consequently, efforts were made to develop size-confined metal nanoparticles/graphene composites for electrocatalytic energy conversion and biosensing applications.21–24
Additionally, metal oxides are considered to be an emerging catalytic support material for PEMFCs. Due to their high surface area, high thermal and mechanical stabilities, easy synthesis, and their ability to be converted into any form, these materials are very versatile. Some metal oxides, such as TiO2, MnO2, SnO2, NiO, CeO2, etc., have been tested as support materials for DAFCs.18–20,24–27 However, these metal oxides suffer from lower conductivities, which cause the overall energy output to decrease. To overcome this shortcoming, these metal oxides have been composited with carbon materials such as carbon black,24,25 carbon nanotubes,28,29 graphene oxide,28–30 etc., in order to develop supports that will help to synergistically enhance DAFC performance.30–41 Additionally, the strong interaction between the metal catalyst and the support plays a significant role in electrode performance.4,20,24,30,31
With this in mind, we have attempted to synthesize graphene oxide/ceria supported palladium quantum dots@carbon hybrid nanostructures for the efficient electrocatalyst of ethylene glycol oxidation. With the aim to provide active oxygen species to the catalyst, ceria has been chosen as an additional support. In addition, this facile approach improves the interaction between the catalytic metal and the support by developing in situ carbon. The influence of the support material (graphene oxide/ceria) and the in situ generated carbon on the electrooxidation of ethylene glycol and water electrolysis are studied in an attempt to reduce the noble metal content while simultaneously maximizing catalytic performance.
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Fig. 1 Powder X-ray diffraction spectra of (a) CeOx, (b) GO, (c) Pd QDs–CeOx/RGO, and (d) PdQDs@C–CeOx/RGO hybrid nanostructures. |
The generation of Pd QDs over the support was achieved by an eco-friendly, solid state method using ascorbic acid (AA) as the reducing agent. AA is beneficial compared to common reducing agents, such as borohydride, hydrazine, etc., because these reducing agents are not environmentally-friendly and reactions with these reductants can be very fast or uncontrollable. Conversely, AA is a mild reducing agent and its reactions can be easily controlled. In addition, the oxidized and/or unoxidized reductant serves as the carbon source; these carbon supports are expected to enhance the interaction between the metal catalyst and the support material. The improved metal catalyst and support yield enhanced mass transfer and maximize the catalytic utilization.24,31
X-Ray photoelectron spectra analyses were carried out to investigate the surface chemical states of C, O, Ce, and Pd species in the PdQDs@C–CeOx/RGO hybrid catalyst. Fig. 2 shows the deconvoluted C1s XPS spectrum of the PdQDs@C–CeOx/RGO hybrid, in which the peak at the binding energy of C1s is observed at ca. 284.4 eV. This feature can be further separated into four peaks at 284.31, 284.58, 286.02, and 288.80 eV, which correspond to C–C/CC, C–C, C
O, and C–O, respectively. The PdQDs@C–CeOx/RGO exhibits two major peaks at 335.5 eV (Pd3d5/2) and 340.5 eV (Pd3d3/2), indicating the formation of metallic Pd nanoparticles. The deconvoluted O1s spectrum exhibits peaks at 529.1 eV, 530.3 eV, and 531.6 eV, corresponding to lattice oxygen, O22−/O−, and OH− of the CeOx material. In addition, a peak at 533.1 eV is also observed,24,42,43 which indicates that the carbon material is formed/derived from an organic precursor (i.e., ascorbic acid). The deconvoluted Ce3d core-level spectrum is presented in Fig. 2. Major peaks were observed at 917.2 and 906.8 eV, corresponding to Ce(IV). Ce(III) also exhibits features at 904.2 eV, 886.2 eV, and some other less intense peaks. Because the Ce3d level signals come from a very complicated satellite structure, their definite bands have yet to be concluded.39 The wide range of XPS profiles shown in this study make it clear that the Ce4+ and Ce3+ oxidation states exist in the PdQDs@C–CeOx/RGO hybrid catalyst.
Fig. 3 shows the Raman spectra of (a) RGO, (b) CeOx/RGO, and (c) PdQDs@C–CeOx/RGO hybrid nanostructures.
The Raman spectra of the RGO (Fig. 3a) exhibits two characteristic peaks at 1359 cm−1 and 1593 cm−1, which correspond to D and G bands, respectively. These peaks have an intensity ratio (ID/IG) of 0.9901.24 The CeOx/RGO exhibits three peaks at 454 cm−1, 1359 cm−1, and 1593 cm−1, which match with the CeOx, D, and G bands of RGO, respectively (Fig. 3b). The main peak at 454 cm−1 is attributed to the F2g vibrational mode of CeOx, which is the Raman active mode of CeOx. In general, the defect free (single crystal) CeO2 exhibits a Raman band at 466 cm−1.44,45 However, the CeOx/RGO shows a peak at 454 cm−1 instead of at 466 cm−1. This shift is attributed to the occurrence of defects and the smaller particle size of CeOx. Additionally, as can be seen from the PdQDs@C–CeOx/RGO Raman spectra shows a peak at 610 cm−1 (Fig. 3c), attributes to the intrinsic oxygen vacancies of the CeOx. The reduced intensity of the CeOx Raman band is associated with reduced particle size of CeOx and the increased D band (RGO) intensity than G band, is presumed to the formation of carbon materials over the CeOx/RGO. This was further confirmed the Raman spectra for Pd over CeOx/RGO heated before and after microwave heating (Fig. S3†), the sample before microwave irradiation shows higher G band than D band, on the other hand after heating the ID is comparatively higher the IG indicates the formation of carbonous material.24
The surface morphologies of the prepared materials were analysed by transmission electron microscopy (TEM). As seen in Fig. 4a, the few layers of the graphene sheets were clearly observed. As seen from Fig. 4b, the CeOx particles formed like oval shaped particles on the graphene sheets. The CeOx particle size about 20 nm. Pure CeOx exhibits an almost identical morphology (Fig. S4†). The high resolution TEM images show (Fig. 4d and e) that the PdQDs with black coloured spherical shaped and CeOx nanoparticles are also spherical morphology with the particle size of about 10 nm were uniformly distributed over the RGO. In addition to that the fringes patterns of CeOx nanoparticles are also shown clearly in Fig. 4e. The particle size of the PdQDs ranges between 2 and 5 nm (Fig. 4f). This clearly indicates that AA effectively reduced both the Pd and CeOx. As-prepared PdQDs@C–CeOx/RGO was further analysed by high-angle annular dark-field (HAADF) imaging using a scanning transmission electron microscope (STEM) equipped with an energy dispersive X-ray analyser. The HAADF-STEM image shows (Fig. S5†) the wide distribution of Pd and CeOx nanoparticles over the graphene sheets. The line scan indicates that the Pd and CeOx catalyst QDs are present individually as well as present in the arrangement where the Pd QDs are over the CeOx (Fig. S5†).
The stability of the PdQDs@C–CeOx/RGO catalyst was analysed by thermogravimetric analysis (TGA) between room temperature and 800 °C under a nitrogen atmosphere. As seen from Fig. 5a, the GO exhibits a major weight loss between 100 and 200 °C, indicating the removal of the oxygen-containing functional groups present in the GO. Another major weight loss, of about 90%, occurred at 220 °C, indicating that more oxygen-containing functional groups were removed.46 The TGA curve for CeOx shows that the material is highly stable until a significant transformation in the structure was observed at 700 °C. A significant difference was observed between the Pd–CeOx/RGO (Fig. 5c) and PdQDs@C–CeOx/RGO nanostructures (Fig. 5d), although both materials do exhibit surface and layered oxygen losses around 200 °C. The Pd–CeOx/RGO exhibits an additional weight loss around 300 °C, indicating the removal of organic materials. This suggests that the oxidized/unoxidized AA is eliminated at this point. Alternatively, the PdQDs@C–CeOx/RGO material shows a major weight loss around 450 °C, indicating the presence of carbon in the catalyst. This improved thermal stability is due to the presence of the Pd and CeOx nanoparticles. The higher weight loss of Pd QDs@C–CeOx/RGO is presumed to be caused by the presence of the carbon materials, which formed over the catalyst, and begin to degrade around 400 °C. The content of the carbon material is higher in the PdQDs@C–CeOx/RGO compared to the Pd–CeOx/RGO.
Fig. 6B shows the CVs of electrooxidation of 0.5 M EG in a 1 M KOH solution on the PdQDs@C–CeOx/RGO hybrid catalytic electrode in the scan range between −1.1 V and +0.2 V (vs. SCE). The EG electrooxidation promoted by the PdQDs@C–CeOx/RGO is characterized by two well-defined peaks, which are observed during the forward and backward scans. These peaks are attributed to the electrooxidation of EG (during the forward scan, Of) and the re-oxidation of the intermediates formed during the forward sweep (during the reverse scan, Ob). For comparison, the Pd/C, Pd/RGO, Pd/CeOx, and Pd/CeOx/RGO electrodes were tested for their EG electrooxidation.
These results indicated that the PdQDs@C–CeOx/RGO electrode exhibited the highest activity. The degree of EG electrooxidation at various electrodes was analysed by the forward (If) and backward (Ib) peak current density ratios. The If and If/Ib of the Pd–RGO/CeOx is much higher than those of the Pd/C, Pd/RGO, Pd/CeOx, and Pd/CeOx/RGO catalysts (Table 1). This indicates that the electrocatalytic activity of the PdQDs@C–CeOx/RGO is clearly higher than those of the other electrodes.
A good catalyst exhibits a lower onset potential of the electrooxidation reaction and plays a significant role in accessing electrocatalytic activity. The onset potential can be estimated by looking at the potential at which the deviation from the baseline occurs in the forward oxidation peak. As seen in Fig. 6C, the electrocatalytic reaction at PdQDs@C–CeOx/RGO starts at −055 V, which is a comparatively lower onset potential compared to the other electrodes, indicates the presence of a greater number of available active sites on the electrode surface. This causes more fuel/electrolyte to approach the electrode surface, facilitating the electrocatalytic reaction.
It is generally accepted that the electrooxidation of alcohols can be poisoned by intermediates [M(CO)ads] that are produced during the forward scan (eqn (1)–(4)), which suppress electrocatalytic activity.2,3 To overcome this, we extended the Eupper range, step by step, from +0.2 V to +1.0 V. This resulted in a gradual decrease in Ib and no change in If. At the higher scanning range (+1.0 V), an insignificant Ib was noticed. In addition, a new oxidation peak was observed at +0.5 V (Of2). This lowered Ib and Of2 indicate that the intermediates were oxidized during the forward sweep itself (Fig. 7B).
2 Pd + CH3OH ⇒ Pd(CH3O)ads + PdH | (1) |
Pd(CH3O)ads + Pd(OH)ads ⇒ Pd2(CH2O)ads + H2O | (2) |
Pd2(CH2O)ads + Pd(OH)ads ⇒ Pd3(CHO)ads + H2O | (3) |
Pd3(CHO)ads + Pd(OH)ads ⇒ Pd2(CO)ads + 2Pd + H2O | (4) |
The oxidation of this strongly bonded intermediate species requires highly active oxygen atoms. Such oxygen atoms may not be available until Eupper = +0.2 V.
As the Eupper is increased, highly active oxygen atoms become available and gradually oxidize the intermediate species As the Eupper is gradually increased above +0.2 V, the catalytic support (CeOx) generates active oxygen; the concentration of active oxygen is directly associated with the Eupper. This active oxygen will help to oxidize the intermediates formed throughout the course of EG electrooxidation.
The maximum potential at which the oxygen evolution reaction (OER) occurs is +1.0 V. This results in the effective oxidation of the intermediates that form on the electrode surface. The enhanced active oxygen generation results from the combined effects of RGO/CeOx. In addition, CeOx is prepared by a low temperature method, so it is enriched with surface oxygen that contains more surface defects. At higher potentials, the CeOx combines with the hydroxyl to generate active oxygen, which is highly energetic and subsequently oxidize the intermediates on the electrode surface (eqn (5) and (6)).
For methanol oxidation, similar activity was observed (Fig. 7C). We have tested methanol oxidation at higher potentials; the backward oxidation current decreased progressively and the maximum reduction of the poisonous intermediates became oxidized when the Eupper reached +0.8 V. Above this potential (Eupper = +0.8 V), PdO formation was higher (confirmed by the observation of an oxygen reduction peak).
Potential ≤ +0.2: Pd@C–[Ce–OVacancy–Ce] + OH− ⇒ Pd@C–[Ce–O–Ce] + H+ | (5) |
Potential ≥ +0.2: Pd@C–[Ce–O–Ce] + OH− ⇒ Pd@C–[Ce–OVacancy–Ce] + [O]active + H2O | (6) |
By comparing these results with Pd/RGO (for Eupper = +0.6 V), the Ob peak current is seen to decrease significantly (Fig. S6†). Alternatively, when the Eupper > 0.6 V, a drastic reduction of the Of peak current was observed. It indicates that the gradually above the forward oxidation peak current reduced significantly. This indicates that the electrode is inactive. We presumed that at higher potentials Pd oxidized into PdO. These oxidized species are less catalytically active than the unoxidized Pd. Therefore, the electrocatalytic activity was reduced/suppressed. From these results, it is clear that the CeOx plays a significant role and acts synergistically enhance the activity of the catalyst. The possible reaction that occurs on the PdQDs@C–RGO/CeOx electrode surface is given by Scheme 1.
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Scheme 1 Reaction sketch for the synergism of CeOx during the oxidation of intermediates on the Pd QDs surface. |
The electrooxidation of methanol and ethylene glycol exhibit similar electrochemical activities. These results indicate that an improved electrocatalytic activity for ethylene glycol oxidation was achieved by using the RGO/CeOx. The RGO/CeOx acts as both the support as well as the co-catalyst and act as bifunctional catalyst. The present solid state method for grafting noble metals onto the support material represents a new, fast way to develop nanocatalysts with improved electrocatalytic performance. The in situ generated carbon will help to enhance the interaction between the catalyst and the support. Additionally, supported ternary nanocatalysts exhibit improved catalytic activity with small quantities of noble metals (5 wt% Pd); in this way, the cost of the catalyst can be reduced. The present work is expected to provide a simple and novel way to produce metallic QDs and improve interaction with the support. These materials have the potential to be utilized extensively in energy (fuel cell) applications.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra04226g |
This journal is © The Royal Society of Chemistry 2015 |