Guangjun Ran,
Qiang Fu and
Weilin Xu*
State Key Laboratory of Electroanalytical Chemistry, Jilin Province Key Laboratory of Low Carbon Chemical Power, Changchun Institute of Applied Chemistry, Chinese Academy of Science, 5625 Renmin Street, Changchun 130022, P. R. China. E-mail: weilinxu@ciac.ac.cn
First published on 26th January 2015
A simple custom-made microfluidic reactor is used to synthesize Pt nanoparticles supported on carbon (Pt/C) as electrocatalysts for fuel cells. By varying the flow rate of reactant in the microfluidic reactor, Pt/C catalyst obtained with a flow rate of 90 μL min−1 of substrate was found to be optimal for both anode and cathode electro-catalytic reactions (oxygen reduction reaction (ORR), methanol and formic acid electro-oxidation). An optimal size of Pt nanoparticles was found to be about 2.8 nm. This microfluidic reactor provides a versatile and portable approach to the large-scale synthesis of uniformly-dispersed carbon supported precious metal catalysts with high performance for fuel cells. The preparation is portable, versatile, fast and energy efficient, and can be a general method for the preparation of other supported metal and alloy systems.
The as prepared carbon supported Pt (Pt/C) catalysts could have different morphology, size and catalytic activity due to a wide variety of preparation methods, such as impregnation, ion exchange, chemical vapor deposition, etc.15–17 Microfluidic synthesis is a micro-reaction technology developed in recent years.18 Compared with conventional synthetic methods, microfluidic reactor has advantages, such as a higher rate of mass transfer and heat transfer, shorter mixing time, continuous reactions and low reagent consumption, etc.19 In addition, their narrow reaction channels and customized mixing geometries can provide very precise control over the timing of reagent addition and improved thermal transport properties, two factors that strongly influence the monodispersity of the product nanomaterials.19–23 Recently, the morphology- and size-controlled synthesis of nanoparticles through microfluidic reactors has caused extensive concern.24–28 Lee et al.29 demonstrated a microfluidic approach to synthesize platinum nanoparticles, which were applied to create a hierarchical catalyst by coating the surface of the magnetic silica nanospheres. Baumgard et al.30 prepared Pt nanoparticles by two-step process using micro-structured devices continuously. The size of Pt-nanoparticles formed inside the microstructures can be controlled by the NaOH/Pt ratio. Luty-Błocho et al.31 reported a synthesis of platinum nanoparticles and their deposition on the active carbon fibers in one microreactor cycle. In this way, the synthesis of platinum nanoparticles and the deposition on support of carbon fibers were separated. However, the microfluidic reactor-based one-step synthesis of Pt nanocatalysts supported by active carbon (Pt/C) for fuel cells is rarely reported.
In this study, based on a simple and operable custom-made microfluidic reactor, with NaBH4 as a reducing agent, PVP as a stabilizing agent, a microfluidic method was applied to study the effect of flow rates of substrate on the catalytic properties of obtained Pt/C catalysts for fuel cell reactions systematically for the first time. As a result, the narrower Pt nanoparticles size and size distribution can be obtained in the microfluidic reactor.
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| Fig. 1 (a) Schematic diagram of the microfluidic reactor system; (b) the real image for the setup of the microfluidic reactor system. | ||
| Catalysts samples | Pt content (wt%) | Average particles size from XRD (nm) | Particle size from TEM (nm) |
|---|---|---|---|
| 30 μL min−1 | 9.2 | 3.2 | 3.3 ± 0.6 |
| 60 μL min−1 | 9.1 | 2.9 | 2.9 ± 0.6 |
| 90 μL min−1 | 8.9 | 2.7 | 2.8 ± 0.5 |
| 120 μL min−1 | 8.8 | 2.6 | 2.7 ± 0.6 |
| 150 μL min−1 | 7.6 | 2.4 | 2.5 ± 0.6 |
The XRD patterns of different Pt/C catalysts are shown in Fig. S1.† All these catalysts exhibit the face centered cubic (fcc) structure of Pt with typical diffraction peaks corresponding to Pt (111), Pt (200), Pt (220) and Pt (311).32 The sizes of Pt crystallite on different Pt/C catalysts were calculated based on the Scherrer equations33 with the (220) peak of the Pt nanoparticles. Interestingly, the results (Table 1) show a decrease of size with the increase of flow rate of reactant in the microfluidic reactor.34,35 The decrease of size could be due to the short growth time of Pt nanoparticles in the microfluidic reactor at high flow rate. The higher peak intensity of (111) facet compared with other facets indicates that the exposed surface on Pt nanoparticle surface is mainly the (111) facets. Furthermore, the Pt/C obtained with flow rate of 90 μL min−1 possesses the highest content of (111) facet. Since Pt (111) facet has been known to be the most active surface compared with others due to its low poisoning rate,36 the catalyst obtained with flow rate of 90 μL min−1 may possess the best catalytic performance among these five catalysts due to its highest content of (111) facet.
The morphologies of these five Pt/C catalysts were further characterized with transmission electron microscopy (TEM). As shown in Fig. 2, TEM images and size distributions of Pt nanoparticles on different catalysts show that the average sizes of Pt nanoparticles on these catalysts are around 3 nm (Table 1). A monotonic decrease of size with the increase of flow rate could be seen clearly, consistent with the XRD results (Table 1 and Fig. S1†). Fig. 2 shows that the Pt nanoparticles on all these catalysts are dispersed on the carbon support uniformly. The high-resolution TEM (HRTEM) image shows (Fig. 2f) the Pt nanoparticles on these Pt/C catalysts are crystalline, consistent with the XRD data shown in Fig. S1,† but amorphous in shape.
To quantify the heterogeneity of Pt size distribution, we used a heterogeneity index (h, in percentage, defined as the full width at half maximum of the distribution divided by the average) to measure the relative spread of values of a parameter from its average, which the larger h is the greater heterogeneity the parameter has.37,38 The values of h for these catalysts were obtained as shown in Fig. 3a. A valley-shape dependence of h on flow rates could be observed clearly with minimum located at the flow rate of 90 μL min−1, indicating the Pt/C catalyst obtained with flow rate of 90 μL min−1 has the narrowest particle-size distribution, further implying that the Pt/C catalyst obtained with flow rate of 90 μL min−1 may possess the best performance among these ones obtained with different flow rates.
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| Fig. 3 The flow rate dependence of h (a), EASA (b) and Ep (c) on Pt/C catalysts obtained with different flow rate. (d) The size dependence of Ep on different Pt/C. | ||
In order to confirm the above prediction about the catalytic properties of these catalysts, in the following these catalysts were tested for three different catalytic reactions. Before that, the electrochemically active surface areas (EASA) of these catalysts were obtained through CO stripping since the EASA has been known to be directly related to the catalytic properties of catalysts.39 Interestingly, Fig. 3b shows that the EASA per gram Pt (m2 gPt−1) on Pt/C could be tuned by varying the flow rate of reactant in the channel: with the flow rate increase, the EASA per gram Pt increases gradually first, then reaches a maximum at the flow rate of 90 μL min−1; after that, it goes through a maximum at 90 μL min−1 at higher flow rates. It probably means that 90 μL min−1 is the optimal flow rate among these few since it has been known that the larger the EASA the better the electrocatalyst is.40
Firstly, the electrochemical properties of the Pt/C catalysts for ORR were evaluated in O2-saturated 0.1 M KOH with a scan rate 200 mV s−1 (vs. SCE). In order to consider the effect of EASA on the performance of catalysts, the currents (mA cm−2) were all normalized based on the real EASA (m2) of the catalysts obtained from CO stripping. As shown in Fig. 4a, the oxygen reduction peaks on CV could be clearly observed on these catalysts, while the one with flow rate of 90 μL min−1 shows the highest peak potential (Ep) for ORR at −0.183 V compared with other catalysts (Fig. 3c). The flow rate dependence of Ep observed here is consistent with the EASA shown in Fig. 3b, confirming that Pt/C with higher EASA usually shows better catalytic performance.40 Fig. 3d shows the volcano-shape dependence of Ep on size of Pt nanoparticles, indicating an optimal size (∼2.8 nm) of Pt corresponds to an optimal catalytic activity, the smaller or larger size of Pt nanoparticles will deteriorate the catalytic activity of catalysts.41 Linear sweep voltammetry (LSV) results further confirm this point as shown in Fig. 4b. It shows the onset potential (Eon) on these Pt/C catalysts for ORR varies with flow rates. As depicted in the inset of Fig. 4b, Eon of the catalyst shows a volcano-shaped dependence on the flow rate or size of Pt nanoparticles, which is consistent with those shown in Fig. 3, further confirming the flow rate of 90 μL min−1 is optimal. For comparison, the performance of commercial Pt/C is also shown in Fig. 4; its performance is almost the same as that of the optimal catalyst obtained with flow rate of 90 μL min−1.
To understand the electron transfer kinetics of the optimal catalyst obtained with flow rate of 90 μL min−1 for ORR, we studied its ORR reaction kinetics on a rotating ring-disk electrode. The disk currents of LSV with various rotation rates were given in Fig. S2a.† Koutecky–Levich equation42 was used for analyzing the transferred electron number (n) during the ORR with disk currents.
485 C mol−1), CO2 is the bulk concentration of O2 (1.2 × 10−6 mol cm−3), DO2 is the diffusion coefficient of O2 (1.9 × 10−5 cm2 s−1), ν is the kinematics viscosity of the electrolyte (0.01 cm2 s−1) and n is the transferred electron numbers in the ORR. In the j−1 versus ω−1/2 plot, the slope is 1/B. As shown in Fig. S2b† (at −0.6 V vs. SCE), the number of electrons transferred (n) was calculated from the slope of the Koutecky–Levich plots, by using the above parameters and Koutecky–Levich equation. The number of electrons obtained from the slope is 4.0 for the optimal catalyst, indicating that the ORR is a four-electron process that completely reduces the O2 to H2O on the optimal catalyst.
To further consider the potential effect on the catalytic activity of optimal catalyst, we analyzed the ring-disk currents on the catalyst at different potential. As shown in Fig. S2c and d,† the optimal Pt/C can greatly inhibit the two electron (or H2O2) pathway and make water the main product (four-electron pathway) in the whole wide potential window, indicating a little bit better performance than that of commercial Pt/C.
In order to further confirm the versatility of the prepared catalysts, these catalysts were also tested as electrocatalysts for both methanol and formic acid electro-oxidation. As shown in Fig. 5a for methanol electro-oxidation in 0.5 M H2SO4 + 0.5 M CH3OH, all these prepared catalysts showed obvious methanol oxidation peaks appeared in both the forward and reverse scans. The peak current densities of methanol oxidation are in the order of 90 μL min−1 > 120 μL min−1 > 60 μL min−1 > 30 μL min−1 > 150 μL min−1, which is consistent with as that shown in Fig. 3 or 4b, further confirming that the catalyst obtained with flow rate of 90 μL min−1 is still the optimal one for methanol electro-oxidation. The ratio of the forward anodic peak current density (If) to the reverse anodic peak current density (Ib), If/Ib, can be used to describe the catalyst tolerance to carbonaceous species accumulation. Low If/Ib ratio indicates poor oxidation of methanol to carbon dioxide during the anodic scan and excessive accumulation of carbonaceous residues on the catalyst surface.43 High If/Ib ratio shows the converse case. The large value (1.47) of If/Ib on optimal catalyst obtained with flow rate of 90 μL min−1 (vs. 0.84 on commercial Pt/C) implicates that methanol molecules can be more effectively oxidized to CO2 on the optimal catalyst during the forward potential scan, generating relatively less poisoning species as compared to commercial Pt/C.
Similarly, Fig. 5b shows the catalyst obtained with flow rate of 90 μL min−1 is also the best one for formic acid oxidation compared with others. The reaction on this catalyst commences in the hydrogen region and proceeds slowly during the forward scan. This corresponds to formic acid oxidation through the dehydrogenation path, but the coverage by CO simultaneously continues to grow and causes only relatively small shoulder peak currents at about 0.28 V.44,45 At higher potentials, the current further increases and reaches another peak at 0.67 V. The peak could be attributed to the oxidation of adsorbed CO and formic acid on available active sites recovered by CO removal.45,46 In the reversing the potential scan, the surface remains inactive until partial reduction of the irreversibly formed surface oxides. One huge anodic peak near 0.29 V is observed, and is due to the oxidation of formic acid after reduction of Pt oxides.47 As compared to commercial Pt/C, the formic acid oxidation shifts to lower potential and this indicates superior catalytic activity.44
In order to chemically understand why the optimal Pt/C obtained with flow rate of 90 μL min−1 possesses the highest catalytic performance compared with others, XPS was employed to analyze the valence state of Pt. The XPS spectrum of Pt 4f in the optimal catalyst Pt/C obtained with flow rate of 90 μL min−1 has been de-convoluted and shown in Fig. 6a. The Pt 4f region displays two doublets from the spin–orbital splitting of the 4f7/2 and 4f5/2 states. The most intense doublets (71.3 and 74.4 eV) could be due to metallic Pt(0). The second set of doublets (72.4 and 75.7 eV) could be assigned to the Pt(II) in PtO.7,41 Similarly, de-convolution of the XPS has been carried out for the catalyst obtained with flow rate of 150 μL min−1 (Fig. 6b) which possesses the lowest catalytic activity and the presence of Pt(0) and Pt(II) species are also confirmed by the peaks shown in Fig. 6b. As shown in Table 2, the binding energies of Pt(0) and Pt(II) show almost no difference between different flow rates, indicating the activity difference was not induced by the different chemical states of Pt. According to the TEM images shown in Fig. 2, the activity difference could be mainly attributed to the difference in morphology or size of Pt nanoparticles induced by the different flow rate.48,49
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| Fig. 6 Pt 4f regions of the XPS spectrum: (a) catalyst of 90 μL min−1, (b) catalyst of 150 μL min−1. | ||
| Catalysts samples | B. E. of Pt(0)/eV | B. E. of Pt(II)/eV |
|---|---|---|
| 90 μL min−1 | 71.3/74.4 | 72.4/75.7 |
| 150 μL min−1 | 71.4/74.5 | 72.4/75.7 |
By now, Pt/C catalysts have been extensively prepared with different methods with the control of size, morphology, or density of Pt nanoparticle supported on carbon-based surfaces.4–17,23 However, most of these preparations are based on traditional method without continuity.4,5,8,14,23 With the microfluidic-based method presented here, besides the fine tuning of the size and morphology of Pt nanoparticles supported on carbon, the Pt/C catalyst with optimal performance could be produced continuously with an optimal flow rate in one step simply.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra12145g |
| This journal is © The Royal Society of Chemistry 2015 |