Cong
Shen‡
,
Xuemin
Li‡
,
Yajing
Wei
,
Zhenming
Cao
,
Huiqi
Li
,
Yaqi
Jiang
* and
Zhaoxiong
Xie
*
State Key Laboratory of Physical Chemistry of Solid Surfaces & Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, P. R. China. E-mail: yqjiang@xmu.edu.cn; zzxie@xmu.edu.cn; Fax: +86-592-2183360
First published on 29th August 2020
Platinum (Pt)-based catalysts have shown excellent catalytic performance in many fields, particularly for the oxygen reduction reaction (ORR) and direct oxidation of small fuel molecules. Further development of Pt-based electrocatalysts relies on the morphology design of Pt-based alloy nanocrystals (NCs) with highly accessible and active surface sites to optimize Pt atomic utilization. In this work, we reported PtCo-excavated rhombic dodecahedral (ERD) NCs consisting of the self-assembly of 24 ultrathin nanosheets synthesized by a simple wet chemical method. The morphology can be regulated from convex to excavated polyhedra by controlling the amount of formaldehyde and the molar ratio of the Co/Pt precursor. The as-prepared PtCo ERD NCs/C catalyst exhibits excellent ORR performance, which has about 12 times higher specific activity and 6 times higher mass activity than the commercial Pt/C catalyst. It also displays good electrocatalytic ability towards methanol oxidation, in which the specific activity and mass activity are about 6 times higher and 2 times higher than the commercial Pt/C, respectively. Their enhanced activity is attributed to the excavated structure and alloy feature.
However, according to the basic principles of thermodynamics, crystals tend to adopt a convex polyhedral shape with the minimum surface energy, namely Gibbs–Wulff polyhedra. The excavated morphology with negative surface curvature is thermodynamically unfavourable in crystal growth.28,29 Consequently, the majority of PtM alloy NCs obtained to date are convex polyhedra, and only a few concaved/excavated structures have been recently explored. Even though their synthetic methods were roughly classified into a thermodynamic or kinetic approach involved in the use of a capping reagent, selective chemical etching or seed-mediated overgrowth,30–34 the growth mechanism of the excavated structures is still not well understood and the rational synthesis is far beyond our knowledge.
In this work, we successfully synthesized excavated rhombic dodecahedral (ERD) PtCo NCs using a simple wet chemical method. Detailed analysis showed that the excavated structure was constructed from an orderly assembly of 24 ultrathin nanosheets. Both formaldehyde and a molar ratio of Co/Pt play vital roles in constructing this excavated morphology. This unique excavated structure and the alloy nature provide the as-prepared PtCo ERD NCs with a large electrochemically active surface area and an excellent catalytic property towards the oxygen reduction reaction and the methanol oxidation reaction (MOR).
Both as-synthesized PtCo NCs were deposited onto carbon supports (Vulcan XC-72) before the electrochemical tests. Typically, the supernatant of the as-synthesized PtCo NCs was discarded first, and then 5 mL of n-butylamine and 3 mg of XC-72 were added to the samples. The mixed solution was transferred to a bottle with a capacity of 20 mL, and sonicated in an ice-bath for 1 h. After it was magnetically stirred for 3 days (1500 rpm) at 25 °C, the PtCo NCs/C catalysts were collected by centrifugation and washed with ethanol several times.
For the oxygen reduction reaction, the total platinum loading for each experiment was 2 μg. The cyclic voltammogram (CV) curve was scanned until it was stable in a N2-saturated HClO4 solution (0.1 M) with a scan rate of 100 mV s−1 from 0.05 to 1.1 V (vs. RHE). The ORR polarization curve was performed in an O2-saturated HClO4 solution (0.1 M) at a scan rate of 10 mV s−1 and a rotation rate of 1600 rpm. The specific and mass activities were studied at 0.9 V (vs. RHE), and depicted as kinetic current densities normalized to the real active surface area (Q/q0) and the loading Pt mass. For the methanol oxidation reaction, the total platinum loading for each experiment was 3 μg. The CV curve was scanned to a stable profile in a N2-saturated H2SO4 solution (0.5 M) at a scan rate of 50 mV s−1. Methanol oxidation was carried out in a N2-saturated solution of 0.5 M H2SO4 + 0.5 M CH3OH at a scan rate of 50 mV s−1. The ECSA of the catalyst was calculated by the following formula: ECSA = Q/(q0·m), where Q was determined by the area of the hydrogen desorption peaks in the CV measurement performed in the corresponding N2 saturated electrolyte, q0 is 210 μC cm−2, and m is the loading Pt mass.
As mentioned above, the formation of excavated structures is thermodynamically unfavoured. To better understand the formation process, a time-dependent experiment was conducted. The intermediates formed at different reaction times were investigated by TEM and XRD techniques. The TEM images (Fig. S5, ESI†) show that the excavated NCs were formed at the very beginning with an average size of 21.4 nm (Fig. S5, ESI†). After that, the excavated NCs grew large with increasing reaction time. The average size of the ERD NCs was increased to 32.6 nm at 1 h, 36.5 nm at 4 h, and finally 38.4 nm at 8 h. The size was almost equal to that of the final product at 10 h (Fig. 1a). It is noteworthy that the Pt and Co contents of the ERD NCs were maintained at different reaction times. The XRD patterns (Fig. S6, ESI†) show that each diffraction peak of the same diffraction index overlaps at the same two theta angles. These results imply that the excavated structure and the ultrathin nanosheets formed at the very beginning, and grew large with increasing reaction time. Different from selective chemical etching or erosion,10,33 the formation of the as-prepared PtCo ERD NCs in this case probably undergoes a surface capping process, such as the reported excavated cubic PtSn NCs formed in the presence of PVP, and the excavated octahedral PtCo formed with the selective capping of Br− ions.31,32
To figure out the influence factor of the ERD morphology formed at the very beginning, we designed a series of control experiments. When oleylamine was replaced by n-butylamine, n-octylamine or octadecylamine in the presence of 300 μL of formaldehyde, the morphologies of the products are all concave or excavated, which is similar to the product obtained using oleylamine (Fig. 2(a1–c1)). However, the morphologies of the products were all convex polyhedra (Fig. 2(a2–c2)) when formaldehyde was not used in the synthesis system described above. All of the XRD patterns (Fig. S7, ESI†) confirmed that the products are PtCo alloy NCs. In contrast, when the formaldehyde volume was decreased to 100 μL, the obtained NCs were convex polyhedra as well (Fig. S8, ESI†). Upon increasing the dosage of the formaldehyde solution to more than 300 μL, such as 500 μL or 700 μL, the surfaces of the obtained NCs became very rough and the ERD structures collapsed (Fig. S8b and c, ESI†). The uniform and well-defined excavated NCs were produced when using only ∼300 μL of formaldehyde (Fig. 1a). We realized that the formaldehyde solution and the amount used have significant influence on the formation of the PtCo ERD NCs; namely, an appropriate amount of formaldehyde is feasible for constructing polyhedra with negative curvature and forming nanosheets as the building blocks. Few similar phenomena have been found in some related research studies. For example, Zheng and co-workers reported that the concavity of Pd tetrahedra was highly dependent on the amount of formaldehyde added.6 We also found that formaldehyde was a crucial factor in the formation of Rh ultrathin nanosheets in the previous work.37
We further evaluated the other factor affecting the formation of the excavated structure. By changing the initial molar ratio of the Co and Pt precursors, a series of rhombic dodecahedral structures with different concavity degrees appeared (Fig. 3). The XRD patterns shown in Fig. S9 in the ESI† show that all of the formed products are PtCo alloy NCs. The SEM image (Fig. 3a) demonstrates that the convex rhombic dodecahedra formed at a Co/Pt molar ratio of 1:1, while a partial concave structure was formed when the molar ratio was tuned to 2:1 (Fig. 3b). When the concentration of cobalt acetate was further changed to a Co/Pt ratio of 5:1, the result was drastically different. The formed NCs became smaller, and part of them were structurally collapsed (Fig. S10, ESI†). Our experiments reveal that the perfect excavated rhombic dodecahedral morphology can be formed when the Co/Pt molar ratio is about 3:1 (Fig. 3c). In addition, when the Co/Pt ratio reached 5:1, we found an unexpected phenomenon in which the concave PtCo NCs can be formed even in the absent of formaldehyde (Fig. S11, ESI†). From a crystallographic view, a crystal tends to grow a convex polyhedral structure under equilibrium conditions. Therefore, the formation of an excavated structure is more likely to occur in a kinetically controlled process. This will hinder the formation of normal nuclei following the Gibbs–Wulff construction rule. The excessive amount of Co2+ ions accelerates the reduction of Co2+ ions, and is beneficial to co-reduction and the growth of PtCo alloy NCs due to its more negative reduction potential compared to that of the Pt4+ ions.38 We performed a contrast synthetic experiment with or without formaldehyde solution, while keeping the molar ratio of Co and Pt precursor at 3:1 and 1 h of reaction time. As shown in Fig. S12,† no product was obtained (left bottle) without formaldehyde. The solution color is the same as that of an unreacted solution of precursor Co(Ac)2·4H2O. Conversely, the PtCo alloy nanoparticle (black product) can be found in the bottom of the right bottle, in which 300 μL of formaldehyde was added. The results in our case suggest that speeding up the reduction rate of transition metal ions is beneficial to the formation of the concave or excavated structure, and the large Co/Pt initial ratio plays a valuable role.
For comparison, a detailed characterization was conducted for the PtCo alloy NCs obtained without formaldehyde. The large-scale SEM image (Fig. S13a, ESI†) and TEM image (Fig. S14, ESI†) show that the shape of the PtCo alloy NCs is a well-defined rhombic dodecahedral, and the element component calculated from XRD pattern (Fig. S13b, ESI†) is about Pt64Co36. This is very close to that of the as-prepared PtCo ERD NCs. The high-resolution TEM image (Fig. S13c, ESI†) of the single PtCo NC matches well with the schematic model of the rhombic dodecahedron oriented along the [011] direction (Fig. S13e, ESI†). Combining the above results, the morphology evolution of PtCo NCs from a convex RD to an excavated RD is schematically demonstrated in Fig. 3d. It is reasonable to believe that this morphology evolution is induced by the synergetic control of formaldehyde and the molar ratio of Co/Pt.
To evaluate the shape-dependent catalytic properties, ORR (in the cathode of PEMFCs) was studied using three catalysts, PtCo ERD NCs/C, PtCo RD NCs/C and commercial Pt/C. Both PtCo ERD and RD NCs were dispersed on Vulcan XC-72 carbon before measurement. All measurements were performed by making use of the RDE technique, and the loading of Pt on the three catalysts was consistent. The CV curves of different catalysts tested in N2-saturated 0.1 M HClO4 (Fig. S15a, ESI†) show obvious peaks associated with the hydrogen adsorption/desorption process in the potential range of 0.05–0.35 V, and the ECSA of the as-prepared PtCo ERD NCs/C was estimated to be 35.0 m2 gPt−1. The polarization curves (Fig. 4a) show that the PtCo ERD and PtCo RD catalysts have more positive onset potentials than Pt/C, revealing that the adsorption of the oxygenate species on the surface of the PtCo NCs/C catalysts was much weaker and thus more active than Pt/C.39 The kinetic currents at 0.9 V versus RHE were normalized to the real active surface area and the mass loading of Pt to obtain the specific and mass activities, respectively. Fig. 4b demonstrates that the specific activities are 2.68, 1.43 and 0.2 mA cm−2 for PtCo ERD NCs/C, PtCo RD NCs/C and commercial Pt/C, respectively, and the mass activities are 0.94, 0.54 and 0.17 A mgPt−1 for PtCo ERD NCs/C, PtCo RD NCs/C and Pt/C, respectively. Among the three catalysts, the as-prepared PtCo ERD NCs/C catalyst exhibits superior ORR performance over the commonly used commercial Pt/C in terms of both specific activity (∼12 times higher) and mass activity (∼6 times higher). Notably, we found that the activity of the as-prepared PtCo ERD NCs/C catalyst is comparable to the highest known reported values so far for Pt–Co catalysts, especially in terms of the specific activity (Table S1, ESI†). We also applied the catalysts to the methanol oxidation reaction, in which the MOR measurements were carried out in a mixture solution of 0.5 M H2SO4 and 0.5 M CH3OH. Fig. 4c shows that two anodic peaks were clearly observed during the forward and backward sweeps, and PtCo ERD NCs/C showed the highest activity among the three catalysts. It was found that the specific activity of 6.8 mA cm−2 and the mass activity of 1.2 A mgPt−1 were about 6 times and 2 times higher than that of commercial Pt/C, respectively (Fig. 4d). The two PtCo NCs/C catalysts exhibited better performance than Pt/C, suggesting the enhanced activity of the as-prepared PtCo ERD NCs/C can be partially contributed to the alloy feature of the Pt and Co elements. It was demonstrated that the improved catalytic performance of the PtM alloys is due to the surface electronic structure modification (d-band centre) from the bimetallic synergetic effect, surface atomic arrangement improvement (bond distance and coordination number) and the possible lattice strain effect of Pt.40–43 On the other hand, it may also be ascribed to the unique excavated structure integrating the merits of the large surface area, which results in high atomic utilization efficiency and the feasible accessibility of the active sites. In addition, by careful observation of the TEM images, we found that the PtCo ERD catalyst is structurally stable due to less agglomeration, and the excavated structure can be maintained after electrochemical measurements (Fig. S16 and S17, ESI†). The stability of the as-prepared PtCo ERD NCs/C catalyst was evaluated by chronoamperometry carried out in a mixed solution of 0.5 M H2SO4 + 0.5 M CH3OH at 0.4 V (vs. SCE). The i–t curves (Fig. S18 ESI†) reveal a slow attenuation in the PtCo ERD NCs/C catalyst, and show a current density that is higher (by ∼1.5 times) than that of Pt/C after 1200 s of measurement.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0na00717j |
‡ Cong Shen and Xuemin Li are co-first authors. |
This journal is © The Royal Society of Chemistry 2020 |