Dong Liu,
Lu Yang,
Jian She Huang,
Qiao Hui Guo and
Tian Yan You*
State Key Laboratory of Electroanalytical Chemistry, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, PR China. E-mail: youty@ciac.jl.cn
First published on 6th March 2014
Pt nanoparticle (NP)-loaded 1-aminopyrene functionalized reduced graphene oxide composites (Pt/1-AP–rGO) were synthesized by a simple polyol process. The morphology and structure of the resulting composites were characterized by transmission electron microscopy, Raman spectroscopy and X-ray diffraction. In comparison with Pt/–rGO, the resulting Pt/1-AP–rGO exhibited much better dispersibility. Higher dispersion and smaller size of Pt NPs was also observed on 1-AP functionalized rGO. As a result, Pt/1-AP–rGO showed higher catalytic activity, better anti-poisoning ability and stability for methanol oxidation. Meanwhile, it also displayed better electrocatalytic performance toward H2O2. The strategy presented here offers an efficient way for the preparation of high-performance electrocatalysts, which will find promising applications in biosensors and fuel cells.
Recently, due to various intriguing properties, graphene has emerged as one of the most promising catalyst support.15–17 In particular, graphene-supported Pt and PtM (M = Pd, Fe etc.) NPs composites have been extensively explored in the field of fuel cells and biosensors.18–21 Various state-of-the-art approaches, such as in situ growth,22 self-assembly23 and one-pot method,24 have been developed for the preparation of graphene-supported NPs composites. Unfortunately, the easy aggregation of the graphene sheets leads to the decrease of the effective surface area and eventually detrimental to the electrochemical applications.25 To address this issue, an effective strategy is by covalent or non-covalent attaching certain molecule onto graphene surface.26 Even more important, the attached molecules with suitable groups, such as amino group, could also serve as nucleating sites of the NPs.27 Non-covalent functionalization of graphene with aromatic molecule takes the advantages of simple decoration process and well-maintained intrinsic electronic properties of graphene. Pyrenecarboxylic acid, perylene tetracarboxylic acid and pyrenesulfonic acid sodium salt-functionalized graphene showed improved dispersibility and excellent electrochemical performance.28–31
1-aminopyrene (1-AP) could be a suitable molecule for the functionalization of graphene which contains both benzene ring structure and amino group.32,33 In this work, we utilized 1-AP as the non-covalent functional reagent to prepare Pt NPs-loaded reduced graphene oxide (rGO) composites. Results demonstrate that Pt NPs supported on 1-AP functionalized rGO showed better dispersity and smaller size than that on rGO. The resulting composites exhibited high electrocatalytic activities towards methanol oxidation and H2O2 reduction.
UV-Vis analysis was performed with a UV-3000PC spectrophotometer. Particle size and morphology were obtained on transmission electron microscope (TEM, HITACHI H-8100 EM). X-ray diffraction (XRD) patterns were acquired using a D8 ADVANCE X-ray diffractometer (Bruker AXS, Germany) with Cu Kα radiation (λ = 1.54056 Å). Raman spectra were recorded on a Renishaw Raman microscope (model RM2000) with laser excitation wavelength of 514.5 nm. Pt-loading in the composites was determined by inductively coupled plasma optical emission spectroscopy (ICP-OES, Thermo Fisher).
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| Fig. 1 UV-visible spectra of (a) 1-AP, (b) Pt/1-AP–rGO and (c) Pt/rGO in ethanol. Inset: photographs of (1) Pt/rGO and (2) Pt/1-AP–rGO in ethylene glycol. Raman spectra of GO, Pt/rGO and Pt/1-AP–rGO. | ||
UV/visible spectra were used to confirm the successful non-covalent binding of 1-AP. As shown in Fig. 1A, Pt/rGO shows a typical featureless spectrum (curve c). The two additional peaks around 355 and 281 nm observed in the spectrum of Pt/1-AP–rGO could be ascribed to the characteristic peaks of 1-AP at 360 and 285 nm (curve a), suggesting that rGO has been successfully functionalized by 1-AP.32
Raman spectroscopy is an effective method to distinguish the ordered and disordered structure of carbon in carbonaceous materials. The Raman spectrum of GO, Pt/rGO and Pt/1-AP–rGO are shown in Fig. 1B. Two prominent scattering peaks located at 1350 and 1595 cm−1 can be assigned to the E2g phonon of sp2 carbon atoms (D-band) and breathing mode of κ-point phonons of A1g symmetry (G-band), respectively. The intensity ratio of D to G band (ID/IG) could be used to evaluate the degree of modification or defects of rGO. In this work, the ID/IG value of GO, Pt–rGO and Pt/1-AP–rGO is 0.97, 1.13 and 1.06. The increased ID/IG value when GO was reduced to rGO reveals a decrease in the average size of sp2 domains in rGO compared with GO.35 However, the ID/IG values decrease slightly for 1-AP–rGO compared with rGO, which could be attributed to the coverage of the defect sites on rGO by 1-AP.33
Fig. 2A and B displays the TEM images of Pt/rGO and Pt/1-AP–rGO. Obviously, Pt NPs on 1-AP functioned rGO exhibit a better dispersion than that on pristine rGO. In fact, Pt/1-AP–rGO possessed smaller Pt size (3.3 nm) than Pt/rGO (4.8 nm) with a narrower size distribution. This result demonstrates that the presence of 1-AP on GO may provide more effective active sites for the nucleation of Pt NPs and benefit the achievement of Pt NPs with small size. Moreover, the aromatic group in 1-AP could also prevent the aggregation of rGO, leading to larger surface area and more active sites for the loading of Pt NPs.
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| Fig. 2 TEM images of Pt/rGO (A) and Pt/1-AP–rGO (B). Insets are the corresponding Pt NPs size distribution. | ||
XRD patterns of GO, Pt/rGO and Pt/1-AP–rGO are shown in Fig. 3. The sharp diffraction peak at 2θ = 10.8° corresponds to the interlayer spacing of 0.87 nm for GO. However, a new wide diffraction peak appeared at 2θ = 25.1° for Pt/rGO and Pt/1-AP–rGO, confirming the successful reduction of GO to rGO. The three diffraction peaks located at 2θ = 39.5°, 45.8° and 67.4° could be indexed to the (111), (200) and (220) planes of face-centered cubic Pt crystals. Moreover, the broader diffraction peaks of Pt/1-AP–rGO suggest smaller size of Pt NPs on 1-AP–rGO than that on rGO, which is consistent with the TEM results.
Fig. 4A shows the cyclic voltammograms (CVs) of Pt/1-AP–rGO–GCE and Pt/rGO–GCE in 0.5 M H2SO4. Both electrodes exhibit the typical characteristics of hydrogen adsorption and desorption behavior on platinum, confirming the successful loading of Pt NPs on rGO. The electrochemical active surface area (ECSA) is an important data to evaluate the number of the available catalytic active sites, and are estimated from hydrogen desorption peaks from −0.2 to 0.2 V. In this work, ECSA for Pt/1-AP–rGO and Pt/rGO are calculated to be 35.1 and 25.2 m2 g−1, respectively. The increased ECSA of Pt/1-AP–rGO compared with Pt/rGO may originate from the smaller size of Pt NPs. We suppose that the improved dispersibility of Pt/1-AP–rGO also contribute to the increased ECSA.
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| Fig. 4 (A) CVs of Pt/rGO (black line) and Pt/1-AP–rGO (red line) modified GCE in 0.5 M H2SO4; (B) CVs and the modified electrodes in 1.0 M KOH containing 1.0 M CH3OH. Scan rate: 50 mV s−1. | ||
The electrocatalytic activity of the as-prepared Pt/1-AP–rGO was firstly evaluated by investigating for methanol oxidation. Fig. 4B shows the typical CVs of methanol oxidation at Pt/1-AP–rGO–GCE and Pt/rGO–GCE, respectively. Both electrode present the typical CVs of methanol oxidation in alkaline condition, with a forward anodic peak current density (jf) which is attributed to the oxidation of methanol to CO2 and Pt adsorbed carbonaceous intermediates, as well as a back anodic peak current (jb) originating from the additional oxidation of carbonaceous intermediates species to CO2. The CVs of Pt/1-AP–rGO displays a jf of 814 mA mg−1 at −0.208 V in the forward scan, which is 2.1-fold higher than that of Pt/rGO (387 mA mg−1), indicating a higher electrocatalytic activity of Pt/1-AP–rGO. The ratio of the jf to jb (jf/jb), is an important index of the catalyst tolerance to poisoning species generated during methanol oxidation. The calculated jf/jb of Pt/1-AP–rGO (3.39) is evidently larger than that of Pt/rGO (2.74), suggesting better tolerance to poisoning species. Furthermore, the jf/jb value for methanol oxidation on Pt/1-AP–rGO is also higher than that on Pt–GCFM36 and Pt NPs@POM/CNT.37 The long-time stability of Pt/1-AP–rGO towards methanol oxidation was examined by chronoamperometry at −0.2 V (not shown here). The results show that the current decreased rapidly at the first few minutes and then reached a steady state current. The current density of Pt/1-AP–rGO remains 37.1%, while 25.1% for Pt/rGO after 7200 s continuous testing. The results above demonstrate that Pt/1-AP–rGO possesses superior electrocatalytic activity, anti-poisoning ability and good stability for methanol oxidation in comparison with Pt/rGO.
We further studied the electrocatalytic activity of Pt/1-AP–rGO towards H2O2 reduction. Fig. 5A shows the CVs of Pt/1-AP–rGO–GCE and Pt/rGO–GCE in PBS (pH = 7.0) with 5 mM H2O2. Both electrodes exhibit remarkable reduction peak at about 0 V, while the reduction peak current at Pt/1-AP–rGO–GCE is about 2-fold as that at Pt/rGO–GCE. I–t curves of Pt/1-AP–rGO–GCE and Pt/rGO–GCE were obtained by successive injection of H2O2 at the potential of −0.1 V as shown in Fig. 5B. Pt/1-AP–rGO–GCE displays fast response to H2O2, and could reach 95% of the steady-state current in 2 s. The corresponding calibration curves (inset of Fig. 5B) reveal that Pt/1-AP–rGO exhibits higher sensitivity (3.47 μA mM−1) than Pt/rGO (1.83 μA mM−1). Although the Pt/1-AP–rGO–GCE does not exhibit wide linear range toward H2O2 as that for biosensors based on spherical porous Pd nanoparticle assemblies38 and Au–graphene–HRP–chitosan biocomposites,39 it shows relatively fast response to H2O2.
The enhanced electrocatalytic performance can be ascribed to following factors: the larger ECSA of Pt/1-AP–rGO provide more active sites for the reduction of H2O2; Pt/1-AP–rGO can easily form a uniform film on the GCE surface, which could facilitate the diffusion of H2O2 and increase the response sensitivity, while Pt/rGO shows inhomogeneous aggregations on the GCE surface.
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