Open Access Article
Yaqi Renab,
Hong Zhao*c,
Jianpeng Lid,
Rui Wanga and
Zhaohuan Wei
*ef
aSchool of Materials and Environmental Engineering, Chengdu Technological University, Chengdu, 611730, China
bCenter of Big Data for Smart Environmental Protection, Chengdu Technological University, Chengdu 611730, China
cSchool of Materials Science and Energy Engineering, Foshan University, Foshan, 528225, China. E-mail: mezhaohong@gmail.com
dSchool of Chemistry and Materials Engineering, Huizhou University, Huizhou, 516007, China
eSchool of Physics, University of Electronic Science and Technology of China, Chengdu, 611731, China. E-mail: zhwei@uestc.edu.cn
fGuangdong Provincial Key Laboratory of Energy Materials for Electric Power, Shenzhen 518055, China
First published on 20th April 2020
Small Ag nanoparticles are well dispersed onto graphene sheets via a simple and environmentally friendly route using disposable paper-cups. The obtained Ag/graphene materials exhibit much higher catalytic activity for the oxygen reduction reaction than the conventional Ag/graphene catalyst does in alkaline media.
To form the electrocatalyst, it is essential to load Ag NPs onto a support material. An excellent support could maximize the active surface area for electrocatalytic reaction, minimize catalyst cost, as well as provide high electronic conductivity for electrochemical reactants. Graphene is now widely used for electronic, energy storage and catalytic applications due to an excellent conductivity and mechanical property. In the electrocatalytic field, graphene is regarded as an excellent support material, mainly because the intimate contact between the graphene support and metal particles enables the catalysts to be formed to have high activity.15–17 However, it is difficult to obtain small and well-dispersed graphene supported Ag NPs since Ag NPs are easy to agglomerate with each other to reduce the surface energy, unless adding stabilizers or surfactants. However, the utilization of surfactants could contaminate the metal catalyst surface, which can seriously impact the performance of the catalyst. Meanwhile, because it is difficult or high cost to produce graphene with high quality in a high yield, which could limit the application of graphene as catalyst support in fuel cells.18–22
As a result, it is very important and urgent to find a feasible route for both preparing high quality graphene with low cost and small sized and well dispersed Ag NPs without using any surfactants to improve the ORR activity of the Ag nanoparticles in alkaline media. Some previous works have focused on high quality graphene on a large scale from disposable paper-cups as a carbon source, as well as well dispersed metal NPs with small sizes supported on graphene nanosheets, which provides a good reference for us to carry out this mission.23–25
In this work, we extend the procedures reported in the previous works as follows: first, graphene with Fe is synthesized from disposable paper-cups with Fe2+ where Fe2+ plays the role of catalyst, in which the resources are environmentally friendly and cheap. Subsequently, after adding the as-prepared Fe/graphene materials into Ag+ solutions, Ag+ would react with Fe via a galvanic replacement process. After this simple route, well dispersed Ag NPs with small sizes are anchored onto graphene sheets without aggregation. Besides, the graphene prepared via this method has little defects, which is benefit for increasing the electrocatalytic activity. Furthermore, no surfactant is used during the synthesis process, clearing off the passive impact of electrocatalytic sites. Based on the above advantages, this Ag/graphene structure could help improve the electrocatalytic performance compared with the Ag/C catalyst prepared by conventional method.26
The structures of the samples were characterized by means of transmission electron microscopy (TEM, JEM-2010), X-ray photoelectron spectroscopy (XPS, ESCALAB 250 system, VG), Raman spectrometer (Jobin Yvon HR 800), X-ray diffraction (XRD, Rigaku D/Max 2500/PC) and thermogravimetric analysis (STA449F3 Jupiter).
Linear sweep voltammograms (LSV) curves were tested in a conventional three-electrode system in 0.1 M KOH media. A platinum wire, Hg/HgO electrode (0.1 M KOH, 0.164 V vs. SHE) and rotating disc electrode (RDE) were used as the counter electrode, reference electrode and working electrode, respectively. A homogeneous ink was processed by dispersing 4 mg catalysts in Nafion–ethanol solution (2 mL, 1 vol%) with sonication for 1 h and dried with an infrared lamp. Then the catalyst ink was coated onto the GC electrode for the ORR test. For comparison, the ORR property of Ag/C (Vulcan XC72) sample prepared with conventional method26 was tested in the same condition.
| Fe + 2Ag+ = 2Ag + Fe2+ | (1) |
As seen from the TEM image at different magnifications of Fig. 2, the well dispersed Ag NPs with small sizes are anchored onto graphene sheets, and the average size of Ag NPs is about 3 nm. The energy dispersive energy dispersive spectrometer (EDS) analysis of confirms the nanostructure contains Ag and C elements. A small amount of Ni is also detected, which results from carbon-coated nick grids used during testing samples. Besides, the signal peak of Fe at 6.398 keV is invisible, which means that Fe is removed thorough from the displacement reaction of Ag+ and Fe mostly.
Fig. 3 shows the results of TEM examination together with EDS mapping for both C and Ag elements. The blue-green and red regions relative to the Ag and C elements, respectively, indicating that Ag nanoparticles are distributed uniformly throughout the whole area of C. The uniform distribution of Ag nanoparticles in graphene is attributed to the in situ synthesis of Ag/graphene, as described in the experimental part.
Furthermore, Fig. 4a shows the XRD diffraction pattern of Ag/graphene. The diffraction peak located at 2θ = 26.2° can be observed, which corresponds to (002) crystal planes of graphite. Meanwhile, the XRD pattern still has peaks at 2θ = 38.0°, 44.3°, and 64.3°, corresponding to the (111), (200), and (220) planes of metal Ag, respectively.29 This result is consistent with the high resolution TEM image (Fig. 2) of the hybrid sample. The XPS pattern of the as-prepared Ag/graphene is shown in Fig. 4b. The two individual peaks at 379.1 and 368.2 eV correspond to the 3d5/2 and 3d3/2 binding energies of Ag, respectively.30
In addition, to further confirm whether the Fe is replaced by Ag completely, the intensity of Fe is also presented in Fig. S1.† From the barely formed peak of XPS curve for Fe as shown in Fig. S1,† we can conclude that Fe is almost replaced as proposed. Also, as shown in Fig. S2,† the signal peak from oxygen is very weak, and the ratio of O/C is about 0.05, which indicates that the content of oxygen is low. To be clear, the existing small amount of oxygen may be attributed to the adsorption of oxygen on the surface of graphene.
Raman is powerful tool to confirm the doping of graphene sheets with Ag NPs.31 As shown in Fig. 5, three differences can be observed through comparing the Raman spectra of graphene and Ag/graphene samples. First, the value of ID/IG increases from 0.16 for graphene to 0.30 for Ag/graphene, which can be explained as the action of silver on carbon change the structure of graphene, leading to a disordered structure after Ag decorating on graphene.32 Meanwhile, the low ID/IG value of graphene verifies that the sample is graphene rather than graphene oxides (GO) since the ratio of ID/IG for GO is close to 1.0.33 Second, the 2D band shifts from 2762 cm−1 to 2711 cm−1, and the G band shifts from 1585 cm−1 to 1588 cm−1 for graphene and Ag/graphene, respectively. This can be attributed to the influence of electron properties during the double resonance process,34,35 and indicates n-doping of graphene with Ag deposition.36 Third, all the density of D-, 2D-, and G-peaks increase greatly for Ag/graphene, which is mainly due to the strong interaction between Ag and graphene.36 These characterization results confirm that the formation of Ag NPs onto graphene sheets.
The ORR measurements are evaluated in O2-saturated 0.1 M KOH electrolyte at room temperature. The RDE polarization curves of ORR on Ag/graphene catalysts is shown in Fig. 6a. The onset potential (Eon) of the ORR is 0.83 V vs. RHE37 and then the reduction current rises rapidly to its diffusion ultimate value. The RDE polarization curves of ORR were calculated by the Koutecky–Levich (K–L) equation:38
485 C mol−1), ω represents the electrode rotation rate, ν is on behalf of the kinematic viscosity of the solution (0.01 cm2 s−1), CO2b is the concentration of oxygen in the bulk (1.2 × 10−6 mol cm−3), and DO2 is the diffusion coefficient of oxygen (1.9 × 10−5 cm2 s−1).39 Fig. 6b shows the K–L plots and the n values were calculated from the K–L equation. The average electron number transferred per O2 molecule is close to four based on the K–L plots. Fig. 6c shows the j–E curves of ORR on different catalysts at a single rotation rate (ω = 2000 rpm). It is found that the onset potentials for Ag/graphene shows a positive shift of approximately 40 mV when compared with Ag/C catalyst (0.79 V vs. RHE) with same mass loading with Ag/graphene (18%, shown in Fig. S3†). Also the value of E1/2 is larger for the latter catalyst. We compared the ORR performance of Ag/graphene catalyst with the published Ag/C electrocatalysts, as shown in Table 1, which indicates that our Ag/graphene exhibits better ORR performance. The superior catalytic activity of the Ag/graphene electrode at the diffusion controlled and kinetic regions can be related to the small size and uniform dispersion of Ag NPs on the graphene surface. Because the homogeneous Fe phase is formed during the formation of graphene, the galvanic displacement reaction between Fe and Ag+ ions will result in better dispersion and small size of Ag NPs on the graphene, tending to increase of the electrochemically active surface area of Ag. Also, no intervene of any stabilizers or surfactants were added through the whole synthesis process, which greatly enhanced the electrocatalytic performance of Ag NPs.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/d0ra02127j |
| This journal is © The Royal Society of Chemistry 2020 |