| Literature DB >> 32432081 |
Wanqing Teng1, Mengtian Huo1, Zhaomei Sun1, Wenrong Yang1, Xiangjiang Zheng1, Caifeng Ding2, Shusheng Zhang1.
Abstract
It is highly promising to design and develop efficient and economical electrocatalysts for oxygen evolution reaction (OER) in alkaline solution. In this work, we prepare FeCoNi sulfide composites (including FeS, Co3S4, and Ni3S4) derived from in situ sulfurization of precursor oxides on carbon cloth (CC), which are used to become an OER catalyst. Such catalyst shows excellent OER performance, low overpotential, small Tafel slope, and high electrochemical stability, and it is a promising electrocatalyst for OER in alkaline media.Entities:
Keywords: FeCoNi sulfides; electrocatalyst; in situ sulfurization; nanowires array; oxygen evolution reaction
Year: 2020 PMID: 32432081 PMCID: PMC7215084 DOI: 10.3389/fchem.2020.00334
Source DB: PubMed Journal: Front Chem ISSN: 2296-2646 Impact factor: 5.221
Figure 1(A) X-ray diffraction (XRD) patterns of different oxygen evolution reaction (OER) catalysts. (B) XRD patterns comparison of different catalysts powder. (C) XRD pattern of the product after sulfidation treatment.
Figure 2(A) SEM pattern of precursor (FeCoNi-FeOOH). (B) SEM pattern of FeCoNiS-FeOx. (C) TEM pattern of FeCoNiS-FeOx. (D) HRTEM pattern of FeCoNiS-FeOx.
Figure 3(A) Energy-dispersive X-ray (EDX) mapping images of FeCoNiS-FeOx. (B) EDX element distribution pattern.
Figure 4X-ray photoelectron spectroscopy (XPS) spectra of FeCoNiS-FeOx catalyst. (A) Survey spectrum. (B) Fe 2p. (C) Co 2p. (D) Ni 2p. (E) S 2p. (F) O 1s.
Figure 5(A) Linear sweep voltammetry (LSV) curves of different oxygen evolution reaction (OER) catalysts. (B) Tafel curves of different OER catalysts. (C) LSV curve of FeCoNiS-FeOx catalyst and another curve after 500 CV cycles. (D) Time-dependent current density curve of FeCoNiS-FeOx OER catalyst under constant potential.
Figure 6Multistep chronopotentiometric of oxygen evolution reaction (OER) catalyst. The current density started at 60 mA cm−2 and finished at 280 mA cm−2, with an increment of 20 mA cm−2 per 500 s without ohmic potential drop (IR) correction.