Glycine-derived nitrogen-doped ordered mesoporous carbons with a bimodal mesopore size distribution for supercapacitors and oxygen reduction

超级电容器 材料科学 介孔材料 碳化 碳纤维 化学工程 氮气 掺杂剂 比表面积 电化学 兴奋剂 无机化学 催化作用 电极 有机化学 复合材料 化学 复合数 物理化学 工程类 光电子学 扫描电子显微镜
作者
Ying Shao,Zeyu Hu,Yan Yao,Xiangru Wei,Xingmin Gao,Zhangxiong Wu
出处
期刊:New Carbon Materials [Elsevier]
卷期号:37 (1): 259-276 被引量:6
标识
DOI:10.1016/s1872-5805(22)60585-7
摘要

Nitrogen-doped carbon materials are promising for electrochemical energy storage and conversion. Dopant control and pore engineering play important roles in improving their performance. We have synthesized nitrogen-doped ordered mesoporous carbons (N-OMCs) with a bimodal mesopore size distribution using a solvent-free nanocasting method. The simplest amino acid (glycine, Gly) was used as the only carbon precursor and ordered mesoporous silica SBA-15 as the hard template. The confined pyrolysis of Gly in SBA-15 leads to efficient carbonization, nitrogen doping and an interesting structure. The N-OMCs have high surface areas (923–1374 m2·g−1), large pore volumes (1.32–2.21 cm3·g−1), a bimodal distribution of mesopore sizes (4.8 and 6.2–20 nm) and high nitrogen contents (3.66%–12.23%). The effects of the Gly/SBA-15 mass ratio (1–3) and carbonization temperature (700–1000 °C) on the physicochemical properties of the N-OMCs were studied. When used as electrode materials the N-OMCs have a high performance in supercapacitors. A typical sample has a large specific capacitance of 298 F·g−1, a good rate capability (70% retention at 30 A·g−1) and high stability. The different capacitances and rate capabilities of the N-OMCs are discussed by correlating them with their physicochemical properties. A balance of surface area, degree of graphitization, nitrogen doping, and an open mesoporous structure is essential to achieve the best performance. The N-OMCs also have a good performance in the electrocatalytic oxygen reduction reaction. A typical sample has a high onset of 0.92 V, a high half-wave potential of 0.83 V and a large limiting current density of 5.06 mA·cm−2.
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