石墨烯纳米管阵列有助于全木质超级电容器获得高能量密度和稳定性

Ruimei Yuan, Xuemin Yin, Bei Xue, Jingjing Chang, Wei Wei, Hejun Li
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引用次数: 4

摘要

具有先进纳米结构和体积性能的多孔碳对微型超级电容器特别有吸引力,对于便携式电子设备和大型电气设备来说,它们都是获得高能量密度和电容的关键。然而,电化学性能和孔结构密切相关,都受到孔体积和孔密度的限制。此处,木屑(~0.7 mm)作为具有丰富大孔的基本骨架,并使用具有中孔的石墨烯纳米管阵列(GNTA)作为原位合成的中间结构以在大孔中形成亚结构;因此,生物质和纳米管阵列共同构成了具有分级孔隙和大表面积的多孔碳。在此基础上,在孔隙表面涂覆Cu-Co氧化物,以增加超级电容器应用中电极的电容。由于GNTA,比表面积从38.2增加到1086.0 m2 g−1,这对Cu-Co氧化物纳米片的沉积非常有帮助,并有效缓解了其典型的自堆积现象。同时,GNTA产生了多尺度孔隙,作为快速电子转移和离子穿梭的通道;结果表明,电阻明显感应,电容增加131%(从323.4增加到747.5 mF cm−2)。对于组装的全木质不对称超级电容器,比电容为151.2 F g−1(1 A. g−1),能量密度为53.8 Wh kg−1,功率密度为900 W kg−1,并且比电容在循环过程中保持非常稳定。我们的工作为高性能超级电容器提供了一种实用的结构设计策略。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Graphene nanotube array assists all-wood supercapacitors to access high energy density and stability

Graphene nanotube array assists all-wood supercapacitors to access high energy density and stability

Porous carbons with advanced nanostructures and volumetric performance are particularly attractive and essential for miniature supercapacitors to access high energy densities and capacitances, both for portable electronics and massive electrical equipments. However, the electrochemical performances and the pore structure are closely bound up, both restricted by pore volume and pore density. Herein, the wood slice (~0.7 mm) with the periodic porous structure is chosen as the basic framework with rich macropores and the graphene nanotube array (GNTA) with mesopores is used as an intermediate structure in situ synthesized to form the substructure in macropores; therefore, the biomass and nanotube array together construct a porous carbon with hierarchical pores and large surface area. On this basis, Cu-Co oxides are coated on the surface of the pores, to increase the capacitance of electrodes for supercapacitor applications. Because of the GNTA, the specific surface area increases from 38.2 to 1086.0 m2 g−1, which is quite helpful for the deposition of Cu-Co oxide nanosheets and effectively alleviates their typical self-stacking phenomenon. Meanwhile, the GNTA creates multiscale pores that served as channels for the rapid electron transfer and ion shuttling; as a result, the resistance obviously induces and capacitance increased by 131% (from 323.4 to 747.5 mF cm−2). For the assembled all-wood asymmetric supercapacitor, the specific capacitance is 151.2 F g−1 (1 A g−1), the energy density is 53.8 Wh kg−1 with a power density of 900 W kg−1, and the specific capacitance remains extremely stable during the cycling. Our work provides a practical structure–design strategy for high-performance supercapacitors.

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