Lightweight and flexible 3D graphene microtubes membrane for high-efficiency electromagnetic-interference shielding

•Lightweight and flexible 3D graphene microtubes membrane has been fabricated.•Interconnected edge-rich VGNs were grown on interwoven conductive CMTs networks.•The 3D GMTs membrane exhibits highly shows ultrahigh EMI shielding performance. Ultralight, flexible and high-performance electromagnetic-in...

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Published inChemical engineering journal (Lausanne, Switzerland : 1996) Vol. 387; p. 124025
Main Authors Yin, Xuemin, Li, Hejun, Han, Liyuan, Meng, Jiachen, Lu, Jinhua, Zhang, Leilei, Li, Wei, Fu, Qiangang, Li, Kezhi, Song, Qiang
Format Journal Article
LanguageEnglish
Published Elsevier B.V 01.05.2020
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Summary:•Lightweight and flexible 3D graphene microtubes membrane has been fabricated.•Interconnected edge-rich VGNs were grown on interwoven conductive CMTs networks.•The 3D GMTs membrane exhibits highly shows ultrahigh EMI shielding performance. Ultralight, flexible and high-performance electromagnetic-interference (EMI) shielding performance materials are urgently required in the areas of aircraft/aerospace, portable and wearable smart electronics. Benefiting from the outstanding properties of graphene and the unique architectures, 3D assembled graphene structures have been widely applied in the field of EMI-shielding. Herein, for the first time, using Si3N4 nanowires as self-sacrificial templates with the thermal decomposition characteristics, 3D graphene microtubes (3DGMTs) membrane is fabricated by plasma enhanced chemical vapor deposition (PECVD) method, exhibiting the characteristics of free-standing and flexibility. 3DGMTs membrane assembled with silicon carbide (SiC) nanocrystals decorated edge-rich vertical graphene nanosheets (VGNs) exhibits superb EMI shielding effectiveness (SE) of around 38 dB in the frequency range of 8.2~12.4 GHz at a density of 0.0036 g cm−3 and a thickness of 1.5 mm. Considering the ultralow density and thickness, 3DGMTs membrane shows a high specific SE (SSE, defined as SE divided by mass density) of 10,556 dB cm3 g−1 in X-band, which far surpasses that of almost all the reported materials. Remarkably, our work not only provides a new idea for preparation of hollow tubular carbon materials for a wide range of applications, but also presents some fundamental insights for edge-rich VGNs applied in EMI shielding.
ISSN:1385-8947
1873-3212
DOI:10.1016/j.cej.2020.124025