Hashemi Seyyed Alireza, Ghaffarkhah Ahmadreza, Ahmadijokani Farhad, Yousefian Hatef, Mhatre Sameer E, Sinelshchikova Anna, Banvillet Gabriel, Kamkar Milad, Rojas Orlando J, Wuttke Stefan, Arjmand Mohammad
Nanomaterials and Polymer Nanocomposites Laboratory, School of Engineering, University of British Columbia, Kelowna, BC, V1V 1V7, Canada.
Bioproducts Institute, Department of Chemical & Biological Engineering, Department of Chemistry and Department of Wood Science, 2360 East Mall, The University of British Columbia, Vancouver, BC V6T 1Z3, Canada.
Nanoscale. 2024 May 9;16(18):8858-8867. doi: 10.1039/d3nr06478f.
For decades, the inherently reflective nature of metallic electromagnetic (EM) shields and their induced secondary EM pollution have posed significant challenges for sensitive electronics. While numerous efforts have been made to develop superior EM shielding systems, the issue of reflection dominancy in metallic substrates remains unresolved. Herein, we addressed this long-lasting obstacle by pairing metallic shields with ultra-lightweight (density of 3.12-3.40 mg cm) elastic anti-reflection aerogels, altering their shielding mechanism from dominant reflection (reflectance >0.8) to absorption (absorbance >0.7) by trapping EM waves inside the aerogel. The aerogel EM traps were generated using interfacial complexation, yielding engineerable filamentous liquid structures. These served as templates for aerogel creation through a follow-up process of freezing and lyophilization. The engineerable lossy medium of aerogels benefits from a multi-scale porous construct with the combined action of dielectric and conduction losses, highly dissipating the EM waves and minimizing the reflections. Notably, declining the diameter of aerogel filaments promoted its absorption dominancy, rendering it a potent dissipating medium for EM waves. Pairing a metallic substrate with filamentous aerogel EM traps has resulted in an exceptionally effective absorption-dominant shielding system, achieving absorbance levels between 0.70-0.81. This system offers a shielding effectiveness of 53-89 dB within the X-band frequency range. This innovation addresses a persistent issue in shielding science related to the reflective characteristics of metallic substrates, effectively inhibiting their induced EM reflections.
几十年来,金属电磁(EM)屏蔽层固有的反射特性及其产生的二次电磁污染给敏感电子设备带来了重大挑战。尽管人们为开发卓越的电磁屏蔽系统付出了诸多努力,但金属基板中反射占主导的问题仍未得到解决。在此,我们通过将金属屏蔽层与超轻(密度为3.12 - 3.40 mg/cm)的弹性抗反射气凝胶配对,解决了这一长期存在的障碍,通过将电磁波捕获在气凝胶内部,将其屏蔽机制从主要反射(反射率>0.8)转变为吸收(吸收率>0.7)。气凝胶电磁陷阱是通过界面络合产生的,形成了可设计的丝状液体结构。这些结构通过后续的冷冻和冻干过程作为气凝胶形成的模板。气凝胶这种可设计的有损介质得益于具有介电损耗和传导损耗共同作用的多尺度多孔结构,能高效耗散电磁波并将反射降至最低。值得注意的是,减小气凝胶细丝的直径会增强其吸收主导性,使其成为一种强大的电磁波耗散介质。将金属基板与丝状气凝胶电磁陷阱配对,产生了一种极其有效的以吸收为主的屏蔽系统,吸收率在0.70 - 0.81之间。该系统在X波段频率范围内提供53 - 89 dB的屏蔽效能。这一创新解决了屏蔽科学中与金属基板反射特性相关的一个长期问题,有效抑制了其产生的电磁反射。