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具有X波段高吸收和屏蔽性能的碳纳米管薄膜平面电大尺寸结构

Planar Electrically Large Structures of Carbon Nanotube Films with High Absorption and Shielding Performance in X-Band.

作者信息

Sotiropoulos Apostolos, Masouras Athanasios, Anastassiu Hristos T, Kostopoulos Vassilis, Koulouridis Stavros

机构信息

Department of Electrical and Computer Engineering, University of Patras, 26504 Patras, Greece.

Department of Mechanical Engineering and Aeronautics, University of Patras, 26504 Patras, Greece.

出版信息

Sensors (Basel). 2025 Jun 25;25(13):3943. doi: 10.3390/s25133943.

DOI:10.3390/s25133943
PMID:40648201
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12251729/
Abstract

We consider light, high-absorbance, low-reflectance, electrically large layered sheet structures composed of thin carbon nanotube films. Such structures can be utilized in electromagnetic absorption and shielding applications in the X-band. They are of increasing interest in sensor-enabling technologies, stealth systems, and EMI shielding of electronic components. Especially in aerospace, this is crucial, as sensors are integral to aerospace engineering, enhancing the safety, efficiency, and performance of aircraft and spacecraft. To that end, sheets with carbon nanotube films embedded in a glass fiber polymer matrix are fabricated. The films have a thickness of around 70 μm. As shown, they cause a significant attenuation of the electromagnetic field. For shielding applications, a single-film sheet structure with total thickness of 1.65 mm presents an attenuation of around 25 dB in the transmission coefficient, while the attenuation can reach 37 dB for a two-film sheet structure with thickness of 1.8 mm. Shielding effectiveness performance is found to be greater than 35 dB for the two-film sheet structure. For applications requiring both high shielding and absorption, a two-layered structure with a thickness of 4.65 mm has been designed. The absorption, represented by the Loss Factor, is calculated to achieve values greater than 90%. The simulation results show good agreement with the measured data. The findings demonstrate a promising structure for materials suitable for sensor housings and smart electromagnetic environments where the suppression of electromagnetic interference is critical. In conclusion, the addition of carbon nanotube films, even at micrometer thicknesses, within a glass fiber polymer matrix significantly enhances both electromagnetic shielding and absorption performance.

摘要

我们考虑由薄碳纳米管薄膜构成的轻质、高吸收率、低反射率、电大尺寸的层状片状结构。这种结构可用于X波段的电磁吸收和屏蔽应用。它们在传感器启用技术、隐身系统以及电子元件的电磁干扰屏蔽方面越来越受到关注。特别是在航空航天领域,这至关重要,因为传感器是航空航天工程不可或缺的一部分,可提高飞机和航天器的安全性、效率和性能。为此,制造了将碳纳米管薄膜嵌入玻璃纤维聚合物基体中的薄片。这些薄膜的厚度约为70μm。如图所示,它们会使电磁场产生显著衰减。对于屏蔽应用,总厚度为1.65mm的单膜片状结构的传输系数衰减约为25dB,而厚度为1.8mm的双膜片状结构的衰减可达37dB。发现双膜片状结构的屏蔽效能性能大于35dB。对于既需要高屏蔽又需要高吸收的应用,设计了一种厚度为4.65mm的双层结构。以损耗因子表示的吸收率经计算可达到大于90%的值。模拟结果与测量数据显示出良好的一致性。这些发现表明,对于适用于传感器外壳和智能电磁环境(其中抑制电磁干扰至关重要)的材料而言,该结构颇具前景。总之,在玻璃纤维聚合物基体中添加碳纳米管薄膜,即使其厚度为微米级,也能显著提高电磁屏蔽和吸收性能。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/e227e96892f3/sensors-25-03943-g015.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/2eaeef47836e/sensors-25-03943-g006a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/225512c20447/sensors-25-03943-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/55a17ca80308/sensors-25-03943-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/39aafd0ece04/sensors-25-03943-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/539d3303071a/sensors-25-03943-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/1d00a18e5f4f/sensors-25-03943-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/4eff245e68e5/sensors-25-03943-g012a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/5df824549f40/sensors-25-03943-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/80708f880fb7/sensors-25-03943-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/e227e96892f3/sensors-25-03943-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/c2c07325b087/sensors-25-03943-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/2eecd0033034/sensors-25-03943-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/e354e75faeb5/sensors-25-03943-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/25cac98afcd5/sensors-25-03943-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/c3d05b8b7d7a/sensors-25-03943-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/2eaeef47836e/sensors-25-03943-g006a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/225512c20447/sensors-25-03943-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/55a17ca80308/sensors-25-03943-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/39aafd0ece04/sensors-25-03943-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/539d3303071a/sensors-25-03943-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/1d00a18e5f4f/sensors-25-03943-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/4eff245e68e5/sensors-25-03943-g012a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/5df824549f40/sensors-25-03943-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/80708f880fb7/sensors-25-03943-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8e22/12251729/e227e96892f3/sensors-25-03943-g015.jpg

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