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使用铝-氮化钛-铁的石墨烯超材料太阳能吸收器用于高效太阳能热能转换及基于机器学习的优化

Graphene metamaterial solar absorber using Al-TiN-Fe for efficient solar thermal energy conversion and optimization using machine learning.

作者信息

Aliqab Khaled, Han Bo Bo, Kumar Om Prakash, Alsharari Meshari, Armghan Ammar, Patel Shobhit K

机构信息

Department of Electrical Engineering, College of Engineering, Jouf University, 72388, Sakaka, Saudi Arabia.

Department of Information and Communication Technology, Marwadi University, Rajkot, 360003, India.

出版信息

Sci Rep. 2024 Dec 30;14(1):31643. doi: 10.1038/s41598-024-80485-0.

DOI:10.1038/s41598-024-80485-0
PMID:39738203
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11685637/
Abstract

The contributed absorber design in graphene addition with the displacement of three materials for resonator design in Aluminum (Al), the middle substrate position with Titanium nitride (TiN), and the ground layer deposition by Iron (Fe) respectively. For the absorption validation highlight, the best four absorption wavelengths (µm) of 0.29, 0.58, 1, and 2 are also selected to indicate the changes in radiation outputs for every observation. With the displacement of wavelength and bandwidth configuration, the current absorber is observed at 97.32% (more than 97%) for 1.5-2.5 µm wavelength range (1000 nm bandwidth) and above 95% rate (95.38%) is displayed by the 2000 nm bandwidth due to 0.5 and 2.5 µm wavelength separation. The 2800 nm band rate demonstration by 0.2-3 µm wavelength separation verifies 92.42%. For every analysis in this work, the output radiation is shown in ultraviolet region (UV), visible spectrum (Vis), and near-infrared (NIR) area respectively. In the following distribution of the current absorber, the design development in lithography and step-by-step, parametric assignment and AM configuration, radiation analysis for each parameter changes in graph presentation and conclusion. Additionally, the ML approach is applied to reduce the time required in the study. The current solar absorber in the new design can be generated for the multi-solar purposes of water heating, lighting, ventilation, charging for electronic devices, and electric vehicle transportation.

摘要

在石墨烯中采用的贡献型吸收体设计,同时对三种材料进行了位移,用于铝(Al)中的谐振器设计,中间衬底位置采用氮化钛(TiN),接地层分别由铁(Fe)沉积。为突出吸收验证,还选择了0.29、0.58、1和2这四个最佳吸收波长(微米)来表明每次观测中辐射输出的变化。随着波长和带宽配置的位移,在1.5 - 2.5微米波长范围(1000纳米带宽)内,当前吸收体的吸收率为97.32%(超过97%);由于波长间隔为0.5和2.5微米,在2000纳米带宽下显示出高于95%的吸收率(95.38%)。波长间隔为0.2 - 3微米时的2800纳米波段吸收率验证为92.42%。在这项工作的每次分析中,输出辐射分别显示在紫外区域(UV)、可见光谱(Vis)和近红外(NIR)区域。在当前吸收体的后续分布中,光刻和逐步的设计开发、参数赋值和增材制造配置、图形展示中每个参数变化的辐射分析以及结论。此外,应用机器学习方法来减少研究所需的时间。新设计中的当前太阳能吸收体可用于水加热、照明、通风、电子设备充电和电动汽车运输等多种太阳能用途。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/76a02154000c/41598_2024_80485_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/e251cd92ff20/41598_2024_80485_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/359d7fb23bc2/41598_2024_80485_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/2aad6c83ed74/41598_2024_80485_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/2aa7986473a5/41598_2024_80485_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/f6920d25057d/41598_2024_80485_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/fd6ee22e1708/41598_2024_80485_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/0c1257935a31/41598_2024_80485_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/82d8a0d382e7/41598_2024_80485_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/3f8801814c16/41598_2024_80485_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/3fc874aa48fa/41598_2024_80485_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/7a8e4cc2c700/41598_2024_80485_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/06cc1792c4d6/41598_2024_80485_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/76a02154000c/41598_2024_80485_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/e251cd92ff20/41598_2024_80485_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/359d7fb23bc2/41598_2024_80485_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/2aad6c83ed74/41598_2024_80485_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/2aa7986473a5/41598_2024_80485_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/f6920d25057d/41598_2024_80485_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/fd6ee22e1708/41598_2024_80485_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/0c1257935a31/41598_2024_80485_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/82d8a0d382e7/41598_2024_80485_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/3f8801814c16/41598_2024_80485_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/3fc874aa48fa/41598_2024_80485_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/7a8e4cc2c700/41598_2024_80485_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/06cc1792c4d6/41598_2024_80485_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fe9e/11685637/76a02154000c/41598_2024_80485_Fig13_HTML.jpg

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