TY - JOUR
T1 - Boosting electromagnetic wave absorption of Ti3AlC2 by improving effective electrical conductivity
AU - Guo, Kai Yu
AU - Chen, Lin
AU - Yang, Guan Jun
N1 - Publisher Copyright:
© The Author(s) 2023.
PY - 2023/8
Y1 - 2023/8
N2 - Electromagnetic wave-absorbing (EMA) materials at high temperatures are limited by poor conduction loss (Lc). However, adding conductors simultaneously increases the conduction loss and interfacial polarization loss, leading to a conflict between impedance matching (Zin/Z0) and electromagnetic wave loss. This will prevent electromagnetic waves from entering the EMA materials, finally reducing overall absorbing performance. Here, the effective electrical conductivity (σ) is enhanced by synchronizing particle size and grain number of Ti3 AlC2 to increase the conduction loss and avoid the conflict between the impedance matching and the electromagnetic wave loss. As a result, the best-absorbing performance with an effective absorption bandwidth (EAB) of 4.8 GHz (10.6–15.4 GHz) at a thickness of only 1.5 mm is realized, which is the best combination of wide absorption bandwidth and small thickness, and the minimum reflection loss (RLmin) reaches −45.6 dB at 4.1 GHz. In short, this work explores the regulating mechanism of the EMA materials of effective electrical conductivity by simulated calculations using the Vienna ab-initio Simulation Package (VASP) and COMSOL as well as a series of experiments, which provide new insight into a rational design of materials with anisotropic electrical conductivity.
AB - Electromagnetic wave-absorbing (EMA) materials at high temperatures are limited by poor conduction loss (Lc). However, adding conductors simultaneously increases the conduction loss and interfacial polarization loss, leading to a conflict between impedance matching (Zin/Z0) and electromagnetic wave loss. This will prevent electromagnetic waves from entering the EMA materials, finally reducing overall absorbing performance. Here, the effective electrical conductivity (σ) is enhanced by synchronizing particle size and grain number of Ti3 AlC2 to increase the conduction loss and avoid the conflict between the impedance matching and the electromagnetic wave loss. As a result, the best-absorbing performance with an effective absorption bandwidth (EAB) of 4.8 GHz (10.6–15.4 GHz) at a thickness of only 1.5 mm is realized, which is the best combination of wide absorption bandwidth and small thickness, and the minimum reflection loss (RLmin) reaches −45.6 dB at 4.1 GHz. In short, this work explores the regulating mechanism of the EMA materials of effective electrical conductivity by simulated calculations using the Vienna ab-initio Simulation Package (VASP) and COMSOL as well as a series of experiments, which provide new insight into a rational design of materials with anisotropic electrical conductivity.
KW - anisotropic electrical conductivity
KW - co-optimize impedance matching (Z/Z)
KW - conduction loss (L)
KW - effective electrical conductivity
KW - electromagnetic wave loss
KW - interfacial polarization loss (L)
UR - https://www.scopus.com/pages/publications/85168139310
U2 - 10.26599/JAC.2023.9220770
DO - 10.26599/JAC.2023.9220770
M3 - 文章
AN - SCOPUS:85168139310
SN - 2226-4108
VL - 12
SP - 1533
EP - 1546
JO - Journal of Advanced Ceramics
JF - Journal of Advanced Ceramics
IS - 8
ER -