Effect of oxidation heat treatment temperature on microstructure and microwave absorption properties of porous nickel foam
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摘要: 为了探究多孔镍泡沫在电磁污染环境应用的可能性,根据多孔镍泡沫在空气下的热重曲线图,采用不同氧化热处理温度对其进行高温处理,借助TG-DSC、XRD、SEM、矢量网络分析仪研究氧化热处理温度对多孔镍泡沫的微观结构和电磁波吸收性能的影响关系。结果表明,当氧化热处理温度超过600℃时,多孔镍泡沫骨架表面产生明显变化,当氧化热处理为900℃时,表面形成大量孔洞,而当氧化热处理温度到达1200℃时,表面呈熔融状。通过物相分析表明,随着氧化热处理温度升高,多孔镍泡沫骨架表面生成氧化镍。对X波段的电磁吸波性能进行测试可以发现,经900℃氧化热处理得到的多孔镍泡沫具有最优异的微波吸收性能,并在10.88 GHz处反射损耗到达最小值−19.66 dB,表明一定的氧化热处理可以有效改善多孔镍泡沫的吸波性能。Abstract: According to the thermogravimetric curve diagram of porous nickel foam in air, different oxidation heat treatment temperatures were employed for high temperature treatment, and the effect of the oxidation heat treatment temperature on the microstructure and electromagnetic microwaves of porous nickel foam was studied by TG-DSC, XRD, SEM, and vector network analyzer to explore the possibility of the application of porous nickel foam in electromagnetic pollution environment. The results show that when the oxidation heat treatment temperature exceeds 600℃, the surface of the porous nickel foam skeleton has obvious changes. When the oxidation heat treatment is 900℃, the surface forms a flaky structure, and when the oxidation heat treatment temperature reaches 1200℃, the surface becomes molten. The phase analysis indicates that with the increase of the oxidation heat treatment, the nickel oxide is formed on the surface of the porous nickel foam network. The electromagnetic absorption performances in the X-band are tested, and the porous nickel foam obtained by the oxidation heat treatment at 900℃ owns the most excellent microwave absorption performance, the reflection loss of which reaches the minimum value of −19.66 dB at 10.88 GHz, indicating that a certain oxidation heat treatment could effectively improve the microwave absorbing properties of the porous nickel foam.
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图 4 氧化热处理后多孔镍泡沫的电磁参数分析:(a)相对复介电常数实部;(b)相对复介电常数虚部;(c)相对复磁导率;(d)介电损耗因子
Figure 4. Electromagnetic parameter analysis of porous nickel foam after oxidation heat treatment: (a) Real part of the relative complex permittivity; (b) Imaginary part of the relative complex permittivity; (c) Relative complex permeability; (d) Dielectric dissipation factor
图 6 经900℃氧化热处理后多孔镍泡沫在不同匹配厚度和电磁波频率下的反射损耗图:(a) 二维平面图;(b) 三维曲面图;(c) 反射损耗最小;(d) 有效吸收频带最宽
Figure 6. Reflection loss maps of porous nickel foam after 900℃ oxidation heat treatment at various matching thickness and electromagnetic frequency:(a) Two-dimensional plan; (b) Three-dimensional surface diagram; (c) Minimum reflection loss; (d) Widest effective absorption band
fE—Effective absorption band; d—Matching thickness; fEmax—Widest effective absorption band; RLmin—Minimum reflection loss
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