• Journal of Inorganic Materials
  • Vol. 34, Issue 4, 407 (2019)
Zhi-Jun MA, Chang-Ye MANG, Hai-Tao ZHAO, Zhi-Hao GUAN, and Liang CHENG
Author Affiliations
  • College of Mining, Liaoning Technical University, Fuxin 123000, China
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    DOI: 10.15541/jim20180280 Cite this Article
    Zhi-Jun MA, Chang-Ye MANG, Hai-Tao ZHAO, Zhi-Hao GUAN, Liang CHENG. Comparison of Electromagnetism Behavior of Different Content Cobalt-zinc Ferrite Loaded with Graphene[J]. Journal of Inorganic Materials, 2019, 34(4): 407 Copy Citation Text show less

    Abstract

    A kind of graphene composite (rGO/Co0.5Zn0.5Fe2O4) was synthesized with the graphene oxide (GO) prepared from natural flake graphite and cobalt-zinc ferrite (Co0.5Zn0.5Fe2O4) manufactured by the hydrothermal method. The structure of composites was characterized by X-ray diffraction (XRD), Raman spectrometer (Raman) and the Fourier-transform infrared spectroscopy (FT-IR). Morphology, electromagnetic loss properties, Debye relaxation, and microwave absorbing properties of rGO/Co0.5Zn0.5Fe2O4 were investigated by transmission electron microscope (TEM) and vector network analyser (VNA). Sharp peak of graphene oxide was changed from 2θ=9.74° to 24.15° in the XRD patterns and the oxygen functional group disappeared after the composite reaction, which demonstrated that GO was successfully reduced to rGO. The graphene was embedded with cobalt-zinc ferrite, observed by transmission electron microscope, with its dispersion worse with the loaded Co0.5Zn0.5Fe2O4 increasing. Absorbing property of rGO/Co0.5Zn0.5Fe2O4 composite prepared with w(Co0.5Zn0.5Fe2O4) : w(GO)= 2 : 1 is the best with the minimum reflectivity of -36.89 dB at 15.11 GHz and the effective absorption frequency bandwidth of 3.74.
    $a=d{{({{h}^{2}}+{{k}^{2}}+{{l}^{2}})}^{-1/2}}$

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    {\varepsilon }''=\frac{1}{2}{{\varepsilon }_{\text{0}}}\text{ }\!\!\pi\!\!\text{ }\rho f

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    ${{\varepsilon }_{\text{r}}}={{\varepsilon }_{\infty }}+\frac{{{\varepsilon }_{\text{s}}}-{{\varepsilon }_{\infty }}}{1+\text{j}2\text{ }\!\!\pi\!\!\text{ }f\tau }={\varepsilon }'(f)+\text{i}{\varepsilon }''(f)$

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    ${\varepsilon }'(f)={{\varepsilon }_{\infty }}+\frac{{{\varepsilon }_{\text{s}}}-{{\varepsilon }_{\infty }}}{1+{{(2\text{ }\!\!\pi\!\!\text{ }f)}^{2}}{{\tau }^{2}}}$

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    ${\varepsilon }''(f)=\frac{2\text{ }\!\!\pi\!\!\text{ }f\tau ({{\varepsilon }_{\text{s}}}-{{\varepsilon }_{\infty }})}{1+{{(2\text{ }\!\!\pi\!\!\text{ }f)}^{2}}{{\tau }^{2}}}$

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    ${{({\varepsilon }'-{{\varepsilon }_{\infty }})}^{2}}+{{({\varepsilon }'')}^{2}}={{({{\varepsilon }_{\text{s}}}-{{\varepsilon }_{\infty }})}^{2}}$

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    ${{R}_{\mathrm{L}}}=20\lg \left| \frac{{{Z}_{\text{in}}}-1}{{{Z}_{\text{in}}}+1} \right|$

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    ${{Z}_{\text{in}}}=\sqrt{\frac{{{\mu }_{\text{r}}}}{{{\varepsilon }_{\text{r}}}}}\tanh \left[ \text{j}\frac{2\text{ }\!\!\pi\!\!\text{ }}{c}\sqrt{{{\mu }_{\text{r}}}{{\varepsilon }_{\text{r}}}}fd \right]$

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    Zhi-Jun MA, Chang-Ye MANG, Hai-Tao ZHAO, Zhi-Hao GUAN, Liang CHENG. Comparison of Electromagnetism Behavior of Different Content Cobalt-zinc Ferrite Loaded with Graphene[J]. Journal of Inorganic Materials, 2019, 34(4): 407
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