Hydrothermal self-assembled Fe3O4/CA core-shell composites for broadband microwave absorption

https://doi.org/10.1016/j.jmmm.2021.168511Get rights and content

Highlights

  • Fe3O4 and CA can easily complete self-assembly under hydrothermal conditions.

  • The Fe3O4/CA composites have good impedance matching and rich loss preformance .

  • The core–shell structure greatly enhances the interfacial polarization.

Abstract

Electromagnetic wave has emerged as a new source of environmental pollution in the daily life. Therefore, the prominent microwave absorbents are urgently needed. In this work, the carbon aerogel and Fe3O4 nanoparticle (Fe3O4/CA) composites with core–shell structure were facilely prepared by a self-assembly process between carbon aerogels and Fe ion under the hydrothermal condition. The microwave absorption performance was significantly enhanced due to the perfect impedance matching and effective interface polarization. Compared with Fe3O4 nanoparticles and carbon aerogels, Fe3O4/CA composites show the advantages of strong microwave absorption and broad absorption bandwidth. The maximum RL value of Fe3O4/CA composites is up to −50.96 dB at 4.80 GHz. And also, the effective absorption bandwidth reaches 3.82 GHz with the thickness of 2 mm.

Introduction

With the increasing use of the electromagnetic devices, the radiation problem of electromagnetic wave has become the focus of attention. Electromagnetic interference (EMI) not only becomes a catastrophic problem of electronic devices, but also affects human health and causes serious disease such as brain tumors [1] and leukemia [2]. Therefore, there is an urgent need for high-performance electromagnetic wave absorbents. Microwave absorbing materials have a wide range of applications, including communication instruments, space exploration, medical electronic equipment and so on [3]. Meanwhile, they are also widely used in military field [4]. For instance, radar absorbing materials are often used to reduce the detectability of targets by eliminating the reflection of radar signal on their surfaces [5], [6]. To date, an ideal microwave absorber should have the characteristics of lightweight, broad bandwidth, strong absorption and so on. Common electromagnetic absorption materials can be divided into two categories: magnetic absorption materials and dielectric absorption materials. Magnetic absorbers have excellent absorption properties, but their density is usually very high. Compared with the magnetic absorbers, the dielectric absorbers have lighter weight, whereas their impedance matching performance is poor and the absorption bandwidth is narrow. Carbon materials and their composites include grapheme [7], [8], [9], [10], [11], [12], carbon nanotubes [13], [14], [15], [16], [17], nanoporous carbon [18], [19] have been widely concerned in the field of microwave absorption due to their superior electrical properties, low cost, environmental friendliness, easy processability and high chemical stability [20]. In recent years, graphene and carbon nanotubes have been developed and shown excellent application in EMI [21]. Unfortunately, the synthesis of these materials requires expensive raw materials and the preparation process is extremely complex (such as chemical vapor deposition (CVD), Hummer method, arc discharge, etc.), which severely hinder their practical application. Therefore, it is urgent to develop suitable carbon materials with facile synthesis process.

It is reported that porous carbon materials (such as foamed carbon) have lower dielectric constant and better impedance matching, indicating that the modification of the porous structure is an effective way to design and prepare good electromagnetic absorbers. Carbon aerogel (CA) is a kind of nanoporous carbon material with light weight, adjustable pore size, high specific surface area and moderate conductivity [22]. More importantly, carbon aerogels show strong optical absorption in a wide optical band. Sun et al. studied the optical property of carbon aerogels with different 3D network nanostructure and found that the reflectivity of the carbon aerogels was strongly dependent on their micropores [23]. However, carbon aerogels have only dielectric loss, and their absorbing capability is limited. At the same time, Fe3O4 based composites have attracted great attention due to their magnetic property, soft metal property, huge magnetic anisotropy, good biocompatibility and low toxicity. However, Fe3O4 also has some problems such as high density, poor corrosion resistance and low impedance matching. The composition of the dielectric loss type carbon materials and the magnetic loss type Fe3O4 can effectively overcome the above problems, which gives full play to their respective advantages and improves the absorbing performance. Ternary core–shell Fe3O4@C@PANI composites synthesized by Manna et al. showed minimum reflection loss of −33 dB in the frequency range (2–8 GHz). Such high value of shielding efficiency was ascribed to the presence of dual interfaces and dielectric-magnetic integration in Fe3O4@C@PANI [24]. Wu at al. prepared Fe3O4/C composite flowers through a facile route including a solvothermal approach and a carbon reduction process, which displayed an optimal reflection loss value of −54.6 dB at 5.7 GHz when the thickness was 4.27 nm [25]. Fe3O4 (core) /C (shell) composites are considered to be an efficient absorption material because of the combination of chemical uniformity, magnetic loss, dielectric loss, structural loss, impedance matching and several key factors affecting microwave absorption. Therefore, Fe3O4/C composites with high dielectric loss and magnetic loss is a good choice for microwave absorption [26].

In this work, carbon aerogels Fe3O4/CA composites were synthesized by hydrothermal method. In the preparation process, the thickness of carbon layer was adjusted by changing the amount of CA. After successfully preparation of Fe3O4/CA composites, the influence of carbon aerogels on the Fe3O4 particles under hydrothermal environment was studied. Then the microwave absorption performance of the composite material loaded with different content of CA was further explored.

Section snippets

Materials

Resorcinol (≥99.5%, AR), formaldehyde aqueous solution (37–40%, AR), sodium carbonate anhydrous (Na2CO3, ≥99.8%, AR), alcohol (≥99.7%, AR), ferric chloride hexahydrate (FeCl3·6H2O), trisodium citrate dihydrate, ethylene glycol and Sodium acetate (NaAc) were purchased from Sinopharm Chemical Reagent Co., Ltd (Shanghai, China).

Synthesis of carbon aerogels.

The organic precursor was prepared by hydrolysis condensation of resorcinol (R) and formaldehyde aqueous solution (F) with a molar ratio of 1:2 (R/F). Using the deionized

Morphology and microstructure

The morphology and microstructure of the CA, Fe3O4 particles and Fe3O4/CA composites were observed with SEM and TEM. It is clearly noticed from Fig. 2(a) that CAs are composed of dendritic carbon skeleton, which is formed by disordered stacking of primary carbon nanoparticles. As shown in Fig. S2 and Table S1, CA is a lightweight nanoparticle-assembled material with a specific surface area of 1978 m2/g and a density of 0.14 g/cm3. As shown in Fig. 2(b), Fe3O4 particles show a spherical shape

Conclusion

This work provides a simple and efficient method for the preparation of Fe3O4/CA composites with a core–shell structure by self-assemble of carbon aerogels and Fe ion under the hydrothermal condition. Due to the ideal impedance matching and efficient interface polarization, the composites exhibit excellent microwave absorption performance in the frequency range of 2–18 GHz. The microstructure of Fe3O4/CA composites can be controlled by adjusting the mass of carbon aerogels. The maximum RL value

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

This work was financially supported by National Key Research and Development Program of China (2017YFA0204600) and National Natural Science Foundation of China (11874288).

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    Q. Zhu and X. Zhang contributed equally to this work.

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