SiC Hybrid Fibers for Highly Efficient

Temasek Laboratories, National University of Singapore, 5A Engineering Drive 1 ..... (No.16GH030138) of China, Shaanxi Province Foundation for Fundame...
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Electrospinning of Fe/SiC Hybrid Fibers for Highly Efficient Microwave Absorption Yi Hou,† Laifei Cheng,† Yani Zhang,*,† Yong Yang,*,‡ Chaoran Deng,‡ Zhihong Yang,§ Qi Chen,† Peng Wang,† and Lianxi Zheng⊥ †

Science and Technology on Thermostructural Composite Materials Laboratory, Northwestern Polytechnical University, 710072 Xi’an, China ‡ Temasek Laboratories, National University of Singapore, 5A Engineering Drive 1, 117411 Singapore § College of Material Science and Technology, Nanjing University of Aeronautics and Astronautics, 210016 Nanjing, China ⊥ Department of Mechanical Engineering, Khalifa University, 127788 Abu Dhabi, United Arab Emirates ABSTRACT: Fe/SiC hybrid fibers have been fabricated by electrospinning and subsequent high-temperature (1300 °C) pyrolysis in Ar atmosphere using polycarbosilane (PCS) and Fe3O4 precursors. It is found that the introduction of Fe has had a dramatic impact on the morphology, crystallization temperature, and microwave electromagnetic properties of the hybrid fibers. In addition, the Fe particles have acted as catalyst sites to facilitate the growth of SiCO nanowires on the surface of the hybrid fibers. As a result, the permittivity and permeability have been enhanced effectively, and the high reflection loss (RL) has been achieved at a low frequency band with a thin absorber thickness. At an optimal PCS/Fe ratio of 3:0.5, the hybrid fiber/silicone resin composite (35 wt %) with a 2.25 mm absorber thickness exhibits a minimal RL of about −46.3 dB at 6.4 GHz. The wide frequency band (4−9.6 GHz) and thin absorber thickness (1.5−3.5 mm) for effective absorption ( −10 dB) (Figure 6c1). Such remarkable drop of microwave absorption property should be attributed to the dramatic decrease of ε″ due to the absent of free carbon at high Fe loading ratio (Figure 5b). Moreover, it is worth noting that the fibers with PCS/Fer ratio of 3:0.5 exhibit the thinnest absorber thickness at the same frequency compared with other two samples. To better understand this, the frequency dependence of quarter-wavelength (λ/4) of the samples was investigated. The λ/4 cancellation was widely accepted to explain the relationship between RL peak frequency and the absorber thickness.41 In the λ/4 model, the relationship between the absorber thickness (tm) and the peak frequency ( f) can be given by42−45 tm = nc /[(4f )(|εr || μr |)1/2 ]

(n = 1, 3, 5...)

(4)

Parts a2−c2 Figure 6 show the frequency-dependent λ/4 and 3λ/4 of the hybrid fibers. Apparently, all of the samples obey the λ/4 model. The λ/4 line of the 3:0.5 (PCS/Fer) ratio sample lied obviously below the λ/4 lines of the other two samples, indicating that the sample with 3:0.5 (PCS/Fer) ratio offered the thinnest absorber thickness. To date, various 1D SiC hybrid materials, including SiC nanowire,18,46 Fe/SiC whisker,20 and Fe3O4- or Co-doped SiC nanowires,21,22 have been reported as promising microwave absorbers. Table 2 compares the microwave absorption performance of these reported 1D SiC hybrids with our Fe/ SiC hybrid fibers (last line in Table 2). It clearly suggests that the Fe/SiC hybrid fibers exhibit outstanding performance especially in the low frequency C band (4−8 GHz), which is not discovered in other SiC hybrids. In addition, the Fe/SiC hybrid fibers also show the thinnest absorber thickness and relatively low weight fraction. All these advantages enable Fe/ SiC hybrid fibers to be an ideal lightweight microwave absorber.

where Zin is the impedance of the composite backed by the ground plane, Z0 is the intrinsic impedance of free space, d is the thickness of absorber, f is the frequency of incident EM waves, and c is the speed of light. Parts a1−c1 Figure 6 provide the calculated RL curves of SiC fibers and Fe/SiC hybrid fibers. As shown in Figure 6a1, the SiC fibers could achieve effective absorption (RL < −20 dB) above 6 GHz in the investigated frequency band, and a minimum RL of −41.1 was observed at around 12.7 GHz when the thickness was 2.5 mm. In comparison, the Fe/SiC hybrid fibers (PCS: Fer = 3:0.5) exhibited effective absorption in the frequency range of 4−9.6 GHz (Figure 6b1), which covered the entire C band (4−8 GHz), and the minimum RL value of −46.3 dB was reached at 7269

DOI: 10.1021/acsami.6b15721 ACS Appl. Mater. Interfaces 2017, 9, 7265−7271

Research Article

ACS Applied Materials & Interfaces

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Table 2. Microwave Absorption Properties of Some 1D Magnetic/Ceramic Materials samples Fe/ SiCwhisker Fe3O4/ SiCnanowire Co/ SiCnanowire SiCnanowire SiCnanowire Fe/SiCfiber

minimal RL (dB)

dm (mm) (RL< −20 dB)

freq band (GHz) (RL < −20 dB)

wt fraction (%)

ref

−21

2

11.2

20

20

−51

2−5

6−18

50

21

−25

2−4.5

6−18

50

22

−31 −30 −42

1−3 4−5 1.5−3.5

8−8.8 6.5−9 4−9.6

35 50 35

18 46



CONCLUSIONS In conclusion, Fe/SiC hybrid fibers were successfully fabricated via electrospinning and heat treatment afterward. It was found that introducing Fe into SiC not only facilitated the growth of amorphous nanowires on the surface of the SiC fibers but also increased the permittivity and permeability, resulting in a shift of RL peak to lower frequency band. At the optimal PCS/Fe ratio of 3:0.5, the hybrid fiber composite (35 wt % fiber) with a 2.25 mm absorber thickness exhibited a minimal reflection loss of −46.3 dB at 6.4 GHz. Compared with other reported 1D SiC hybrid materials, the Fe/SiC hybrid fibers could achieve effective absorption (