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Bitao Fan, Qiufang Yao, Chao Wang, Ye Xiong, Qingfeng Sun, Chunde Jin, "Spawns Structure of Rod-Like ZnO Wrapped in Cellulose Nanofibers for Electromagnetic Wave Absorption", Journal of Nanomaterials, vol. 2017, Article ID 6329072, 6 pages, 2017. https://doi.org/10.1155/2017/6329072
Spawns Structure of Rod-Like ZnO Wrapped in Cellulose Nanofibers for Electromagnetic Wave Absorption
Spawns structure of rod-like ZnO wrapped in the cellulose nanofibers was successfully fabricated through a facile one-step hydrothermal method, and their electromagnetic wave absorption properties were investigated. The structure and properties of the composite aerogel were characterized. The enlarged morphology images showed that the as-prepared cellulose nanofiber/ZnO samples were spawns structure of rod-like ZnO wrapped in the cellulose nanofibers. The composite aerogel in a wax matrix exhibited excellent electromagnetic wave absorption performance over 2–18 GHz. The widest absorption bandwidth of 30 wt% contained with reflection loss values less than −10 dB was up to 12 GHz (6–18 GHz) at the thickness of 5.5 mm and the minimum reflection loss value reached −26.32 dB at 15.2 GHz when the thickness of the absorber was 3 mm.
The nanosized metal oxides are becoming very potential materials due to their physicochemical properties and various applications in different fields [1, 2]. Among oxide metals, zinc oxide (ZnO) nanoparticle has attracted more attention because the zinc oxide nanoparticle is a promising material for applications in sensors, magnetics, electronics, and photocatalysis. In the past decade, ZnO-based materials had been focused on for a candidate for electromagnetic (EM) wave absorption due to their excellent dielectric properties [3, 4], semiconductive properties , selectable mechanical properties  for a typical structural absorber, and large-scale synthesis [7, 8].
The research of inorganic nanoparticles/polymer composite was a very interesting materials, which could combine the properties of organic and inorganic materials [9, 10]. On the other hand, the inorganic nanoparticles/polymer composite could improve the stability, retain the special morphology, and control the synthesis of nanoparticles . Nanometer-sized single cellulose, the natural polymer, had been extensively used in kinds of fields due to its nanoscale dimensions , high surface area , unique morphology , low density , and high mechanical strength  with the entanglement of high-aspect-ratio  cellulose nanofibers (CNF).
In this study, the spawns structure of rod-like ZnO wrapped in CNF was successfully fabricated for EM wave absorption. In the system of the CNF/ZnO (CNFZ) composite, cellulose nanofibers were used as a scaffold. Combining cellulose and ZnO rods into the spawns structure could be considered as an effective and competitive route to obtain lightweight composites with outstanding EM wave absorbing performance.
2. Material and Methods
Zinc nitrate hexahydrate (Zn(NO3)2·6H2O), hexamethylene tetramine (C6H14N4), and other chemicals were of analytical grade and were produced by Aladdin Industrial Co. The bamboo was obtained from the bamboo forest in Zhejiang, China. All the chemicals were used as received. Deionized water was used in all experiments.
2.2. Preparation of CNF
The purified cellulose after ultrasonic treatment was obtained; refer to Xie et al. . Then the CNF colloid solution was obtained from the suspension after centrifugation at 6000 rpm for 5 minutes. CNF colloid solution was separated into molds and placed in a refrigerator for about 12 h. The frozen samples were freeze-dried for 60 h using a Scientz-18N freeze-dryer to sublime the materials. The cold trap temperature was less than −55°C, and the vacuum pressure was less than 10 μPa during the freeze-drying process. The sponge-like CNF was successfully prepared.
2.3. Preparation of the CNFZ Composite Aerogel
The spawns structure of rod-like ZnO wrapped in CNF was prepared by one-step hydrothermal approach . 100 mg CNF, 3 mmol Zn(NO3)2·6H2O, and 3 mmol C6H14N4 were put into deionized water (100 mL) with magnetic stirring for 10 min at room temperature. Subsequently, the mixtures were transferred to a Teflon-lined stainless-steel autoclave. The autoclave was placed in an oven and heated at 100°C for 120 min. After the suspension was cooled down naturally, the obtained homogeneous suspension was freeze-dried at −55°C at 10 μPa for 60 h. The lightweight, solid, and sponge-like CNFZ aerogel was successfully fabricated.
The morphological feature of the CNF and CNFZ was observed using scanning electron microscope (SEM, FEI, Quanta 200, USA) and transmission electron microscope (TEM, FEI, Tecnai G20, USA). Crystalline structures were identified by X-ray diffraction technique (XRD, Rigaku, D/MAX 2200, Japan) operating with Cu Kα radiation (λ = 1.5418 Å) at a scan rate (2θ) of 4° min−1 and the accelerating voltage of 40 kV and the applied current of 30 mA ranging from 5° to 75°. The X-ray photoelectron spectroscopy (XPS, ULVAC–PHI, Inc., Japan) analysis of the specimen was carried out using a microfocused (100 lm, 25 W, 15 kV) monochromatic Al-Ka source ( = 1486.6 eV), a hemispherical analyzer, and a multichannel detector. The composite samples used for EM wave absorption measurement were prepared by mixing the aerogel with paraffin wax 30 wt% of the aerogel. The EM wave absorption of the mixtures at 2–18 GHz frequency range was measured by using an Agilent E8363B vector network analyzer.
3. Results and Discussion
Figure 1 showed the morphological features of CNF and CNFZ. As shown in Figure 1(a), it could be observed that the slender fibers were cross-linked with a length of 150 μm. Figure 1(b) showed TEM image of CNF, which exhibited some slender fibrils with average diameter of 56.3 nm. It could be concluded that the CNF had a large length-diameter ratio of about 2664. Figure 1(c) showed the SEM image of CNFZ. After the hydrothermal reaction, spawns structure of ZnO rods wrapped in the CNF was formed. Figure 1(d) showed the enlarged image of the spawns structure. Figure 1(e) showed the selected-area electron diffraction (SAED) pattern of CNFZ which indicated that a single rod was a single crystal. HRTEM image was shown in Figure 1(f). It was clearly revealed that lattice fringe with a spacing value of 0.28 nm depicts the lattice-resolved (100) crystalline plane of hexagonal ZnO.
Figure 2 showed the XRD patterns of the CNF and CNFZ. As shown in Figure 2(a), it was clear that the diffraction peaks in XRD pattern at 2θ = 16.5° and 22.5° were typical cellulose structure. In the case of CNFZ, the peaks of cellulose still exist in Figure 2(b), revealing that the crystal structure of cellulose did not change after the hydrothermal treatment. Furthermore, the additional diffraction peaks of CNFZ were observed at 31.75°, 34.5°, 36.3°, 47.5°, 56.6°, 62.9°, 66.4°, 68.0°, and 69.1° corresponding to the planes of (100), (002), (101), (102), (110), (103), (200), (112), and (201), which could be indexed to the hexagonal ZnO (wurtzite, JCPDS Number 36-1451).
Figure 3 showed the XPS spectra of the CNF and CNFZ. As shown in Figure 3(a), the wide scan spectra of the CNF exhibited two major peaks with binding energy at 286.1 eV and 532.1 eV corresponding to the C 1s and O 1s of CNF, respectively. However, in the CNFZ, it exhibited four major peaks with binding energy at 286.1 eV, 532.1 eV, 1021.4 eV, and 1044.4 eV corresponding to the C 1s (286.1 eV), O 1s (532.1 eV), and Zn 2p (1021.4 eV and 1044.4 eV) of CNFZ, respectively, which could indicate that the Zn element was added in the sample of CNFZ. The high-resolution XPS spectra of key elements (C 1s and O 1s) and extra element (Zn 2p) were carried out and were shown in Figures 3(b)–3(f). As shown in Figure 3(b), the binding energies of Zn appeared at 1021.37 eV and 1044.47 eV (Figure 3(b)), respectively, which could be well attributed to the Zn element. It could be concluded that ZnO has been produced in CNFZ successfully. Figure 3(c) showed three peaks observed at 284.9 eV, 286.3 eV, and 287.9 eV in the high-resolution spectra of C 1s in CNF, which clearly indicated the presence of C-C, C-O, and O-C-O. Upon hydrothermal reaction, the high-resolution C 1s spectrum of CNFZ (Figure 3(d)) showed similar results to those of CNF. The same peaks were located in the same places. The differences in the same peak on intensity at 284.9 eV were attributed to C-C; the results might be attributed to some degradation during hydrothermal treatment. Two peaks which attributed to O-H and O-C-O and C-O-C were observed at 532.8 eV in the high-resolution spectra of O 1s in CNF (Figure 3(e)). Another peak was observed at 530.12 eV in the high-resolution spectra of O 1s in CNFZ except the two peaks in the high-resolution spectra of O 1s in CNF at the same location (Figure 3(f)). The additional peak could be attributed to the original lattice oxygen species in ZnO . According to the above results, it could be deduced that ZnO would have been produced in CNFZ successfully.
Figure 4 showed the formation mechanism of the spawns structure of rod-like ZnO wrapped in CNF. A possible mechanism could be inferred from the basic physics of electrostatic interaction between positively charged ZnO and negatively charged CNF. Firstly, spawns structure of ZnO wrapped in CNF was prepared by a hydrothermal method. When C6H14N4 and Zn(NO3)2 were added in cellulose nanofibers solution at 100°C for 120 min, ZnO crystal seed was proceeding and homogeneously distributed in the solution. With the ZnO rods growing, spawns structure of rod-like ZnO wrapped in CNF was created by an electrostatic interaction between positively charged ZnO and negatively charged CNF. Therefore, CNF could be close to ZnO rods and wrapped ZnO rods like a net acted as a shell. Subsequently, freeze-drying was carried out to sublimate the liquid into gas phase. The lightweight aerogel with the structure of ZnO spawns wrapped in cellulose nanofibers was fabricated.
Figure 5 showed the reflection loss (RL) values versus frequency of the CNFZ at different thickness (1–5.5 mm) with a filler loading of 30 wt%. It could be observed that the CNFZ exhibited a certain degree of abilities for EM wave absorption. The different thickness of the CNFZ had a great influence on the frequency of electromagnetism wave absorption properties. When the thickness increased, the frequency of RL peak had a tendency to shift from high frequency to low frequency. The value reached −26.32 dB at 15.2 GHz when the thickness of the absorber was 3 mm. Importantly, the widest absorption bandwidth corresponding to RL value less than −10 dB was almost up to 12 GHz (6.0–18.0 GHz) at the thickness of 5.5 mm. In order to increase the properties of absorption for EM, many researches had been conducted in the previous investigation. The summary of results for EM absorption employed by different structure of ZnO was shown in Table 1. The RL behaviors of CNFZ usually depend on their loss mechanisms, which are determined by their nature and structure. The above results indicated that the spawns structure of rod-like ZnO wrapped in CNF had strong absorption for EM. This was mainly because of the interfacial electric polarization. It can be noticed that the spawns structure of rod-like ZnO wrapped in CNF had unique multiple interfaces between the rod-like ZnO, CNF, paraffin matrix, and air bubbles. It is available for the EM to penetrate the porous layer formed by the multiple poles at the interfaces and the energy will be induced into dissipative current, which leads to the energy attenuation.
Spawns structure of rod-like ZnO wrapped in CNF was successfully fabricated through a facile hydrothermal process. CNF could be close to ZnO rods and wrapped ZnO rods like spawns structure due to the basic physics of electrostatic interaction between positively charged ZnO and negatively charged CNF. The composite aerogel in a wax matrix exhibits excellent EM wave absorption performance. The widest absorption bandwidth with RL values less than −10 dB was up to 12 GHz (6–18 GHz) and the minimum RL value reached −26.32 dB at 15.2 GHz.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this manuscript.
This work was supported by Zhejiang Provincial Natural Science Foundation of China (no. LZ14C160001), Scientific Research Foundation of Zhejiang A&F University (Grant no. 2014FR077), Public Projects of Zhejiang Province (no. 2015C32014), and the Fund for Innovative Research Team of Forestry Engineering Discipline (101-206001000713).
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