Journal of Nanomaterials

Journal of Nanomaterials / 2013 / Article

Research Article | Open Access

Volume 2013 |Article ID 591893 | 7 pages |

Facile Preparation, Characterization, and Highly Effective Microwave Absorption Performance of CNTs/Fe3O4/PANI Nanocomposites

Academic Editor: John Zhanhu Guo
Received05 Sep 2013
Accepted03 Oct 2013
Published12 Nov 2013


A facile method has been developed to synthesize light-weight CNTs/Fe3O4/PANI nanocomposites. The formation route was proposed as the coprecipitation of Fe2+ and Fe3+ and an additional process of in situ polymerization of aniline monomer. The structure and morphology of CNTs/Fe3O4/PANI were characterized by transmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), and Fourier transform infrared (FTIR) spectroscopy. The TEM investigation shows that the CNTs/Fe3O4/PANI nanocomposites exhibit less intertwined structure and that many more Fe3O4 particles are attached homogeneously on the surface of CNTs, indicating that PANI can indeed help CNTs to disperse in isolated form. The wave-absorbing properties were investigated in a frequency of 2–18 GHz. The results show that the CNTs/Fe3O4/PANI nanocomposites exhibit a super absorbing behavior and possess a maximum reflection loss of −48 dB at 12.9 GHz, and the bandwidth below −20 dB is more than 5 GHz. More importantly, the absorption peak frequency ranges of the CNTs/Fe3O4/PANI composites can be tuned easily by changing the wax weight ratio and thickness of CNTs/Fe3O4/PANI paraffin wax matrix.

1. Introduction

With the rapid increase in the use of telecommunications, digital systems, and fast processors, electromagnetic interference (EMI) has become a great concern. A microwave absorber is a kind of functional material that can absorb electromagnetic (EM) waves effectively and convert EM energy into thermal energy or make EM waves dissipate by interference [1]. Over the past decade, a variety of materials used as microwave absorbers have been extensively studied with increasing demand for innovative EMI shielding [26]. Among the pursued materials, carbon nanotubes (CNTs) have attracted extensive development effort for their unique structural, high electrical conductivity, outstanding chemical stability, and mechanical properties [79]. However, excellent microwave absorption properties cannot be obtained for unmodified CNTs because their magnetic loss is so small [10]. To optimize the performances of CNTs as microwave absorbers, it is necessary to modify CNTs by decorating other nanomaterials, which are expected to exhibit ideal electromagnetic absorption properties [11, 12].

In recent years, more and more research has been conducted in decorating CNTs with iron oxide and preparing magnetic nanoparticles due to their unique magnetic features, low cost, and strong absorption characteristics [13, 14]. Various chemistry-based processing routes have been developed to synthesize iron oxide/CNTs nanocomposite. Correa-Duarte et al. [15] coated CNTs with iron oxide nanoparticles (magnetite/maghemite) via a layer by layer assembly technique and aligned CNTs chains in relatively small external magnetic fields. Youn et al. [16] decorated single walled carbon nanotubes (SWNTs) with iron oxide nanoparticles along the nanotube via a magnetoevaporation method. In addition, Jia et al. [17] initiated the self-assembly of magnetite particles along multiwalled CNTs via a hydrothermal process. However, there are still disadvantages in most of these processes, which mainly include the points as follows: Fe3O4 materials usually suffer from ease of oxidation and relatively narrow absorption frequency range, which hamper their applications, and the dispersion of the nanocomposite is poor, and the orientation of the deposition of Fe3O4 nanoparticles on the surfaces of CNTs is difficult to control.

In order to solve these problems, here in this report the CNTs/Fe3O4/PANI nanocomposites were fabricated by the coprecipitation of Fe2+ and Fe3+ and an additional process of in situ polymerization of aniline monomer. Polyaniline (PANI), polymerized from the inexpensive aniline monomer, was considered as an ideal matrix or a second phase incorporated with CNTs for its unique electromagnetic shielding and attenuation [18]. Furthermore, the facile preparation, structure characterization, and wave absorption performance of CNTs/Fe3O4/PANI nanocomposite materials were investigated. The effects of several factors on wave absorption properties of CNTs/Fe3O4/PANI nanocomposites were discussed.

2. Experimental Section

2.1. The Pretreatment of MWCNTs

MWCNTs (purity >95 wt%, 20–30 nm outer diameter, 10–30 μm length) were purchased from Chengdu Organic Chemicals Co. Ltd, Chinese Academy of Science. The as-supplied MWCNTs were processed in concentrated sulfuric acid with vigorous ultrasonic vibration treatment (30 W, 40 kHz) for 2 h at 50°C. After that, the mixture was followed by vacuum filtration, and washed with deionized water until the pH value of washing solution is neutral. Then, the filtered solid was dried under vacuum for 24 h at 60°C, obtaining acidulated MWCNTs.

2.2. The Preparation of CNTs/Fe3O4/PANI Nanocomposite Materials

was employed as the precursor for the synthesis of Fe3O4 magnetic nanoparticles. (1.0 g) was dissolved first in a mixture of deionized water (15 mL) and hydrazine hydrate solution (5 mL) with a volume ratio of 3 : 1 under constant stirring. Then, 0.4 g of acidulated MWCNTs was added into the above solution. After 30 min ultrasonic vibration, a black suspension with homogeneously dispersed MWCNTs was obtained. Ammonia water (1.0 mol/L) was then added until the pH value of the solution was 11.0. The stable aqueous suspension was subsequently long-drawn reflux condensed in a thermostatic water bath at the temperature of 100°C. After approximately 2 h, the products were cooled to room temperature. Meanwhile, the obtained products were quickly redispersed in 30 mL deionized water. Benzenesulfonic acid with certain concentration (1.5 mol/L) and aniline (0.2 g) was subsequently added. Until homogenous suspension was achieved, ammonium persulfate (APS) aqueous solution (0.2 g of APS in 20 mL of deionized water) was dropwise added to the suspension. The polymerization process was applied in an ice bath for 6 h under vigorous stirring. The resulting precipitations were washed with deionized water and absolute ethanol several times to remove the remaining impurities. In the next step, the as-prepared product was dried under vacuum for 24 h at 60°C.

3. Characterization

The morphology and size distribution of the samples were investigated by means of transmission electron microscopy (TEM, JEM-2010F, Germany). The ferroferric oxide nanoparticle in CNTs/Fe3O4/PANI nanocomposites was examined specially by X-ray photoelectron spectroscopy (XPS). Fourier transform infrared spectroscopy (FTIR) was carried out on a Nicolet 8700 FTIR system. The reflection loss was measured with an Anritsu 37269D vector network analyzer in the 2–18 GHz range for which the samples were prepared by uniformly mixing the CNTs/Fe3O4/PANI nanocomposites in a paraffin matrix which is pressed in a cylindrical shape with thickness of 2.00 mm.

4. Results and Discussion

4.1. TEM Images of CNTs/Fe3O4/PANI and CNTs/Fe3O4

The typical morphology of the as-prepared CNTs/Fe3O4/PANI is shown in Figure 1(a). As a comparison, CNTs/Fe3O4 samples prepared without PANI are presented in Figure 1(b), demonstrating smaller average diameter observed in the latter because of the nonexistence of PANI coating. What is more, in Figure 1(b) samples of CNTs/Fe3O4 prepared without PANI seem to be a bundle that CNTs are intertwined with each other and that Fe3O4 magnetic nanoparticles aggregate closely. However, the samples prepared in the presence of PANI (shown in Figure 1(a)) exhibit less entangled structure due to the wrapping of PANI. In other words, the use of PANI as a dispersant in the preparation process of CNTs/Fe3O4 can indeed help CNTs to disperse as individuals or smaller bundles. On the other hand, the TEM image of CNTs/Fe3O4/PANI also indicates that a large number of Fe3O4 nanoparticles adhered on the CNTs are distributed relatively homogeneously and with tiny diameters in the range of 3–5 nm; promising CNTs/Fe3O4/PANI nanocomposites prepared with PANI may have higher magnetic properties and absorption characteristics. Furthermore, it is noticeable that the interaction between Fe3O4 nanoparticles and CNTs was strong in the presence of PANI, as few Fe3O4 nanoparticles were observed on the copper grids suffering from repeated washing and sonicating in the process.

4.2. XPS Analysis of CNTs/Fe3O4/PANI

XPS has often been used for the surface characterization of various materials, and unambiguous results are readily obtained when the various surface components each contain unique elemental markers. Here, in order to further analyse the CNTs/Fe3O4/PANI products, XPS was measured to understand the composition of the magnetic nanoparticles surface in Figure 2. Figure 2(a) shows the XPS signals of the Fe 2p region. Two peaks of Fe 2p1/2 at 710.6 eV and Fe 2p3/2 at 723.9 eV were observed, respectively. The O 1s spectrum in Figure 2(b) consisted of a mean peak originating from the oxygen in Fe3O4 (at 529.7 eV) and a shoulder centered at 531.3 eV, which has been ascribed to surface traps [19]. The Fe/O ratio was estimated as 0.74 with curve resolution analysis, which matches well with the stoichiometric ratio of Fe3O4 (0.75). The data are also consistent with the values reported for Fe3O4 in the literature [2022]. Therefore, XPS results also prove the composition of the products.

4.3. FTIR Analysis of CNTs/Fe3O4/PANI

FTIR spectra of samples were recorded at room temperature, which are shown in Figure 3. Figure 3(a) shows the results of neat PANI. Figure 3(b) shows the CNTs/Fe3O4/PANI samples prepared in the presence of PANI. For the CNTs/Fe3O4/PANI nanocomposite, the peaks appearing at 3268, 1587, 1496, 1310, 1165, and 832 cm−1 indicate the formation of PANI. The peaks at 1587 and 1496 cm−1 are assigned to the stretching vibration of C=N in quinoid ring and C=C in benzenoid ring [23]. The peak at 3268 cm−1 is attributed to the N−H stretching vibration in PANI [23]. However, compared with the spectra of the PANI, the peaks of the CNTs/Fe3O4/PANI nanocomposites shifted slightly in the direction of low wavenumber. This may be attributed to the interaction between the CNTs and the PANI [24]. What is more, owing to lower concentrations of PANI in CNTs/Fe3O4/PANI samples and the introduction of the CNTs, the intensity of the peaks of the CNTs/Fe3O4/PANI nanocomposite decreased.

4.4. Reaction Mechanism Explanation of As-Prepared CNTs/Fe3O4/PANI

In view of the unique and facile synthesis process, the reaction mechanism of CNTs/Fe3O4/PANI nanocomposites is schematically illustrated in Figure 4. It is well known that treating the CNTs with sulfuric acid could create considerable functional groups such as carboxyl or carbonyl on the outside surface of CNTs which became negatively charged. The large number of the carboxylic acid or carbonyl groups on the outside of the CNTs could catch and strongly bond with Fe2+ ions in solution through electrostatic attraction. Then, after the addition of N2H4 solution, many primary Fe2+ ions further interacted with N2H4 into Fe3+ ions under alkaline condition (PH = 11–13). In the following long-drawn reflux process, large quantities of obtained Fe3+ ions and incipient unreacted Fe2+ ions went through intensive coprecipitation reaction. Finally the Fe3O4 magnetic nanoparticles formed and adhered on the surface of CNTs driven by the minimization of surface energy. The OH ions play an important role in the formation of Fe3O4 magnetic nanoparticles. When creating OH ions took place in the aqueous solution, the OH, as an inorganic ligand, would first interact with Fe2+ forming Fe(OH)2. This will promote the further interaction between Fe(OH)2 and N2H4 so that the obtained Fe(OH)3 could combine with Fe(OH)2 under the favourable OH condition. The reaction processes can be briefly described as Then, the in situ polymerization happened in the quick process, which seemingly improved the distribution of Fe3O4 magnetic nanoparticles, getting the fine CNTs/Fe3O4/PANI nanocomposites (Figure 1(a)).

4.5. Microwave Absorption Theory

For the microwave absorption properties, the samples were first disposed by mixing with paraffin wax in an ether solution, followed by evaporating the solvent. The dried samples were collected and compressed into a toroidal shape. The reflection loss (RL) values of CNTs/Fe3O4/PANI and CNTs/Fe3O4 composites were calculated using the relative complex permittivity and permeability at a given frequency and thickness layer according to the transmit line theory, which is summarized as the following equations [25]: where and are the relative complex permittivity and permeability of the composite medium, respectively, is the frequency of the microwave in free space, is the velocity of light, is the absorber thickness, and is the input impedance of the absorber.

4.6. The Comparison of Microwave Absorption Properties between CNTs/Fe3O4/PANI and CNTs/Fe3O4

Figure 5 shows the reflection loss characteristics curve of the CNTs/Fe3O4/PANI and CNTs/Fe3O4 samples under the same paraffin wax weight ratio (20 wt%) condition, which was calculated by the previous equations (4) and (5). In this calculation, was considered to be 2 mm. The samples prepared with PANI exhibit the largest reflection loss of −48 dB at 12.9 GHz, which is in an interval width of 5.2 GHz with losses all below −20 dB. The samples prepared without PANI have a maximum reflection loss of −44 dB at 13.1 GHz with about 5.5 GHz bandwidth below −20 dB. In the comparison of CNTs/Fe3O4/PANI with CNTs/Fe3O4, the CNTs/Fe3O4/PANI samples with PANI have the largest reflection loss of −48 dB, which is higher than that of samples without PANI, while the frequency region (below −20 dB) between the two is approximated. These results indicate that the samples prepared with PANI have relative better absorption properties than those of samples without PANI. Normally, microwave absorption depends on the impedance match conditions of the interfaces between the fillers and air [26]. Thus, the existence of PANI coatings with a different electrical conductivity and dielectric properties could change the impedance between CNTs and air, leading to CNTs/Fe3O4 microwave absorption performance superior to CNTs/Fe3O4/PANI composites. However, the results display the deviation which can be attributed to the dispersion of the CNTs/Fe3O4/PANI samples, which is better than that of the samples prepared without PANI. It is further proved that the dispersion of the CNTs/Fe3O4 nanocomposites is poor, and the orientation of the deposition of Fe3O4 nanoparticles on the surfaces of CNTs is difficult to control. Also, it is worth noting that the reflection loss results of both are much more effective than those of many naked CNT composites in previous reports [27, 28].

4.7. The Effects of Several Factors on Wave Absorption Properties of CNTs/Fe3O4/PANI

Figure 6(a) presents the experimental results of the reflection loss versus frequency for CNTs/Fe3O4/PANI wax composites with the increase of paraffin wax weight ratio from 10 to 25 wt% in the range of 2–18 GHz. The CNTs/Fe3O4/PANI composites with a paraffin wax weight ratio of 10 wt% show weak wave-absorbing ability, and the absorption peak increases to 33 dB at paraffin wax weight ratio of 15 wt% and then reaches the maximum value of 48 dB at the paraffin wax weight ratio of 20 wt%. But with further increasing paraffin wax weight ratio, the wave-absorbing ability decreases. Also, it is clearly seen that the peak position moves to lower frequencies with increasing paraffin wax weight. In addition, we also explored the influence of absorber thickness on wave-absorbing performance by calculation. The absorber thickness () was considered to be 1, 1.5, 2, 2.5, 3, 3.5, and 4 mm, respectively. The evaluated reflection loss of CNTs/Fe3O4/PANI composites coupled with different thicknesses is shown in Figure 6(b). It is obviously exhibited that the reflection loss peaks shift from higher to lower frequency as the thickness increases, associated with quarter-wavelength attenuation [29]. Furthermore, the CNTs/Fe3O4/PANI composites demonstrate excellent microwave absorption performance with wide absorption bandwidth in an effective range of thickness. In the investigated region, the maximum reflection loss peak achieves up to 48 dB (2 mm in thickness). These results above are of importance since the absorption peak frequency ranges of the CNTs/Fe3O4/PANI composites can be tuned easily by changing the wax weight ratio and absorber thickness, and thus a broadband and effective absorption design could be achieved using CNTs/Fe3O4/PANI composite nanomaterials.

5. Conclusions

In summary, we have developed a simple method to synthesize the CNTs/Fe3O4/PANI composite nanostructures. The Fe3O4 magnetic nanoparticles have the diameters of 3–5 nm. The Fe3O4 nanoparticles were strongly attached to the surface of CNTs by the action of PANI. The CNTs/Fe3O4/PANI composites reveal super microwave absorption properties and possess a maximum reflection loss of −48 dB at 12.9 GHz, and the bandwidth below −20 dB is more than 5 GHz, which is much higher than many CNT-based samples. In addition, the absorption peak frequency ranges of the CNTs/Fe3O4/PANI composites can be tuned by changing the wax weight ratio and its thickness. All the results indicate that the CNTs/Fe3O4/PANI composite nanomaterials may be attractive candidate materials for microwave absorption applications.


This work was supported by the National Science Foundation of China (Grant nos. 50972014, 51072024, and 51132002).


  1. C. Tong, Advanced Materials and Design for Electromagnetic Interference, Taylor & Francis, Boca Raton, Fla, USA, 2008.
  2. J. Zhu, S. Wei, N. Haldolaarachchige, D. P. Young, and Z. Guo, “Electromagnetic field shielding polyurethane nanocomposites reinforced with core-shell Fe-silica nanoparticles,” Journal of Physical Chemistry C, vol. 115, no. 31, pp. 15304–15310, 2011. View at: Publisher Site | Google Scholar
  3. H. Gu, Y. Huang, X. Zhang et al., “Magnetoresistive polyaniline-magnetite nanocomposites with negative dielectrical properties,” Polymer, vol. 53, no. 3, pp. 801–809, 2012. View at: Publisher Site | Google Scholar
  4. X. Zhang, S. Y. Wei, N. Haldolaarachchige, and H. A. Colorado, “Magnetoresistive conductive polyaniline-barium titanate nanocomposites with negative permittivity,” Journal of Physical Chemistry C, vol. 116, no. 29, pp. 15731–15740, 2012. View at: Publisher Site | Google Scholar
  5. H. Li, Y. Huang, G. Sun et al., “Directed growth and microwave absorption property of crossed ZnO netlike micro-/nanostructures,” Journal of Physical Chemistry C, vol. 114, no. 22, pp. 10088–10091, 2010. View at: Publisher Site | Google Scholar
  6. S. J. Yan, L. Zhen, C. Y. Xu, J. T. Jiang, W. Z. Shao, and J. K. Tang, “Synthesis, characterization and electromagnetic properties of Fe1xCox alloy flower-like microparticles,” Journal of Magnetism and Magnetic Materials, vol. 323, no. 5, pp. 515–520, 2011. View at: Publisher Site | Fe1xCox%20alloy%20flower-like%20microparticles&author=S. J. Yan&author=L. Zhen&author=C. Y. Xu&author=J. T. Jiang&author=W. Z. Shao&author=&author=J. K. Tang&publication_year=2011" target="_blank">Google Scholar
  7. R. H. Baughman, A. A. Zakhidov, and W. A. De Heer, “Carbon nanotubes—the route toward applications,” Science, vol. 297, no. 5582, pp. 787–792, 2002. View at: Publisher Site | Google Scholar
  8. Y. Shan, K. Chen, X. Yu, and L. Gao, “Preparation and characterization of biocompatible magnetic carbon nanotubes,” Applied Surface Science, vol. 257, no. 2, pp. 362–366, 2010. View at: Publisher Site | Google Scholar
  9. L. Zhang, Q.-Q. Ni, T. Natsuki, and Y. Fu, “Carbon nanotubes/magnetite hybrids prepared by a facile synthesis process and their magnetic properties,” Applied Surface Science, vol. 255, no. 20, pp. 8676–8681, 2009. View at: Publisher Site | Google Scholar
  10. R. Che, L.-M. Peng, X. Duan, Q. Chen, and X. Liang, “Microwave absorption enhancement and complex permittivity and permeability of Fe encapsulated within carbon nanotubes,” Advanced Materials, vol. 16, no. 5, pp. 401–405, 2004. View at: Google Scholar
  11. F. S. Wen, F. Zhang, and Z. Y. Liu, “Investigation on microwave absorption properties for multiwalled carbon nanotubes/Fe/Co/Ni nanopowders as lightweight absorbers,” Journal of Physical Chemistry C, vol. 115, no. 29, pp. 14025–14030, 2011. View at: Publisher Site | Google Scholar
  12. X.-L. Shi, M.-S. Cao, J. Yuan, and X.-Y. Fang, “Dual nonlinear dielectric resonance and nesting microwave absorption peaks of hollow cobalt nanochains composites with negative permeability,” Applied Physics Letters, vol. 95, no. 16, Article ID 163108, 2009. View at: Publisher Site | Google Scholar
  13. K. Jia, R. Zhao, J. Zhong, and X. Liu, “Preparation and microwave absorption properties of loose nanoscale Fe3O4 spheres,” Journal of Magnetism and Magnetic Materials, vol. 322, no. 15, pp. 2167–2171, 2010. View at: Publisher Site | Google Scholar
  14. S. B. Ni, X. L. Sun, X. H. Wang et al., “Low temperature synthesis of Fe3O4 micro-spheres and its microwave absorption properties,” Materials Chemistry and Physics, vol. 124, no. 1, pp. 353–358, 2010. View at: Publisher Site | Google Scholar
  15. M. A. Correa-Duarte, M. Grzelczak, V. Salgueiriño-Maceira et al., “Alignment of carbon nanotubes under low magnetic fields through attachment of magnetic nanoparticles,” Journal of Physical Chemistry B, vol. 109, no. 41, pp. 19060–19063, 2005. View at: Publisher Site | Google Scholar
  16. S. C. Youn, D.-H. Jung, Y. K. Ko, Y. W. Jin, J. M. Kim, and H.-T. Jung, “Vertical alignment of carbon nanotubes using the magneto-evaporation method,” Journal of the American Chemical Society, vol. 131, no. 2, pp. 742–748, 2009. View at: Publisher Site | Google Scholar
  17. B. Jia, L. Gao, and J. Sun, “Self-assembly of magnetite beads along multiwalled carbon nanotubes via a simple hydrothermal process,” Carbon, vol. 45, no. 7, pp. 1476–1481, 2007. View at: Publisher Site | Google Scholar
  18. B. Q. Yuan, L. M. Yu, L. M. Sheng, K. An, and X. L. Zhao, “Comparison of electromagnetic interference shielding properties between single-wall carbon nanotube and graphene sheet/polyaniline composites,” Journal of Physics D, vol. 45, Article ID 235108, 2012. View at: Publisher Site | Google Scholar
  19. T. Fujii, F. M. F. De Groot, G. A. Sawatzky, F. C. Voogt, T. Hibma, and K. Okada, “In situ XPS analysis of various iron oxide films grown by NO2-assisted molecular-beam epitaxy,” Physical Review B, vol. 59, no. 4, pp. 3195–3202, 1999. View at: Google Scholar
  20. S. Y. Lian, Z. H. Kang, E. B. Wang, M. Jiang, C. Hu, and L. Xu, “Convenient synthesis of single crystalline magnetic Fe3O4 nanorods,” Solid State Communications, vol. 127, no. 9-10, pp. 605–608, 2003. View at: Publisher Site | Google Scholar
  21. W. Kim, K. Kawaguchi, N. Koshizaki, M. Sohma, and T. Matsumoto, “Fabrication and magnetoresistance of tunnel junctions using half-metallic Fe3O4,” Journal of Applied Physics, vol. 93, no. 10, pp. 8032–8034, 2003. View at: Publisher Site | Google Scholar
  22. J. G. Deng, Y. X. Peng, C. L. He, X. Long, P. Li, and A. S. C. Chan, “Magnetic and conducting Fe3O4-polypyrrole nanoparticles with core-shell structure,” Polymer International, vol. 52, no. 7, pp. 1182–1187, 2003. View at: Publisher Site | Google Scholar
  23. M. Amrithesh, S. Aravind, S. Jayalekshmi, and R. S. Jayasree, “Enhanced luminescence observed in polyaniline-polymethylmethacrylate composites,” Journal of Alloys and Compounds, vol. 449, no. 1-2, pp. 176–179, 2008. View at: Publisher Site | Google Scholar
  24. M. G. Deng, B. C. Yang, and Y. D. Hu, “Polyaniline deposition to enhance the specific capacitance of carbon nanotubes for supercapacitors,” Journal of Materials Science, vol. 40, no. 18, pp. 5021–5023, 2005. View at: Publisher Site | Google Scholar
  25. R. Che, L.-M. Peng, X. Duan, Q. Chen, and X. Liang, “Microwave absorption enhancement and complex permittivity and permeability of Fe encapsulated within carbon nanotubes,” Advanced Materials, vol. 16, no. 5, pp. 401–405, 2004. View at: Publisher Site | Google Scholar
  26. M.-S. Cao, W.-L. Song, Z.-L. Hou, B. Wen, and J. Yuan, “The effects of temperature and frequency on the dielectric properties, electromagnetic interference shielding and microwave-absorption of short carbon fiber/silica composites,” Carbon, vol. 48, no. 3, pp. 788–796, 2010. View at: Publisher Site | Google Scholar
  27. Z. J. Fan, G. H. Luo, Z. F. Zhang, L. Zhou, and F. Wei, “Electromagnetic and microwave absorbing properties of multi-walled carbon nanotubes/polymer composites,” Materials Science and Engineering B, vol. 132, no. 1-2, pp. 85–89, 2006. View at: Publisher Site | Google Scholar
  28. Z. F. Liu, G. Bai, Y. Huang et al., “Microwave absorption of single-walled carbon nanotubes/soluble cross-linked polyurethane composites,” Journal of Physical Chemistry C, vol. 111, no. 37, pp. 13696–13700, 2007. View at: Publisher Site | Google Scholar
  29. W.-L. Song, M.-S. Cao, B. Wen, Z.-L. Hou, J. Cheng, and J. Yuan, “Synthesis of zinc oxide particles coated multiwalled carbon nanotubes: Dielectric properties, electromagnetic interference shielding and microwave absorption,” Materials Research Bulletin, vol. 47, no. 7, pp. 1747–1754, 2012. View at: Publisher Site | Google Scholar

Copyright © 2013 Deqing Zhang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1405 Views | 928 Downloads | 7 Citations
 PDF  Download Citation  Citation
 Download other formatsMore
 Order printed copiesOrder