下載本文檔
版權(quán)說明:本文檔由用戶提供并上傳,收益歸屬內(nèi)容提供方,若內(nèi)容存在侵權(quán),請進(jìn)行舉報或認(rèn)領(lǐng)
文檔簡介
1、<p> 中文3050字,2200單詞,11500英文字符</p><p> 文獻(xiàn)出處:Liu J R, Itoh M, Machida K. Electromagnetic wave absorption properties of α-Fe/Fe 3B/Y2O3 nanocomposites in gigahertz range[J]. Applied Physics Letters, 2003
2、, 83(19):4017-4019.</p><p><b> 原文1</b></p><p> Electromagnetic wave absorption properties of a-Fe/Fe3B/Y2O3nanocomposites in gigahertz range</p><p> Jiu Rong Liu, Mas
3、ahiro Itoh, and Ken-ichi Machidaa)</p><p> a Collaborative Research Center for Advanced Science and Technology Osaka University, 2-1 Yamadaoka,</p><p> Suita, Osaka 565-0871, Japan</p>
4、<p> (Received 24 February 2003; accepted 8 September 2003)</p><p> Abstract: Nanocomposites a-Fe/Fe3B/Y2O3 were prepared by a melt-spun technique, and the electromagneticwave absorption properties we
5、re measured in the 0.05–20.05 GHz range. Compared witha-Fe/Y2O3 composites, the resonance frequency (fr) of a-Fe/Fe3B/Y2O3 shifted to a higher frequency range due to the large anisotropy ?eld (HA) of tetragonal Fe3B (~0.
6、4 MA/m). The relative permittivity () was constantly low over the 0.5–10 GHz region, which indicates that the composite powders have a high resistiv</p><p> Keywords: Nanocomposites a-Fe/Fe3B/Y2O3; Electrom
7、agnetic; Absorption performance </p><p> 1. Introduction</p><p> Recent employment of communication devices using the electromagnetic wave range of 1–6 GHz, (e.g., mobile telephones, intellig
8、ent transport systems, electronic toll collection systems, and local area network systems)has rapidly expanded. Therefore, serious electromagnetic interference problems have worsened. Concern for these problems has promp
9、ted the study of electromagnetic wave absorbing materials with antielectromagnetic interference coatings, self-concealing technology, and microwave darkro</p><p> The complex permeability () and permittivit
10、y() of materials determine the re?ection and attenuation characteristics of the electromagnetic wave absorbers. For magnetic electromagnetic wave absorbers, there is a relationship between absorber thickness (dm) and mag
11、neticloss () according to the Eq. (1):</p><p><b> (1)</b></p><p> where c is velocity of light and fm the matching frequency.Metallic magnetic materials have a large saturation mag
12、netization and the Snoek’s limit is at the high frequency[1–3]. Consequently, their complex permeability values still remain high in such high frequency range. Therefore, it is possible to make thin absorbers from these
13、materials. However, the magnetization of these materials decreases due to eddy current losses induced by electromagnetic wave. For this reason,it is better to use sma</p><p> Sugimoto et al. have reported t
14、he good electromagnetic wave absorption properties of a-Fe/SmO composites in the 0.73-1.3 GHz range derived from a rare earth intermetallic compound Sm2Fe17 prepared by a conventional arc-melting technique[4,5]. We also
15、have reported that a-Fe/Y2O3 composites prepared by melt-spun technique showed good electromagnetic wave absorption properties in the 2.0–3.5 GHz range due to the ?ne particle size of a-Fe (~20 nm)[6].</p><p&g
16、t; 2. Experimental procedure</p><p> 2.1. Materials preparation</p><p> Rare earth magnets of nanocomposite materials, such as Fe3B/Nd2Fe14B, have been noted as high-performance magnets, whic
17、h could be fabricated by annealing the amorphous melt-spun ribbons7,8. The microstructure of nanocomposites is strongly dependent on the annealing temperature and time as well as the alloy composition. The purpose of thi
18、s study was to investigate the electromagnetic wave absorption properties of a-Fe/Fe3B/Y2O3 nanocomposites, which are prepared from Fe3B/Nd2Fe14B, and compare th</p><p> 2.2. Characterization</p><
19、;p> Ternary alloy ingots of Y5Fe77.5B17.5 were ?rst prepared from Y, Fe, and B metals (>99.9 % in purity) by means of induction melting in Ar. Amorphous Y5Fe77.5B17.5 alloy ribbons with 1.5 mm in width and about 3
20、0 mm in thickness were prepared by the single-roller melt-spun apparatus at a roll surface velocity of 20 m/s using the earlier ingots as the starting materials. After ball milling, the powders with particle sizes of 2-4
21、 µm were heated to 953 K in He with a heating rate of 40 K/min for 10 m</p><p> 3. Results and discussion</p><p> 3.1. Structure characteristics</p><p> Epoxy resin composit
22、es were prepared by homogeneously mixing the composite powders with 20 wt% epoxy resin and pressing into cylindrical shaped compacts. These compacts were cured by heating at 453 K for 30 min, and then cut into toroidal s
23、haped samples of 7.00 mm outer diameter and 3.04 mm inner diameter. The scattering parameters (S11, S21) of the toroidal shaped sample were measured using a Hewlett-packard 8720B network analyzer. The relative permeabili
24、ty (μr) and permittivity (εr) values wer</p><p><b> (2)</b></p><p><b> (3)</b></p><p> where f is the frequency of the electromagnetic wave, d is the thic
25、kness of an absorber, c is the velocity of light, Z0 is the impedance of air, and Zin is the input impedance of absorber.</p><p> FIG. 1. The XRD pattern of Y5Fe77.5B17.5 powders:(a)as obtained,(b)after ann
26、ealing at 953 K for 10 min in He gas, and(c)oxidation-disproportionating the sample(b)in O2 at 573 K for 2 h.</p><p> Figure 1 shows the typical x-ray diffraction patterns measured on the amorphous Y5Fe77.5
27、B17.5 powder: (a) as obtained,(b)after annealing at 953 K for 10 min in He, and(c)after oxidation-disproportionating sample (b)at 573 K for 2 h in O2 . From Fig. 1(a), it was found that the Y5Fe77.5B17.5 alloy powders pr
28、epared by using the melt-spun technique were amorphous. After annealing as shown in Fig. 1(b), the powders were composed of both the Fe3B and Y2Fe14B phases. After oxidation-disproportionation</p><p> 3.2.
29、Microwave properties</p><p> The frequency dependence on the relative permittivity for resin composites, including 80 wt% a-Fe/Fe3B/Y2O3 powders, is shown in Fig. 2(a). The real part and imaginary part of
30、 relative permittivity were almost constant over the 0.5–10 GHz range, and hence the relative permittivity () showed almost constant (=15,=0.6). This ?nding indicates high resistivity of the composites. The measured resi
31、stivity value was around 100 Ωm for the a-Fe/Fe3B/Y2O3 composites, but the electric resistivity of the </p><p> The real part and imaginary part of relative permeability are plotted as a function of frequ
32、ency in Fig. 2(b). The real part of relative permeability declined from 1.6 to 0.9 with frequency. However, the imaginary part of relative permeability increased from 0.1 to 0.6 over a range of 1-7.1 GHz, and then decr
33、eased in the higher frequency range. The imaginary part of relative permeability exhibited a peak in a broad frequency range(2-9 GHz). Compared with a-Fe/Y2O3 , the a-Fe/Fe3B/Y2O3 compos</p><p> FIG. 2. Fre
34、quency dependences of relative permittivityεr(a)and permeability µr (b) for the resin composites with 80 wt % of a-Fe/Y2O3 and a-Fe/Fe3B/Y2O3 powders.</p><p> 3.3. Absorption performance</p><
35、;p> Figure 3(a) shows a typical relationship between RL and frequency for the resin composites with 80 wt% a-Fe/Fe3B/Y2O3 powders. First, the minimum re?ection loss was found to move toward the lower frequency region
36、 with increasing the thickness. Second, the RL values of resin composites less than -20 dB were obtained in the 2.7-6.5 GHz frequency range, with thickness of 6-3 mm, respectively. In particular, a minimum RL value of -3
37、3 dB was observed at 4.5 GHz on a specimen with a matching thickness</p><p> It is well known that one criterion for selecting a suitable electromagnetic absorption material is the location of its natural r
38、esonance frequency (fr). The natural resonance frequency is related to the anisotropic ?eld (HA) value by the following equation:</p><p><b> (4)</b></p><p> where is the gyrometric
39、 ratio and HA is the anisotropic ?eld. Many workers have reported that the large HA values of the M-type ferrites used as electromagnetic wave absorption materials result in a remarkable shift to high frequency range in
40、fr[10–12]. Therefore, one can expect that the frequency of microwave absorption for the metallic magnets can be controlled by changing the fr value of materials. Figure 3(b) shows the frequency dependence of RL, for resi
41、n composites with 80 wt% a-Fe/Y2O3 po</p><p> FIG. 3. Frequency dependences of RL for the resin composites with 80 wt % of(a)a-Fe/Fe3B/Y2O3 and (b)a-Fe/Y2O3 powders.</p><p> 4. Conclusions<
42、/p><p> In conclusion, the nanocomposites a-Fe/Fe3B/Y2O3 powders have been uniformly prepared by a melt-spun technique and the subsequent annealing and oxidation-disproportionation treatments. The excellent el
43、ectromagnetic wave absorption properties are due to the low relative permittivity and high relative permeability value during 2.7-6.5 GHz range. Our study of a-Fe/Fe3B/Y2O3 demonstrates the possible application of three-
44、phase type composites as electromagnetic wave absorbers.</p><p> This work was supported by Grant-in-Aid for Scienti?c Research No. 15205025 from the Ministry of Education, Science, Sports, and Culture of J
45、apan.</p><p> References</p><p> [1] S. Yoshida, J. Magn. Soc. Jpn. 22, 1353(1998).</p><p> [2] S. Yoshida, M. Sato, E. Sugawara, and Y. Shimada, J. Appl. Phys. 85,4636 ~1999.<
46、;/p><p> [3] J. L. Snoek, Physica ~Amsterdam! 14, 207(1948).</p><p> [4] T. Maeda, S. Sugimoto, T. Kagotani, D. Book, M. Homma, H. Ota, and Y. Houjou, Mater. Trans., JIM 41, 1172(2000).</p>
47、<p> [5] S. Sugimoto, T. Maeda, D. Book, T. Kagotani, K. Inomata, M. Homma, H.Ota, Y. Houjou, and R. Sato, J. Alloys Compd. 330, 301(2002).</p><p> [6] J. R. Liu, M. Itoh, and K. Machida, Chem. Lett
48、. 32,394(2003).</p><p> [7] Y. Q. Wu, D. H. Ping, B. S. Murty, H. Kanekiyo, S. Hirosawa, and K.Hona, Scr. Mater. 45, 355(2001).</p><p> [8] S. Hirosawa, H. Kanekiyo, Y. Shigemoto, K. Maurakami
49、, T. Miyoshi, and Y. Shioya, J. Magn. Magn. Mater. 239, 424(2002).</p><p> [9] M. Sagawa, S. Fujimura, N. Togawa, H. Yamamoto, and Y. Matuura, J.Appl. Phys. 55, 2083(1984).</p><p> [10] M. Mat
50、sumoto and Y. Miyata, J. Appl. Phys. 8, 5486(1996).</p><p> [11] S. Sugimoto, K. Okayama, S. Kondo, H. Ota, M. Kimura, Y. Yoshida, H.Nakamura, D. Book, T. Kagotani, and M. Homma, Mater. Trans., JIM 10,1080(
51、1998).</p><p> [12] S. B. Cho, D. H. Kang, and J. H. Oh, J. Mater. Sci. 31, 4719(1996).</p><p> [13] W. Coene, F. Hakkens, R. Coehoorn, D. B. de Mooij, C. de Waard, J.Fidler, and R. Grossinger
溫馨提示
- 1. 本站所有資源如無特殊說明,都需要本地電腦安裝OFFICE2007和PDF閱讀器。圖紙軟件為CAD,CAXA,PROE,UG,SolidWorks等.壓縮文件請下載最新的WinRAR軟件解壓。
- 2. 本站的文檔不包含任何第三方提供的附件圖紙等,如果需要附件,請聯(lián)系上傳者。文件的所有權(quán)益歸上傳用戶所有。
- 3. 本站RAR壓縮包中若帶圖紙,網(wǎng)頁內(nèi)容里面會有圖紙預(yù)覽,若沒有圖紙預(yù)覽就沒有圖紙。
- 4. 未經(jīng)權(quán)益所有人同意不得將文件中的內(nèi)容挪作商業(yè)或盈利用途。
- 5. 眾賞文庫僅提供信息存儲空間,僅對用戶上傳內(nèi)容的表現(xiàn)方式做保護(hù)處理,對用戶上傳分享的文檔內(nèi)容本身不做任何修改或編輯,并不能對任何下載內(nèi)容負(fù)責(zé)。
- 6. 下載文件中如有侵權(quán)或不適當(dāng)內(nèi)容,請與我們聯(lián)系,我們立即糾正。
- 7. 本站不保證下載資源的準(zhǔn)確性、安全性和完整性, 同時也不承擔(dān)用戶因使用這些下載資源對自己和他人造成任何形式的傷害或損失。
最新文檔
- 納米復(fù)合材料外文翻譯--鋇鐵氧體納米復(fù)合材料的電磁微波
- 納米復(fù)合材料外文翻譯
- 碳納米管復(fù)合材料微波吸收性能的模擬計算及其優(yōu)化.pdf
- 納米鐵氧化物-石墨復(fù)合材料的制備及其微波吸收性能研究.pdf
- 氧化鈰-石墨烯(聚苯胺)納米復(fù)合材料的制備及微波吸收性能研究.pdf
- 納米復(fù)合材料
- 多壁碳納米管-雙馬來酰亞胺復(fù)合材料微波吸收性能的研究.pdf
- TiN-TiO2納米復(fù)合材料制備及光吸收性能.pdf
- 金屬基納米粉體-聚合物復(fù)合材料的制備及微波吸收性能研究.pdf
- 納米磁性復(fù)合材料和納米有序復(fù)合材料的制備及性能研究.pdf
- 納米陶瓷復(fù)合材料
- 聚苯胺-鈷鉻鋅鐵氧體復(fù)合材料的微波吸收性能和磁性能
- 硫化鈷基復(fù)合納米材料的制備及微波吸收性能研究.pdf
- FeCo-石墨復(fù)合材料的制備及微波吸收性能調(diào)控研究.pdf
- 粘土-橡膠納米復(fù)合材料的界面設(shè)計及高性能納米復(fù)合材料的制備.pdf
- 鎳鋅鐵氧體納米復(fù)合材料的制備、磁性能與微波吸收特性.pdf
- pet/clay納米復(fù)合材料
- 氧化鋅—鋇鐵氧體復(fù)合材料制備及其微波吸收性能的研究.pdf
- 石墨烯三維復(fù)合材料的制備及其微波吸收性能研究.pdf
- SiC納米復(fù)合材料微波損耗模型及性能預(yù)測.pdf
聯(lián)系客服
本站為文檔C2C交易模式,即用戶上傳的文檔直接被用戶下載,本站只是中間服務(wù)平臺,本站所有文檔下載所得的收益歸上傳人(含作者)所有。眾賞文庫僅提供信息存儲空間,僅對用戶上傳內(nèi)容的表現(xiàn)方式做保護(hù)處理,對上載內(nèi)容本身不做任何修改或編輯。若文檔所含內(nèi)容侵犯了您的版權(quán)或隱私,請立即通知眾賞文庫,我們立即給予刪除!
- 備案號: 經(jīng)營許可證編號:浙ICP備20018660號
-
Copyright ? 2013-2023 眾賞文庫版權(quán)所有 違法與不良信息舉報電話:15067167862
評論
0/150
提交評論