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磁致伸缩材料对颗粒状 CZFO/NKNLS 复合材料磁电响应的结构效应

Structural Effects of Magnetostrictive Materials on the Magnetoelectric Response of Particulate CZFO/NKNLS Composites.

作者信息

Choi Moon Hyeok, Ko Kyujin, Yang Su Chul

机构信息

Department of Chemical Engineering, Dong-A University, Busan 49315, Korea.

出版信息

Materials (Basel). 2019 Mar 30;12(7):1053. doi: 10.3390/ma12071053.

DOI:10.3390/ma12071053
PMID:30935041
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6480309/
Abstract

In this study, magnetostrictive powders of CoFe₂O₄ (CFO) and Zn-substituted CoFe₂O₄ (CZFO, Zn = 0.1, 0.2) were synthesized in order to decrease the optimal dc magnetic field (), which is required to obtain a reliable magnetoelectric (ME) voltage in a 3-0 type particulate composite system. The CFO powders were prepared as a reference via a typical solid solution process. In particular, two types of heterogeneous CZFO powders were prepared via a stepwise solid solution process. Porous-CFO and dense-CFO powders were synthesized by calcination in a box furnace without and with pelletizing, respectively. Then, heterogeneous structures of pCZFO and dCZFO powders were prepared by Zn-substitution on calcined powders of porous-CFO and dense-CFO, respectively. Compared to the CFO powders, the heterogeneous pCZFO and dCZFO powders exhibited maximal magnetic susceptibilities () at lower values below ±50 Oe and ±10 Oe, respectively. The Zn substitution effect on the shift was more dominant in dCZFO than in pCZFO. This might be because the Zn ion could not diffuse into the dense-CFO powder, resulting in a more heterogeneous structure inducing an effective exchange-spring effect. As a result, ME composites consisting of 0.948NaKNbO₃⁻0.052LiSbO₃ (NKNLS) with CFO, pCZFO, and dCZFO were found to exhibit = 966 Oe (NKNLS-CFO), = 689⁻828 Oe (NKNLS-pCZFO), and = 458⁻481 Oe (NKNLS-dCZFO), respectively. The low values of below 500 Oe indicate that the structure of magnetostrictive materials should be considered in order to obtain a minimal for high feasibility of ME composites.

摘要

在本研究中,合成了CoFe₂O₄(CFO)和锌取代的CoFe₂O₄(CZFO,Zn = 0.1、0.2)磁致伸缩粉末,以降低在3-0型颗粒复合系统中获得可靠的磁电(ME)电压所需的最佳直流磁场()。通过典型的固溶工艺制备CFO粉末作为参考。特别地,通过逐步固溶工艺制备了两种类型的非均相CZFO粉末。多孔CFO粉末和致密CFO粉末分别通过在箱式炉中不造粒和造粒煅烧合成。然后,分别通过在多孔CFO和致密CFO的煅烧粉末上进行锌取代制备了pCZFO和dCZFO粉末的非均相结构。与CFO粉末相比,非均相pCZFO和dCZFO粉末分别在低于±50 Oe和±10 Oe的较低值下表现出最大磁化率()。锌取代对偏移的影响在dCZFO中比在pCZFO中更显著。这可能是因为锌离子无法扩散到致密CFO粉末中,导致更不均匀的结构诱导了有效的交换弹簧效应。结果发现,由0.948NaKNbO₃⁻0.052LiSbO₃(NKNLS)与CFO、pCZFO和dCZFO组成的ME复合材料分别表现出 = 966 Oe(NKNLS-CFO)、 = 689⁻828 Oe(NKNLS-pCZFO)和 = 458⁻481 Oe(NKNLS-dCZFO)。低于500 Oe的低值表明,为了使ME复合材料具有高可行性而获得最小的,应考虑磁致伸缩材料的结构。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/53e446ae4fc6/materials-12-01053-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/12fe074a9a20/materials-12-01053-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/51ae5b416163/materials-12-01053-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/3f2fe3aef472/materials-12-01053-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/efec5a269a18/materials-12-01053-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/53e446ae4fc6/materials-12-01053-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/12fe074a9a20/materials-12-01053-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/51ae5b416163/materials-12-01053-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/3f2fe3aef472/materials-12-01053-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/efec5a269a18/materials-12-01053-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ed7a/6480309/53e446ae4fc6/materials-12-01053-g005.jpg

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本文引用的文献

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