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1.
采用氧化物陶瓷工艺制备2~4MHz高频开关电源用Mn Zn功率铁氧体,通过对铁氧体断面显微结构、密度和磁性能的测试,研究了TiO_2掺杂量对材料微观结构、磁导率和功率损耗的影响。结果表明,随着TiO_2掺杂量的增加,样品平均晶粒尺寸先减小后增大,磁导率单调减小,不同温度(25℃、100℃)下的磁心总功率损耗(激励条件3MHz,10m T、25m T)先减小后增大。说明TiO_2的适量掺杂可以改善高频Mn Zn功率铁氧体的微观结构,降低其功耗。  相似文献   

2.
为研究微波铁氧体器件,需要获知磁化后铁氧体的电磁性能参数。以具有高磁晶各向异性场的六角晶型铁氧体为材料,在22-40GHz的频率范围内对磁化后材料的共极化和交叉极化透射系数进行了测试,然后采用数值仿真透射系数与实验测试结果拟合的方法,得到了磁化六角晶型铁氧体的各向异性场H0为1095kA/m,共振线宽AH为7.5kA/m,饱和磁化强度Ms为160kA/m和在Ka频段时的介电常数ε约为22.1。结果表明六角晶系铁氧体具有高磁晶各向异性场,借助这些已获知的电磁参数,就可以使用此种材料进行微波铁氧体器件的研究与设计。  相似文献   

3.
以永磁锶铁氧体预烧料(Sr Fe12O19)为原料,添加SiO_2、CaCO_3、H_3BO_3、Al_2O_3、Cr_2O_3以及葡萄糖酸钙,利用陶瓷法在烧结温度为1210℃、保温时间为2 h的条件下制备锶铁氧体。利用X射线衍射、扫描电镜、激光粒度分析仪以及磁性能测量仪表征和测量物相组成与结构、微观形貌、粒度以及磁性能等。结果表明,二次复合添加后样品的矫顽力较未进行二次复合添加的样品有很大提高,性能可达到Br=412.7 mT,Hcj=336.7k A/m,(BH)max=32.15 kJ/m~3。最后探究了料水比对磁性能的影响。  相似文献   

4.
采用固相反应法制备Sr_(1-x)La_x Fe_(11.8-x) Zn_x O_(19)(0≤x≤0.42)M型六角铁氧体磁粉和磁体。X射线衍射(XRD)分析表明,La-Zn取代量x在0~0.42范围内磁粉是单一的磁铅石型相。磁体的FESEM观察表明,不同La-Zn取代量的磁体形成了均匀的六角片状结构。随La-Zn取代量的增大,磁体的剩磁B_r和最大磁能积(BH)_(max)先增后降,最大值对应的取代量为0.3,而其内禀矫顽力H_(cj)和磁感应矫顽力H_(cb)则单调下降。  相似文献   

5.
采用传统氧化物陶瓷工艺制备Mn_(0.777)Zn_(0.133)Fe_(2.09)O_4铁氧体材料,研究了预烧温度对材料微结构和磁性能的影响。结果表明,随着预烧温度的升高,材料的密度(d)、起始磁导率(μi)和饱和磁感应强度(Bs)均先升高后降低,材料的损耗(Pcv)先降低后升高。当预烧温度为910℃时,材料具有最大的烧结密度、饱和磁感应强度、起始磁导率以及最小的磁芯损耗。  相似文献   

6.
7.
采用陶瓷工艺制备高频MnZn功率铁氧体材料,研究了MoO3添加对材料微结构和磁性能的影响。用X射线衍射仪(XRD)、扫描电子显微镜(SEM)表征材料结构,用B-H分析仪测试材料磁性能,并对材料功率损耗进行分离。结果表明,适量添加MoO3可以有效改善材料的微观结构,提高致密度,提高材料饱和磁通密度和起始磁导率,降低功率损耗。功耗分离后发现,随着MoO3添加量的增加,磁滞损耗比例下降,涡流损耗所占比例上升。最佳MoO3添加量为0.01 wt%,获得低功耗的MnZn功率铁氧体,100℃、500kHz、50mT条件下功耗为86 kW/m3,起始磁导率约为1928,25℃下的饱和磁通密度为513 mT。  相似文献   

8.
ABSTRACT

In the present ferrites (soft & hard) series, Saturation Magnetization, increases only at lowers concentration of Indium. The cation distribution from Mössbauer analysis indicates that Indium ion at lower concentration (10 to 20%) goes to tetrahedral site only, whereas higher concentration it goes octahedral sites also. Magnetization has been explained on the basis of super exchange hyperfine interactions as well as cation distribution of magnetic ions as per the Neel's two sub lattice model of ferromagnetism. In all the chosen ferrite series magnetic behavior is consistent with substitution of dopant (In3+ ions). Ferromagnetic results are further authenticated by Mössbauer Spectroscopic analysis.  相似文献   

9.
以Fe_2O_3、MnO、ZnO粉体为原料,采用固相烧结法,通过一次球磨,850℃预烧并掺杂,二次球磨,1200℃烧结最后压制成型制得不同MoO_3掺杂量的锰锌铁氧体,运用SEM、XRD、VSM等手段研究该材料的组织与性能。结果表明,无论是否掺杂MoO_3,均生成了典型的尖晶石铁氧体相和Fe_2O_3相。材料的饱和磁化强度和磁导率随掺杂量增加先增大后减小,矫顽力和剩余磁化强度先减小后增大。表现为掺杂0.06wt% MoO_3的锰锌铁氧块体组织最为致密,磁性能达到最优,矫顽力及剩余磁化强度最小,磁导率和饱和磁化强度最大。  相似文献   

10.
The electronic structure, elastic constants, and magnetic properties of lanthanum cobaltite oxide \(\hbox {La}_{4}\hbox {Co}_{3}\hbox {O}_{9}\) compound, which crystallizes in orthorhombic space group Pnma, are investigated theoretically for the first time using the full potential linearized augmented plane wave (FP-LAPW) method based on the density functional theory plus Hubbard correction term (DFT \(+\) U). The calculated equilibrium lattice constants and fractional atomic coordinates are in a good agreement with available experimental data. Our result for the formation energy and elastic constants confirms that the predicted \(\hbox {La}_{4}\hbox {Co}_{3}\hbox {O}_{9}\) is mechanically stable. This compound is found to be ductile in nature in accordance with Pugh’s criteria. The anisotropy factors (\({A}_{1})\), (\({A}_{2})\), and (\({A}_{3})\) of \(\hbox {La}_{4}\hbox {Co}_{3}\hbox {O}_{9}\) material are also predicted through the elastic constants. The electronic band structures show metallic behavior; the conductivity is mostly governed by Co-3d and O-2p states. The total magnetic moments of the tetrahedral (\(\hbox {CoO}_{4})\) and octahedral (\(\hbox {CoO}_{6})\) environments are, respectively, 2.502 \(\mu _{B}\) and 2.874 \(\mu _{B}\), which are consistent with the experimental measurements.  相似文献   

11.
NiZn铁氧体是一种十分重要的磁性功能材料,在电子信息产业中有着广泛应用,而添加剂是改善NiZn铁氧体材料性能的重要措施.归纳了不同添加剂在NiZn铁氧体材料中的作用,同时分析了一些典型的添加剂WO3、MoO3、Bi2O3、V2O5、SnO2、SiO2、MnO2、CoO和Al2O3对NiZn铁氧体材料性能的影响及其作用...  相似文献   

12.
The measurement of the iron loss in ferrites is important for developing high‐efficiency switching power supplies. The authors have proposed the dynamic magnetic loss parameter, λf, for evaluating the iron loss in ferrites. In previous studies, the parameter was assumed to be a constant value for an individual ferrite material and defined for one period of a small BH loop. In this paper, assuming that λf is a function of the time derivative of the magnetic flux density, dB/dt, a novel measurement method of λf of a Ni‐Zn ferrite is proposed using rectangular wave voltage excitation and the Fourier expansion of the exciting current. In order to realize an iron loss measurement system with the rectangular wave voltage excitation, a high‐frequency FET inverter has been developed. The results of measuring λf show that it is uniquely determined by dB/dt regardless of the BH loop size. The measured dB/dt characteristics of λf are applied to practical examples for switching power supplies and sinusoidal wave voltage excitations. Their experimental and computational results coincide and it is clarified that the measured dB/dt characteristics are effective and useful. © 2006 Wiley Periodicals, Inc. Electr Eng Jpn, 156(1): 1–6, 2006; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/eej.20101  相似文献   

13.
采用固相反应法制备了Mg_(1-x)Cu_xFe_2O_4(x=0,0.4,0.6和0.8)系多晶铁氧体,分别采用X射线衍射(XRD)、扫描电镜(SEM)和振动样品磁强计(VSM)对样品的结构和静态磁性能进行了表征,并测试了磁环在10k Hz~1MHz范围的磁导率、品质因数以及功率损耗。结果表明,Cu含量x=0~0.6时,样品均为单相立方尖晶石结构,Cu含量进一步增加至x=0.8时呈现大量的四方相另相;晶粒尺寸和密度均随x值增加逐渐增大,而电阻率则呈减小趋势;饱和磁化强度由20.7 A m2/kg逐渐增大到30.4 A m2/kg,矫顽力先减小后增大,在x=0.6时具有最小值445.7 A/m。利用适量的Cu2+取代Mg2+可以提高Mg1-xCuxFe2O4铁氧体的磁导率并降低其品质因数,样品的功耗相应地明显增大;在交变磁场频率为370k Hz时,磁通密度低于20 m T范围内,Mg_(0.4)Cu_(0.6)Fe_2O_4具有相对较高的功耗。  相似文献   

14.
15.
用传统氧化物法制备了组分为Y2.3Ca0.7Zr0.3V0.2Fe4.5-δO1(20≤δ≤0.1)的石榴石型铁氧体(YCaZrVIG)。用XRD、SEM对样品进行物相和微结构表征。研究了缺铁量对YCaZrVIG铁氧体物相组成、烧结性能、微观结构及电磁性能的影响。结果表明,小量缺铁不会改变物相组成,但会造成样品更难烧结;随缺铁量的增大,介电常数基本不变,介电损耗明显降低后保持稳定,剩磁逐渐减小,矫顽力则是先减小再增大。当缺铁量δ=0.05时,可获得低损耗、低矫顽力的铁氧体。  相似文献   

16.
Polycrystalline Ni-Zn ferrites with a well-defined composition of Ni0.4Zn0.6Fe2-xSbxO4 synthesized using sol–gel method. Morphological characterizations on the prepared samples were performed by high resolution transmission electron and field emission scanning electron microscopy. The powders were densified using microwave sintering method. The room temperature complex permittivity (ε′ and ε″) and permeability (μ′ and μ″) were measured over a wide frequency range from 1 MHz–1.8 GHz. The real part of permittivity varies as ‘x’ concentration increases and the resonance frequency was observed at much higher frequencies and there is a significant decrease in the loss factor (tanδ). The electrical resistivity and permeability of NiZn ferrites increased with an increase of Sb content. As the concentration of ‘x’ increases from 0 to 0.08 the saturation magnetisation decreases. The saturation magnetization (Ms)?≈?52.211 A.m2/Kg for x?=?0 at room temperature. The room temperature electro paramagnetic resonance (EPR) were studied.  相似文献   

17.
用固相法两段连续升温法合成了LiCoxMn2-xO4,研究了钴掺杂对锂锰氧化物性能的影响,分析了样品中的Mn3 和Mn4 的含量.XRD测试表明:Co3 取代了六配位的Mn3 ,晶胞体积收缩,结构更加稳定.通过恒流法和循环伏安法测定了材料的电化学性能.结果表明:钴掺杂使Li 嵌脱一步进行.  相似文献   

18.
钴的添加方式对镍电极析氧特性的影响   总被引:9,自引:1,他引:8  
首先制备出添加剂Co2+以不同方式添加的5种氢氧化镍,然后分别做成电极。通过循环伏安法考察电极充放电过程中氧气析出的难易程度、通过排水取气法考察各电极充电过程中氧气析出的时间、速度及不同时刻的充电效率。将这两种方法相结合研究了钴的添加方式对镍电极析氧特性的影响。结果表明:Co2+固溶体掺杂和表面掺杂均可强化镍电极充电过程中的析氧极化、提高充电效率、改善电极性能,但当两种方式按适当的比例相结合时强化析氧极化的效果会更好。在本文所讨论的几种掺杂方式中,Co2+以表面掺杂1.5%+固溶体掺杂1.5%混合方式添加是降低镍电极的氧化电位、提高析氧电位、提高电极充电接受能力、改善电极充放电性能最好的添加方式  相似文献   

19.
杜荣斌  刘峥 《电源技术》2006,30(9):736-739
利用流变相反应法合成了两种化合物LixMn2O4(0.90≤x≤1.2)和LiMn2-xCoxO4(0.05≤x≤0.5),探讨了不同锂含量对尖晶石材料结构和性能的影响,并对掺钴材料LiMn2-xCoxO4的结构和电化学性能作了初步研究。不同Li/2Mn对合成的尖晶石LiMn2O4的结构有很大的影响,对于纯的尖晶石LiMn2O4化合物,其Li/2Mn值应控制在0.95 ̄1.15之间。Co3 离子掺入到LiMn2O4能稳定尖晶石的骨架结构,并且极大地改善了LiMn2O4在充放电过程中的循环稳定性能。  相似文献   

20.
采用传统氧化物法制备了MnZn功率铁氧体,研究了CoO掺杂对MnZn功率铁氧体微观结构和磁性能的影响.结果表明,CoO掺杂导致密度增大,功耗降低,并改善其起始磁导率μi的温度特性.当CoO含量为0.3wt%时,试样晶粒尺寸大小均匀,结构致密,具有良好的综合性能:密度D=4.91g/cm3,起始磁导率μi=2768,饱和磁通密度Bs=519mT,剩磁Br=69mT,矫顽力Hc=9.2A/m,功率损耗Pcv<440kW/m3(15 ~ 120℃),起始磁导率的温度因数αF=4.8×10-7/℃(20~80℃).  相似文献   

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