Co2+或Sn4+对MnZn功率铁氧体磁特性的影响研究

用普通陶瓷工艺制备了掺Co2+及Sn4+的MnZn功率铁氧体材料,研究了Co2+及Sn4+杂质掺入对MnZn功率铁氧体磁性能的影响.研究结果表明,由于Co2+具有大的正的磁晶各向异性常数K1,所以可与MnZn功率铁氧体负的K1进行补偿.当CoO掺入量为2×10-3时,可得到在20～120℃温度范围内具有非常平坦功率损耗-温度特性的MnZn功率铁氧体.Co2+的掺入还可以大大改善MnZn功率铁氧体的起始磁导率的温度特性.由于Sn4+掺入MnZn功率铁氧体时,Sn4+进入晶格中,减少了Fe3+Fe2+之间的电子跳跃,提高了材料电阻率.当SnO2掺入量为4×10-4时,可得到具有很低功率损耗的MnZn功率铁氧体材料.     

NiO-CoO复合掺杂对高B_s低损耗MnZn铁氧体性能影响

采用传统氧化物工艺制备了NiO-CoO掺杂的MnZn软磁铁氧体材料。研究了NiO、CoO复合掺杂对高Bs低损耗的MnZn铁氧体微结构及电磁性能的影响。结果表明,掺杂0.1%(质量分数)CoO和1.28%(质量分数)NiO的MnZn铁氧体晶粒生长均匀,具有较高的饱和磁感应强度,最低损耗点位于100℃。随着NiO掺杂量的增加,最低功耗点向高温方向移动。CoO掺杂导致材料密度增大,功耗降低。在钟罩炉中按特定烧结曲线烧结MnZn铁氧体具有较好的综合性能:μi=2 198,Pcv=319kW/m3,Bs=540mT(T=25℃),Bs=451mT(T=100℃)。     

Al替代和烧结温度对NiZn铁氧体磁性能的影响

采用陶瓷工艺制备了Al替代的Ni0.5Zn0.5AlxFe2-xO4(x=0~0.10)铁氧体材料,用XRD、B-H分析仪和阻抗分析仪对其结构和磁性能进行了研究。实验发现,最佳烧结温度为1 250℃,过高和过低的烧结温度不利于降低磁芯损耗。当Al3+替代量x=0.06时,铁氧体能获得较好综合磁性能。     

SnO2掺杂对MnZn铁氧体微观结构和性能的影响

采用氧化物陶瓷工艺制备MnZn功率铁氧体,研究了SnO2掺杂对MnZn功率铁氧体微观结构及磁性能的影响。结果表明添加适量的SnO2可以有效提高晶粒均匀性和致密度。随着SnO2添加量的增加,起始磁导率先上升后下降,磁损耗先下降后上升。当添加量为0.5%(摩尔分数)时,μi达到最大值,损耗最低。此外,铁氧体损耗最低点所对应的温度随着SnO2掺杂量的增加向低温移动。通过对比一次掺杂和二次掺杂,发现一次掺杂的SnO2主要作用于晶粒内部,二次掺杂的SnO2主要作用于晶界处,而且一次掺杂所获得的样品性能更优。     

等量La-Co掺杂对干压各向异性SrFe_(12)O_(19)结构和磁性能的影响

以Y30H-2预烧料作为基料,采用陶瓷法制备La-Co掺杂的干压各向异性Sr1-xLaxFe12-xCoxO19(x=0~0.10)锶铁氧体,研究La3+-Co2+共同替代对锶铁氧体结构和磁性能的影响。XRD射线衍射分析表明,La-Co掺杂并没有改变锶铁氧体结构,锶铁氧体主体仍为六角晶结构;SEM分析表明,La-Co掺杂能使晶粒粒度变细;磁性能测量显示,样品的Hcj随掺杂量的增加先增大后减小,当取代量x=0.06时,Hcj达到最大值。Br则随掺杂量的增加呈现不规则的变化。K值的变化表明,当x=0.04时,锶铁氧体的综合性能最佳。     

Co替代Y型六角铁氧体粉末在X波段的吸波特性

采用固相反应方法制备了Ba2Zn1.6-xCoxCu0.4Fe12O22(x=0,0.2,0.4,0.6)铁氧体粉末,将粉末在1050℃下退火4小时。利用X射线衍射(XRD)、振动样品磁强计(VSM)以及矢量网络分析仪研究了退火样品的晶体结构及其在8.2～12.5GHz波段的微波吸收特性。XRD分析表明样品为Y型六角铁氧体。VSM及微波矢量网络测量表明,掺Co样品的介电常数实部ε′的平均值由不掺时的6.5降为5.0。随着Co替代量的增加,样品的饱和磁化强度和剩磁不断增大;矫顽力先维持在62～70Oe之间,至Co含量x=0.6时迅速增为315.5Oe。在磁导率虚部μ″谱中观察到样品的自然共振吸收峰,其共振频率和峰值与样品中的Co含量有关,Co含量x=0.2的样品的μ″峰值达6.579,相应的反射功率损耗达41.796dB,吸波性能良好,基本达到在共振频率附近提高μ′、μ″和ε″值,同时降低ε′值的目的。     

掺杂对高磁导率低损耗锰锌铁氧体材料磁性能的影响

采用氧化物陶瓷工艺制备了高磁导率低损耗锰锌铁氧体材料,研究了Nb2O5掺杂对材料磁性能的影响。结果表明掺杂0.015%（质量分数）Nb2O5的锰锌铁氧体材料具有较好的磁性能：起始磁导率μi=13386,起始磁导率比温度系数αμ/μi=-0.6×10-6/K,相对损耗因数tanδ/μi=3.2×10-6。     

掺Gd^3＋、Sn^4＋的YIG微波铁氧体高功率特性

宽温度稳定性,大功率一直是微波铁氧体材料研究的重点.本文根据器件对材料的要求,采用陶瓷工艺.通过研究.Gd3 、Sn4 离子对YIG的c位Y3 、a位Fe3 离子的取代,得出在适当工艺条件下,当x=0.7、Y=O.3时,材料具有良好的温度稳定性,Ms=75×104T、ΔHk=1.1 kA/m.材料很好地满足了宽温度稳定性、高功率用x波段旋磁器件的要求.     

Ti取代对MnZn功率铁氧体微结构及磁性能的影响

采用氧化物陶瓷工艺制备了MnZn功率铁氧体,研究亮磁性能的影响,由于Ti4 是非磁性离子,它对磁性离子Mn2 的取代,必将对材料的微结构、磁性能以及居里温度产生影响.结果表明,Ti4 取代Mn2 可提高MnZn铁氧体居里温度,适量的Ti4 取代,有利于提高致密度和起始磁导率,并降低磁损耗.为了得到优良的电磁性能,适宜的Ti4 取代量为0.5mol%.     

Zn-Ti取代BaM型铁氧体材料结构与性能的研究

用固相反应合成的方法,制备出了不同比例的Zn-Ti取代BaM型六角晶系铁氧体材料,研究了温度和取代量对产物的相组成、微观形貌以及电磁性能的影响。结果表明,温度的提高有利于晶体的长大和发育完整,样品晶粒均呈六角形板片状,比较适合用于吸波用途。随着取代量的增加,BaZnTiM的复介电常数增大,介电损耗呈波动变化,磁损耗则呈下降趋势。     

Investigating the Characteristics of Cobalt-Substituted MnZn Ferrites by Equivalent Electrical Elements

We investigated the electrical and magnetic properties of cobalt-substituted manganese-zinc soft ferrite by using the equivalent lumped elements acquired from the appropriate equivalent electrical circuit of polycrystalline ferrite. We applied the equivalent lumped circuit, combined with equivalent lumped resistances and capacitance, to determine the effect of microstructure on electrical and magnetic properties of cobalt-substituted manganese-zinc ferrites. Both the hysteresis loss and the eddy-current loss of soft ferrites account for a major proportion of iron loss in high-frequency switching mode power supplies. Replacing a small portion of Fe²⁺ with Co²⁺ remarkably increases the bulk resistivity of the MnZn ferrite and decreases the core loss by lowering eddy-current loss. A longer isothermal duration causes grain growth and forms a larger equivalent capacitance, which leads to a reduction in hysteresis loss. However, excess substitution of Co²⁺ for Fe²⁺ is disadvantageous to magnetic permeability and raises core loss. We measured the dc resistivity by the four-probe method on sintered disks with both sides polished and coated with a thin layer of silver paste as a good contact material. We measured the magnetic permeability by an impedance analyzer at room temperature. The total loss of Mn_0.58Zn_0.37 Co_0.01Fe_2.04O₄ ferrite core does not exceed 420 mW/cm³ at 300 kHz/70 mT.     

Co替代对纳米晶Ni0.4CoxZn0.6-xFe2O4结构和电磁性能的影响

采用聚丙烯酰胺凝胶法制备了尖晶石型纳米晶Ni0.4CoxZn0.6-xFe2O4(x=0、0.2、0.4),同时考察了铁氧体的电磁性能.由X射线衍射(XRD)可知,随着x的增大,Ni0.4CoxZn0.6-xFe2O4的晶格常数从0.838 4 nm减小到0.835 7 nm.透射电镜(TEM)结果表明,Ni0.4Zn0.6Fe2O4铁氧体粒子的平均直径约为20 nm.Ni0.4CoxZn0.6-xFe2O4在8.2～12.4 GHz的测试频率范围内具有介电损耗和磁损耗.在频率为9.0 GHz时,Ni0.4CoxZn0.6-xFe2O4(x=0.4)复介电常数虚部的最大值达到19.6.随着X值的增加,复数磁导率虚部的共振吸收峰向高频移动.制备的复合物可以被广泛地用于抑制电磁辐射和吸收雷达波等领域.     

Effect of BiVO4 doping on the magnetic properties and microstructure of NiCuZn ferrites

Effects of BiVO₄ addition on the microstructural development and magnetic properties of a NiCuZn ferrite were investigated by conventional solid state reaction method. For the low temperature sintering (<961 °C), 0–2 wt% of BiVO₄ was added to the ferrites. The grain size and bulk density gradually increased with the increase in the BiVO₄ content and more uniform and compact structure at 1.0 wt% BiVO₄ were obtained. The permeability decreases gradually with increase in BiVO₄ content BiVO₄ doped in NiCuZn ferrites improved magnetic properties and reduced the magnetic loss tangent. The samples may be excellent candidates to fabricate multilayer chip inductors and LTCC passive devices.     

Effect of W ion doping on magnetic and dielectric properties of Ni-Zn ferrites by “one-step synthesis”

W-doped Ni-Zn ferrites with a nominal composition of Ni_0.5Zn_0.5W_xFe_2−xO₄ (where x = 0, 0.02, 0.04, 0.06, and 0.08) were prepared by one-step synthesis through the incorporation of WO₃ into the raw powders. The magnetic and dielectric properties of the as-prepared Ni-Zn ferrites were investigated. All samples have a typical spinel cubic structure. With increasing amount of W ions doped, the lattice constant decreases, while the grain size increases. The density and diameter shrinkage of the samples raise with small amount of W ions doped, but drop down with large amount of W ions doped. However, an uneven abnormal growth and closed pores were observed when too much of WO₃ was added. The saturation magnetization of the samples increases with small amount of W ions doped, but decreases with large amount of W ions doped, and the coercivity shows an opposite trend. The Curie temperature raises with increasing amount of W ions doped. Both the real and imaginary parts of permeability of the ferrites decrease with increasing amount of W ions doped, while the natural resonance changes very little. Both the dielectric constant and dielectric loss present a decrease with small amount of W ions doped, but increase with large amount of W ions doped.     

Thermoelectric power studies of Sn/Nb substituted Mn-Zn ferrites

Thermoelectric power studies of polycrystalline materials of Sn/Nb substituted Mn-Zn ferrites have been carried out. The Seebeck coefficient, carrier concentration and drift mobility were evaluated. The Seebeck coefficient increases up to 420 K and 400 K for Nb and Sn substituted ferrites respectively. All the ferrites exhibited n-type conduction over the range of temperature studied. At high temperatures, a non-degenerate type of semiconductor behaviour has been observed. The conduction of these materials is explained by hopping of electrons from Fe2+ to Fe3+, in addition to the existence of narrow bands and localized levels. The variation of drift mobility is explained by wavy bands [1, 2].     

Effect of dopants on the magnetic properties of MnZn ferrites forhigh frequency power supplies

The effect of additions on the magnetic properties of MnZn ferrites for high frequency power supplies was studied. The investigation revealed that various combinations of dopants added to the ferrite modify the grain boundary resistivity and the magnetic permeability spectra at constant microstructure. Particularly, the combined effect of Sn⁴⁺, Ti⁴⁺ and Ta⁵⁺ was found to increase the grain boundary resistivity in the ferrites studied and remarkably decrease the power loss at higher frequencies     

Microstructure studies on Ti4+- and Zr4+-substituted Li-Zn ferrites

XRD and microstructure studies were carried out on Ti⁴⁺ and Zr⁴⁺-substituted Li-Zn ferrites prepared by standard ceramic technique. All the ferrite compositions exhibit single phase formation. The lattice parametera increases linearly with the content of Zn²⁺Zr⁴⁺ and Zn²⁺Ti⁴⁺, which is attributed to the ionic volumes of the cations involved. With substitution by Zr⁴⁺ the average size decreases, while with substitution by Ti⁴⁺ the grain size increases. In both the series grain size varies with the composition. Excess substitution of Zr⁴⁺ (x>0·4) leads to the formation of secondary images and discontinuous grain growth. Both Zr⁴⁺ and Ti⁴⁺ compositions obey Kurtz theory.     

Structural and dielectric properties of nanocrystalline Nd<Superscript>3+</Superscript> substituted nickel–zinc ferrites

Ferrite samples with general formula Ni_1−xZn_xNd_yFe_2−yO₄ (x = 0, 0.2, 0.4, 0.6, 0.8 and 1; y = 0.01, 0.02 and 0.03) were synthesized by oxalate co-precipitation technique. The X-ray diffraction study confirms the formation of single-phase cubic spinel structure. The lattice constant of the samples increases with increase in zinc content and obeys Vegard’s law. On Nd³⁺ substitution lattice constant of the samples slightly increases except zinc ferrite. The frequency dependence of the dielectric constant, dielectric loss and AC conductivity of the samples were determined in the frequency range from 20 Hz to 1 MHz at room temperature. The experimental results reveal that the dielectric constant and dielectric loss decreases where as AC electrical conductivity increases with increase in frequency. The dielectric loss increases with increase in zinc content whereas it decreases with increase in Nd³⁺ content. There is no appreciable change in permittivity of the samples with increase in Nd³⁺ content. Permeability of all the samples increases with increase in Nd³⁺ content. Because of lower dielectric loss, Nd³⁺ substituted Ni–Zn ferrites are useful in electronic devices.     

自蔓延高温合成La-Zn掺杂锶铁氧体改性研究

采用高温自蔓延(SHS)方法制备了化学组成为Sr1-xLaxFe12-xZnxO19(x=0～0.4)的La-Zn联合掺杂的锶铁氧体,并研究了晶体结构与离子掺杂量对铁氧体磁性能的影响.根据相关的热力学数据,分析了合成过程中产生不同氧化物杂质的热力学机制,结果显示,通过合适控制反应体系中的Fe粉含量,可以合成单一的M型铁氧体相.SEM表明SHS方法制备的样品比传统方法制备的样品结晶更完整,粉体颗粒呈明显的六角平板状,颗粒尺寸基本分布在0.5～1.2 μm之间.La3 ,Zn2 的加入能够明显地提高试样的综合磁性能,相比于未掺杂的试样,在未取向情况下其剩磁提高了14.4%,Hcb提高了15.3%,(BH)m提高了30.7%,并且与传统制备方法相比,采用SHS方法获得的样品的内禀矫顽力Hcj提高尤为明显,最高可达322kA/m.