巨磁阻抗效应实验研究

利用物理实验室中常见的设备,搭建了一组巨磁阻抗效应实验装置,测量了在不同轴向外磁场及不同频率下钴基非晶态软磁合金细丝的阻抗.阻抗实部虚部均随外磁场增大迅速减小,而随频率增大缓慢增大.与交流阻抗的电磁理论比较,该实验结果与理论一致.实验观察到在40 MHz的频率、10 mT外磁场中阻抗变化达80%.根据数据和理论公式拟合,发现材料复磁导率随磁场强度增大迅速减小.     

用于HIRFL-CSRm纵向压缩高频腔的磁合金环测试

在HIRFL-CSRm上进行高能量密度物理和等离子体物理的研究需要一个能提供高电压的高频腔来对束团进行纵向压缩, 而磁合金加载腔获得较高的加速场梯度可以满足这一要求, 且腔体不需要调谐, 从而简化了高频控制系统。为了选择磁导率和阻抗较大、Q值(品质因数)小于1的磁合金材料来加载压缩高频腔, 对型号为V和A的两种磁合金材料进行了测试。测试结果表明: 型号为V的材料具有较大的磁导率、 阻抗和小于1的Q值, 将被用来加载腔体以获得足够高的加速电场梯度。A high voltage RF cavity is required to compress the beam bunch in the longitudinal for high energy density physics and plasma physics research at HIRFL CSRm. A magnetic alloy (MA) loaded cavity which has high acceleration gradient and without tuning loop (can simplify the RF control system), can meet the requirement. In order to select a proper MA material with higher permeability and shunt impe dance, Q< 1 value to load the RF compression cavity, two different MA materials V and A have been tes ted. The results indicate that the material V will be better for the construction of the RF cavity than material A because of its higher permeability and shunt impedance, Q< 1 value.     

RL-C并联电路阻抗最大值的讨论

讨论了RL-C并联电路阻抗值随电感、电容,以及电源频率变化的关系,给出了3种情况下最大阻抗值和谐振时的阻抗值,论证了调节电源频率或电感达到谐振时,其阻抗模并非最大值.     

非晶和纳米晶软磁丝状样品的环向磁化过程

采用阻抗法测定了不同磁结构的软磁丝状样品(非晶及纳米晶合金)的环向磁导率随环向磁场 强度和频率的变化. 按照Chen等的理论公式计算了样品的环向磁化曲线，结果发现，这一实 验原理公式对具有较大损耗的磁化过程并不适用. 因此，将其发展给出了更一般情况下的理 论公式. 此外，通过分析复数磁导率对环向磁场的依赖关系，确定了两类不同畴结构样品的 不同的环向矫顽力机理. 研究了交流频率对磁化过程的影响. 关键词： 非晶和纳米晶软磁丝 阻抗 环向磁化曲线     

一维负磁导率材料中的缺陷效应

理论和实验已经表明，金属开口谐振环（split ring resonators,简称SRR）可以实现材料的有效磁导率μeff在某一频率范围内为负.采用波导法实验研究了不同几何尺寸的六边形SRR在X波段微波作用下的近邻相互作用.实验发现，相同尺寸的六边形SRR周期性排列而成的一维负磁导率材料存在一个谐振频率；当缺陷谐振环引入一维负磁导率材料时，主谐振频率和缺陷环谐振频率同时发生移动；主谐振频率和缺陷环谐振频率的移动量随缺陷与双环谐振频率之差的增加而减小，当缺陷环谐振频率与双环谐振频率接近时，环间的相互作用增强，频率的移动量增大. 关键词： 负磁导率 缺陷效应 开口谐振环     

CSNS铁氧体环性能初步测试

用于中国散裂中子源CSNS的环射频铁氧体同轴谐振腔, 工作频率在1.02MHz至2.42MHz. 论文对决定腔性能的铁氧体环材料进行了性能测试研究. 通过改变铁氧体环的偏置磁场来改变铁氧体的磁导率, 使腔的等效电感发生变化, 从而使得LC并联谐振回路的谐振频率改变, 进而获得铁氧体环在不同频率, 不同高频磁场强度下的μ_rQf、品质因数和功率密度值. 本文比较了几种不同铁氧体环的测量结果, 选择适合于CSNS的环射频铁氧体谐振腔的材料为4M2.     

对九脚探头磁导率、检测电压与应力相关性研究

为了研究九脚探头的磁导率、检测电压与应力之间的关系,基于法拉第电磁感应定律和磁路定律,推导了九脚探头的磁导率同检测电压的关系.利用该探头测试了Q235,Q255,Q345钢试件在不同应力条件下,探头的检测电压同励磁电压、应力之间的变化曲线关系,实验结果表明:在相同的励磁电压下,测试应力在达到试件屈服点之前,检测电压同应力呈线性关系,在测试应力达到试件屈服点附近时,检测电压随应力增加而快速降低,呈非线性关系,从而证明了磁导率、检测电压、应力三者之间的关联性.     

CSNS铁氧体环性能初步测试

用于中国散裂中子源CSNS的环射频铁氧体同轴谐振腔,工作频率在1.02MHz至2.42MHz.论文对决定腔性能的铁氧体环材料进行了性能测试研究.通过改变铁氧体环的偏置磁场来改变铁氧体的磁导率,使腔的等效电感发生变化,从而使得LC并联谐振回路的谐振频率改变,进而获得铁氧体环在不同频率,不同高频磁场强度下的μrqf、品质因数和功率密度值.本文比较了几种不同铁氧体环的测量结果,选择适合于CSNS的环射频铁氧体谐振腔的材料为4M2.     

射频负离子源200kV高压平台磁缓冲器系统中磁芯的性能测试和分析

在射频负离子源200kV高压平台磁缓冲器系统设计中,首次通过旁路电阻的方式,解决了系统运行时次级直流偏置电路中电阻的过热问题。分析了磁缓冲器系统在高压电源启动阶段(工况1)和负离子源运行阶段电极间打火时(工况2)的主要工作频率。在工况1对应的工作频率下,测试了磁缓冲器核心部件铁基纳米晶软磁合金(FINEMET)磁芯的B-H曲线,得出加入直流偏置后的振幅磁导率与无直流偏置时相比,下降了60%(200Hz)～80%(100Hz)。在工况2对应的主要频率下,测试了磁芯的复数起始磁导率并进行了储能耗能分析。在25～525kHz频率范围内,测得了磁芯的磁谱以及品质因数随频率变化的曲线,得出随着频率的增加,磁芯单位耗能下的储能逐渐减小;当频率达到100kHz以上后,磁芯的能量存储与耗散状态趋于稳定。     

应用NiZn铁氧体的宽带传输线变压器性能分析

研究了变换比为4∶1的宽频带传输线变压器,给出了考虑线圈互耦的等效电路模型,分析了其阻抗变换特性。针对在以往传输线变压器分析中忽略频率变化对磁导率的影响这一问题,以应用NiZn铁氧体的宽带传输线变压器为例,将频率变化对磁导率的影响应用到分析传输线变压器特性中。对测试结果的分析和比较表明:在传输线变压器输入阻抗的分析中,频率对其的影响是存在的,在等效电路模型分析中加以考虑,可以更好地与实际值吻合。     

SSC新高频腔设计与分析

简要分析了HIRFL SFC与SSC之间的束流匹配关系, 给出了新高频腔的频率范围。 利用经典三维电磁场数值模拟软件MAFIA对SSC新高频腔体进行了模拟计算, 得出了SSC新高频腔体的相关物理参数, 并对频率范围、Q值、 并联阻抗和电压分布等参数进行了分析。 高频腔体的模拟计算结果完全符合SSC回旋加速器改造的物理设计及空间结构要求。     

双间隙输出腔开放腔的高频特性分析

 建立了S波段相对论速调管放大器双间隙输出腔开放腔的3维模型。采用时域有限差分法，通过监测激励电流源的响应计算了该双间隙输出腔的谐振频率、有载Q值、场分布以及特性阻抗，并分析了腔体结构尺寸对谐振频率、有载Q值和特性阻抗的影响。研究表明：腔体半径对开放腔的谐振频率影响很大，耦合孔尺寸对腔体谐振频率的影响较小；随着耦合孔张角增加，有载Q值逐渐减小；随着腔体半径增大、间隙的减小，腔体特性阻抗降低。研究结果可为S波段强流相对论速调管放大器双间隙输出腔的设计提供理论依据。     

快放电直线型变压器驱动源磁芯脉冲磁化特性

针对25 μm 2605TCA非晶涂层、25 μm 2605SA1非晶夹膜和50 μm DG6硅钢夹膜三种材料和工艺磁芯,对比研究了不同激磁条件下的磁化特性。结果表明:改变磁芯激磁条件,磁通密度变化量(ΔB)几乎不变,DG6硅钢夹膜磁芯和2605TCA非晶涂层磁芯ΔB均为3.1 T,2605SA1非晶夹膜磁芯ΔB仅为2.4 T;不同激磁条件下,相对磁导率变化较为明显,三种磁芯相对磁导率均随激磁特征参数的增加而迅速减小,当激磁特征参数由67 V/(cm2·ns)增加至129 V/(cm2·ns)时,2605SA1非晶夹膜磁芯最大相对磁导率由1800减小至1200,2605TCA非晶涂层磁芯最大相对磁导率由1100减小至400,相同激磁特征参数下2605TCA非晶涂层磁芯相对磁导率小于2605SA1非晶夹膜磁芯相对磁导率;DG6硅钢夹膜磁芯在快脉冲条件下磁化性能较差,最大相对磁导率仅为130。     

An untuned MA-loaded cavity for HIRFL-CSR

In order to realize high energy density physics and plasma physics research at HIRFL-CSR, a magnetic alloy (MA)-loaded cavity has been studied. According to the theoretical calculation and simulation for the MA-loaded cavity, we achieved a better result. The MA-loaded cavity had a higher μQf value, with a higher shunt impedance and a higher accelerating gradient. The accelerating gradient was about 95 kV/m at 1.8003 MHz, 130 kV/m at 0.9000 MHz. Compared with the ferrite-loaded cavities that are used at HIRFL-CSR, with about 10 kV/m accelerating gradient, the MA-loaded cavity obviously has an advantage. The results of the theoretical calculation and the simulation, which meet the design requirements are in good agreement.     

Permeability enhancement by induced displacement current in magnetic material with high permittivity

Based on a analytical model, this paper reveals that instead of demagnetization, the induced displacement current in a Mn–Zn ferrite core due to its high permittivity can produce a magnetic field that effectively adds to the incident magnetic field in the low-loss frequency region. This leads to a resultant magnetic field being larger than incident field in magnitude, and results in measured permeability being higher than its intrinsic value in the low-loss frequency region. It is also found that such effect is more pronounced in large core than in small core. With increasing frequency and consequently the core being more lossy, the induced magnetic field due to both conductivity and imaginary part of complex permittivity demagnetize the magnetic material and counteracts the incident magnetic field. In consequence, the measured real part of complex permeability becomes smaller than its intrinsic value. The larger the core dimension, the smaller the real part of complex permeability is. These conclusions based on the numerical analysis are in good agreement with the experimental observation in the aspect of change tendency of permeability versus frequency.     

磁场退火对Co基熔体抽拉丝巨磁阻抗效应的影响

对Co基熔体抽拉非晶丝进行了普通炉内退火和不同磁场强度（500 Oe,1600 Oe,4000 Oe）下的横向和纵向磁场退火,利用HP4192阻抗分析仪和Lakeshore7407VSM分析了退火态样品的巨磁阻抗（GMI）效应和软磁性能.研究结果表明,纵向磁场降低了环向各向异性,纵向磁场退火样品GMI效应降低且GMI曲线为单峰,最大阻抗变化率ΔZ/Z为131%,磁场响应灵敏度为7%/Oe;而横向磁场提高了环向畴体积,增加了环向各向异性场,导致退火样品GMI曲线随频率升高由单峰转 关键词： 非晶丝 巨磁阻抗效应 退火     

Finite element method calculations of GMI in thin films and sandwiched structures: Size and edge effects

The impedance values of magnetic thin films and magnetic/conductor/magnetic sandwiched structures with different widths are computed using the finite element method (FEM). The giant magneto-impedance (GMI) is calculated from the difference of the impedance values obtained with high and low permeability of the magnetic material. The results depend considerably on the width of the sample, demonstrating that edge effects are decisive for the GMI performance. It is shown that, besides the usual skin effect that is responsible for GMI, an “unexpected” increase of the current density takes place at the lateral edge of the sample. In magnetic thin films this effect is dominant when the permeability is low. In the trilayers, it is combined with the lack of shielding of the central conductor at the edge. The resulting effects on GMI are shown to be large for both kinds of samples. The conclusions of this study are of great importance for the successful design of miniaturized GMI devices.     

A novel multimode negative inductance negative resistance shunted electromagnetic damping and its application on a cantilever plate

Based on the characteristic of the electromagnetic damping, a novel multimode vibration control treatment, negative inductance negative resistance electromagnetic shunt damping (NINR-EMSD), is proposed and employed to control multimode vibration of a cantilever plate. The negative inductance of the shunt impedance can cancel the inherent inductance of the electromagnet, and the impedance of circuit consisted of the coils and shunt will be a pure resistance and the shunt current will be frequency independent when the inductance of the shunt and the electromagnet are equal with each other. The negative resistance cancels the resistance of electromagnet, and as a result the resistance and the current of the closed circuit will change, which make it feasible to control the multimode vibration of the system. Electromechanical coupling coefficient is obtained based on the equivalent current method. The governing equation of the plate with the electromagnetic shunt damping (EMSD) is established according to Hamilton's principle. Multimode vibration control of the system is simulated and experiments are carried out to verify the performance of the NINR-EMSD. The numerical predictions and experimental results agree well with each other and show that: the negative inductance negative resistance (NINR) of the shunt impedance can increase the damping of the structure notably; the decrease of the resistance of shunt impedance have a significant contribution to the improvement of vibration control performance; the first four modes vibration of the plate can be suppressed simultaneously with the NINR-EMSD.     

基于超材料吸波体的低雷达散射截面波导缝隙阵列天线

提出利用超材料吸波体减缩波导缝隙阵列天线带内雷达散射截面的设计方法. 设计具有超薄(厚度仅为0.01λ, λ为吸波体中心频率对应波长)、无表面损耗层和高吸波率的超材料吸波体, 将其加载到波导缝隙天线E面方向辐射缝隙间的金属表面上, 并与辐射缝隙保持一定的间距. 该加载方式没有破坏天线的口径馈电振幅分布, 并利用超材料吸波体对电磁波的强吸收特性降低了天线阵的结构模式项散射. 仿真和实验结果表明, 加载超材料吸波体后天线阵的反射系数、增益、波瓣宽度保持不变, 在x极化和y极化条件下, 波导缝隙阵列天线的带内雷达散射截面减缩量均在6 dB 以上, 且在-25°-+25°范围内天线雷达散射截面均有明显的减缩, 鼻锥方向减缩超过10 dB. 该研究成果对阵列天线雷达散射截面减缩具有重要的借鉴意义和工程应用价值.