五自由度磁悬浮电主轴结构与有限元分析

提出一种五自由度稳定悬浮的电主轴,由二自由度磁悬浮异步电机与三自由度轴向混合磁轴承实现五个自由度的稳定悬浮。其中,三自由度混合磁轴承采用四个定子磁极来控制轴向悬浮力与径向扭转力,可有效减少轴向长度。文中介绍了五自由度磁悬浮电主轴工作原理,建立磁悬浮异步电机和混合磁轴承的数学模型,并用电磁场分析软件welll5．0分析其磁场和悬浮力,验证电主轴的可行性,最后运用biatlab软件建立基于转子磁场定向的无轴承异步电机控制系统,仿真结果表明该控制方法可有效稳定控制电机。     

五自由度混合磁轴承结构参数设计与分析

提出一种新型的五自由度混合磁轴承支承高速电机系统,由径向二自由度混合磁轴承、径向-轴向三自由度混合磁轴承和高速电机构成.文中介绍混合磁轴承的结构和工作原理,二自由度混合磁轴承采用轴向充磁的环形永磁体提供偏置磁场,定子采用双片式八极结构,每片定子有四个凸极.三自由混合磁轴承集成径向和轴向磁轴承功能,采用径向充磁的环形永磁体提供径向和轴向偏置磁场.导出磁轴承的数学模型,给出详细的参数设计方法,最后采用Maxwell电磁场有限元分析软件对磁轴承的磁路和主轴受力情况进行分析.理论研究和有限元分析表明,这种五自由度混合磁轴承系统结构参数设计合理.     

磁悬浮风力机用轴向磁轴承电磁场分析

介绍了磁悬浮风力机的工作原理,对其进行磁场分析。以功率1k W自重364N的风力机样机为例,通过有限元软件分析气隙值和主轴倾角对轴向磁轴承电磁场的影响。结果表明:在正常工况下,气隙值取0.4±0.006mm,主轴倾角在±0.06°内时,磁轴承漏磁小,电磁力较稳定,主轴转子抗干扰能力强,能满足磁悬浮风力机稳定悬浮并平稳运行的要求。为磁悬浮风力机的结构优化提供了理论依据。     

一种气体-磁轴承混合支承的电主轴及其控制系统设计

提出一种新型气体轴承、径向-轴向磁轴承混合支承的电主轴,设计基于粗集理论方法的磁轴承电主轴模糊控制系统,并进行了相关性能试验,结果表明:设计的控制系统使主轴系统具有良好的静动态性能。     

磁悬浮支承技术在机床中的应用

磁悬浮支承技术是目前世界上公认的高新技术之一。它在高档数控机床中可以作为高速机床电主轴和高速机床直线电机进给平台的支承技术。主动控制磁悬浮轴承(简称主动磁轴承A M B)是利用可控磁场力提供无接触支承、使转子稳定悬浮于空间且其动力学性能可由控制系统调节的一种新型     

支承高速电机的混合磁轴承结构参数设计与分析

提出了一种5自由度混合磁轴承支承高速电机系统,由径向2自由度混合磁轴承、径向-轴向3自由度混合磁轴承和高速电机构成.2自由度磁轴承定子采用8极结构,4个是控制磁极,4个是嵌入永磁体的永磁磁极.3自由度混合磁轴承集成了径向和轴向轴承功能,采用径向充磁的环形永磁体提供径向和轴向磁轴承偏置磁场.文中介绍了混合磁轴承的结构和工作原理,导出了磁轴承的数学模型,给出了详细的参数设计方法,最后采用MAXWELL电磁场有限元分析软件对磁轴承的磁路和主轴受力情况进行了分析.理论研究和有限元分析表明:这种5自由度磁轴承系统结构参数设计合理.     

直驱风力发电机径向-轴向混合磁轴承设计及分析

为解决或降低传统直驱风力发电机系统的机械摩擦问题,以有效提高风能利用率,提出直驱风力发电机采用机械轴承和磁悬浮轴承集成支承技术,即采用机械轴承和径向-轴向三自由度混合磁轴承实现直驱风力发电机的集成支承。针对径向-轴向三自由度混合磁轴承,采用等效磁路法进行数学建模,并利用有限元分析软件对其进行参数设计与机理分析。在此基础上,构建了径向-轴向三自由度磁轴承试验平台,试验结果证明设计的径向-轴向三自由度磁轴承能够实现稳定悬浮。     

三支承磁悬浮轴承的不对中特性

应用多个磁悬浮轴承支承的转子系统,由于机械加工以及安装等方面的误差会导致各个磁悬浮轴承之间有一定的不对中量。提出了将转子偏离磁轴承中心悬浮,以减小各个支承悬浮位置的不对中量;结合单自由度磁轴承控制原理,分析了转子悬浮位置偏离中心对磁轴承悬浮性能的影响;从理论和试验两个方面对比研究了3个不对中磁悬浮轴承支承的转子悬浮在磁轴承中心和偏离中心后磁轴承的控制电流和抗扰动性能。研究结果表明一定程度的偏离磁轴承中心悬浮能够提高磁悬浮轴承系统的稳定性。     

磁悬浮飞轮用永磁偏置磁轴承漏磁分析

磁悬浮飞轮用永磁偏置磁轴承的定转子气隙间存在漏磁现象,为了准确计算漏磁的大小,从而精确地对磁轴承进行磁路设计,利用有限元法对该现象进行了分析.通过ANSYS软件针对一台磁悬浮飞轮样机用径向磁轴承的磁场分布进行分析,提出了一种等效气隙漏磁系数的计算方法,得到样机用磁轴承的漏磁系数.样机试验结果表明,用这一方法计算得到的漏磁系数进行磁轴承参数设计及性能分析具有足够的精度,能够满足实际工程需要.     

风力发电机磁轴承参数设计及控制系统研究

为减小风力发电机的机械摩擦及减少其维护成本,降低风力发电机启动风速,减小旋转阻力矩,提高风能利用率,在垂直轴风力发电机中采用混合轴承支承,即风力发电机径向采用1个径向磁轴承和1个机械轴承支承,轴向采用一个轴向磁轴承来实现五自由度支承。针对轴向磁轴承,首先介绍了其结构及工作原理,然后采用等效磁路法建立数学模型,并按性能指标要求进行参数设计,然后用Ansoft软件对轴向磁轴承磁场及受力等进行分析验证,设计了轴向磁轴承控制系统,并用Matlab软件对磁轴承的控制系统进行了阶跃响应、起浮和扰动等仿真研究。研究结果表明:参数设计合理,控制系统够实现磁轴承可靠及稳定的悬浮。     

磁悬浮轴承结构与磁路分析

从受控自由度数、磁力产生方式、磁极结构形式、控制电流性质等方面对磁悬浮轴承进行了分类与比较.针对各种典型磁悬浮轴承给出了其结构与磁路示意图,并进行了定性分析与比较,最后分析了磁悬浮轴承结构与磁路方面研究与发展方向.     

Rotating magnetic beacons magnetic field strength size in SAGD

Rotation magnetic beacons magnetic field strength is very important to drill parallel horizontal twin wells in steam assisted gravity drainage (SAGD). This paper analyzes a small magnet with a diameter of 25.4 mm. At each end, there is a length of 12.6 mm with permanent magnet, and in the middle, there is a length of 78mm with magnetic materials. The magnetic field strength generated by the magnetic material of 1J12, 1J50, and 1J79 is analyzed, respectively. ANSOFT software is used to simulate the magnetic field strength generated by different magnetic materials above, which also be tested through experimental methods. The comparison of the simulation and experimental results show that experimental and simulation results are basically consistent, and the results can meet the specific requirements of engineering applications.     

磁悬浮陀螺飞轮用隐式洛伦兹力磁轴承

针对磁悬浮陀螺飞轮用显式洛伦兹力磁轴承气隙磁密均匀性差的问题,提出了一种磁钢内置的隐式洛伦兹力磁轴承,并采用三维有限元法对两种方案的气隙磁密进行比较分析。隐式方案的气隙磁密在周向和纵向的变化率分别为0.8%和8.4%,远优于显式方案的15.0%和23.7%。利用磁场分割法对隐式方案的磁阻进行了区域分割,采用积分法精确计算各区域磁阻,建立了磁轴承磁路数学模型,得到了影响偏转电流刚度的关键结构参数,并基于有限元法对隐式方案形状及结构参数进行详细优化。结果表明,在不恶化气隙磁密变化率的前提下,优化前后绕组区域的最大磁密和最小磁密分别从0.404T和0.368T增加至0.464T和0.427T,增幅为14.6%和16.0%。根据优化结果研制了一台隐式洛伦兹力磁轴承,并进行了气隙磁密和偏转电流刚度实验测试,测试结果与设计结果相符,对洛伦兹力磁轴承的设计具有重要意义。     

Tribological properties of Mn-Zn-Fe magnetic fluids under magnetic field

A controllable and variable magnetic field was got by improving the oil cup of a MS-800 four-ball tester. By this improved four-ball tester, the tribological properties of Mn_0.78Zn_0.22Fe₂O₄ magnetic fluid in the magnetic field were tested. The worn surfaces of the steel balls lubricated with 6 wt% Mn_0.78Zn_0.22Fe₂O₄ magnetic fluid under different magnetic fields were observed by using a scanning electron microscope (SEM), while the elemental compositions of the wear scars were analyzed by means of energy dispersive spectrometry (EDS). It was found that the Mn_0.78Zn_0.22Fe₂O₄ nanoparticles had a diameter about 20 nm. Under magnetic field, the 46^# turbine oil containing 6 wt% Mn_0.78Zn_0.22Fe₂O₄ nanoparticles showed much better friction-reducing and anti-wear abilities compared with lubrication without magnetic field. The worn surface, lubricated by 6 wt% Mn_0.78Zn_0.22Fe₂O₄ magnetic fluid lubricated under the effect of magnetic field, is smooth and the plowing is almost disappeared. Moreover, it is found that 22 mT magnetic induction is the optimum magnetic induction. Form theory study we found that under the effect of magnetic field, the bearing capacity increasing with the increasing of magnetic induction. When the eccentricity is small, the side leakage is highly decreased.     

Wear coatings for magnetic thin film magnetic recording heads

Many coatings are in use today for the wear protection of thin film heads. With the trend towards smaller head-media distances, the thickness of the coating has to diminish. In this paper some of these coatings: zirconia, chromium nitride, chromium oxide and diamond (+diamond-like carbon) will be discussed. It will be shown that the film hardness is influenced by the microcrystalline structure, the texture and the film stress. The film hardness shows a good correlation with the reciprocal wear coefficient. The wear resistance of the materials discussed increases in the order: zirconia, chromium nitride, chromium oxide, diamond.     

Nuclear magnetic resonance apparatus for pulsed high magnetic fields

A nuclear magnetic resonance apparatus for experiments in pulsed high magnetic fields is described. The magnetic field pulses created together with various magnet coils determine the requirements such an apparatus has to fulfill to be operated successfully in pulsed fields. Independent of the chosen coil it is desirable to operate the entire experiment at the highest possible bandwidth such that a correspondingly large temporal fraction of the magnetic field pulse can be used to probe a given sample. Our apparatus offers a bandwidth of up to 20 MHz and has been tested successfully at the Hochfeld-Magnetlabor Dresden, even in a very fast dual coil magnet that has produced a peak field of 94.2 T. Using a medium-sized single coil with a significantly slower dependence, it is possible to perform advanced multi-pulse nuclear magnetic resonance experiments. As an example we discuss a Carr-Purcell spin echo sequence at a field of 62 T.     

数字磁罗盘的全姿态罗差补偿

针对现有磁罗盘罗差补偿方法成本高、效率低和全姿态补偿能力不足的问题,提出了一种基于几何变换的全姿态罗差补偿方法.首先,根据外磁干扰对磁传感器采样值的影响,建立了几何变换罗差补偿模型,将罗差补偿参数由12个减少到9个.其次,将牛顿法算子引入到粒子群算法中建立了混合粒子群优化算法,采用粒子群算法选取优化参数初始值,以牛顿法...     

Thrust bearing using a magnetic fluid lubricant under magnetic fields

This paper describes a thrust bearing using a magnetic fluid lubricant under a magnetic field. The critical pressures of the bearing versus the magnitude of the magnetic flux densities have been investigated experimentally. It is shown that the critical pressures of the proposed bearing are larger than those of the normal lubricated bearing under high speeds.     

Modeling and analysis of magnetic dipoles in weak magnetic field

The magnetic leakage field distribution resulting from linear defects of a tube sample in the geomagnetic field is modeled according to the magnetic dipole theory. The formula to compute the normal component of the weak magnetic field is deduced based on the spatial distribution of the magnetic dipole. The shape and characteristics of the zero line (an important criterion for magnetic memory testing) of the normal field is analyzed under different longitudinal magnetizations. Results show that the characteristics of the zero line should be considered when the metal magnetic memory testing method is used to find and locate the defect. __________ Translated from Transactions of Beijing Institute of Technology, 2007, 27(147): 395–398 [译自: 北京理工大学学报]