共查询到18条相似文献,搜索用时 156 毫秒
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永磁行星齿轮和同轴永磁齿轮是两类具有不同拓扑结构和运行原理的磁力齿轮,采用定量设计比较法设计了具有相同有效体积和永磁体用量的上述两类磁齿轮,并通过有限元分析法对二者的转矩传递性能进行比较研究。研究结果表明,永磁行星齿轮较同轴永磁齿轮有更高的转矩密度和更低的转矩脉动。此外,由于永磁行星齿轮具有更加灵活的运行模式,并且能实现功率分流,使其在混合动力汽车领域有很好的应用前景。加工了一台永磁行星齿轮样机,并搭建试验平台进行了相关的试验,结果表明了该拓扑结构的有效性。 相似文献
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植入式人工心脏泵要求体积小、质量轻、功耗低,为了满足这些要求,需要研究磁悬浮人工心脏泵的轴承特性。为此,对径向永磁轴承自身的耦合特性进行了理论分析与仿真,据此提出了心脏泵转子的磁悬浮支承方案,该方案采用两个径向永磁轴承和一个轴向电磁轴承来实现转子的五自由度稳定悬浮。根据径向永磁轴承的磁场分布特性,提出了采用两个关于转子轴线对称布置的霍尔传感器,从转子径向方向检测转子轴向位移的方法,理论分析揭示了转子径向位移和轴向位移在检测结果中的耦合关系,并给出了解耦方法,得出了轴向位移。基于研究成果设计了轴流式磁悬浮人工心脏泵原型机,并成功实现了转子的五自由度稳定悬浮。 相似文献
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基于永磁同步电机和电磁轴承的人工心脏研究 总被引:2,自引:0,他引:2
提出了的新型可植入式人工心脏是由轴向磁场结构的永磁同步电动机直接发驱动。电机转子安装在人工心脏泵的叶轮上,并因电磁轴承的作用而悬浮。文中将重点分析该电机及轴承的结构与设计,并给出了一些相关的仿直结果。 相似文献
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平行轴永磁齿轮的特性研究 总被引:4,自引:0,他引:4
永磁齿轮利用永磁磁场的相互耦合作用产生磁性力来实现非接触传动。采用有限元法求得了永磁齿轮的磁场,进而采用虚功原理求得了磁力矩以及永磁齿轮的矩角特性。通过仿真分析了动轮随主动轮转动的机理。制作了实验模型,实验结果验证了分析方法的正确性。 相似文献
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依据永磁体充磁方向和排列方式的不同,轴向磁齿轮可分为轴向充磁磁齿轮、聚磁式轴向磁齿轮和Halbach式轴向磁齿轮。采用3D有限元法对三种轴向磁齿轮的磁场、转矩特性和轴向力进行了比较。基于气隙磁场的谐波分析,利用公式计算出各次谐波磁场产生的转矩和轴向力,得出各次谐波磁场对转矩传递和轴向力的作用。比较表明,聚磁式轴向磁齿轮的转矩能力和永磁体利用率最大,比轴向充磁磁齿轮提高了17.5%和32.6%,比Halbach式轴向磁齿轮提高了2%和15.1%。Halbach式轴向磁齿轮的气隙中引起转矩波动的磁场谐波的幅值最小,转矩波动也最小。轴向充磁磁齿轮低速转子的轴向力最小,比聚磁式轴向磁齿轮小38.3%,比Halbach式轴向磁齿轮小32.7%。 相似文献
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杜世勤 《上海电机学院学报》2011,14(3)
为避免机械齿轮振动,或要在分开物体间传递力矩,可以采用磁力齿轮传动装置。设计该磁力传动装置时需要对其设计参数进行精确计算。在电机设计时,使用有限元方法对一种大力矩磁力齿轮——磁场调制式磁力齿轮进行了磁场计算,为设计该磁力齿轮提供了有力的工具。 相似文献
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Rens J. Atallah K. Calverley S. D. Howe D. 《Industry Applications, IEEE Transactions on》2010,46(1):206-212
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Rasmussen P.O. Andersen T.O. Jorgensen F.T. Nielsen O. 《Industry Applications, IEEE Transactions on》2005,41(3):764-770
This paper presents calculation and measurement results of a high-performance permanent-magnetic gear. The analyzed permanent-magnetic gear has a gear ratio of 5.5 and is able to deliver 27 N/spl middot/m. The analysis has shown that special attention needs to be paid to the system where the gear is to be installed because of a low natural torsion spring constant. The analyzed gear was also constructed in practice in order to validate the analysis and predict the efficiency. The measured torque from the magnetic gear was only 16 N/spl middot/m reduced by the large end-effects. A systematic analysis of the loss components in the magnetic gear is also performed in order to figure out why the efficiency for the actual construction was only 81%. A large magnetic loss component originated in the bearings, where an unplanned extra bearing was necessary due to mechanical problems. Without the losses of magnetic origin in the bearings and less end-effects caused by relatively short stack, an impressive efficiency estimated at 96% can be obtained. Comparison with classical mechanical gears has shown that the magnetic gear has a better efficiency and a comparable torque per volume density. Finally, it is concluded that the results in this paper may help to initiate a shift from mechanical gears to magnetic gears. 相似文献
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磁齿轮能够实现低速大转矩输出。为了进一步提高同轴磁齿轮的输出能力,提出一种双磁场调制磁齿轮拓扑结构。双磁场调制磁齿轮将传统的表贴式同轴磁齿轮低速转子侧的转子轭用辅助调磁环代替,结构上包含2个转子,2个调磁环和3层气隙。分析双磁场调制磁齿轮的工作原理,采用有限元法,对新增调磁环的尺寸进行了优化。对比分析双磁场调制磁齿轮和传统表贴式同轴磁齿轮的磁场分布和传动转矩。不同传动比下,双磁场调制磁齿轮的转矩能力普遍高于传统表贴式同轴磁齿轮。当传动比为7.5时,双磁场调制磁齿轮的低速转子最大输出转矩达到70.81N·m,与相同尺寸的传统表贴式同轴磁齿轮相比,转矩能力提升了54%。稳定运行时,双磁场调制磁齿轮的低速转子转矩脉动有所增大。 相似文献
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When two power supplies with nearby frequencies are connected to a two‐phase induction motor, the motor generates two kinds of oscillatory torque components, which have frequency components of the sum and the difference between the frequencies of the power supplies. These oscillatory torque components are sinusoidal, and the torque with the frequency component of the difference is considerably larger than the torque with the frequency component of the summation. Consequently, the motor behaves as a swing motor, which alternately changes the direction of rotation. Because of the regularity of the period of the human heartbeat, this swing motor is suitable for use as the driver of an artificial heart. We propose here to use this swing motor as the pump for artificial hearts. In this paper, we present the fundamental theory and the characteristics of the swing motor, and an outline of the motor action for artificial hearts. © 2000 Scripta Technica, Electr Eng Jpn, 132(1): 73–80, 2000 相似文献
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Most industrial robots are driven through reduction gears such as Harmonic Drives and RV gears. Due to the flexibility of the drive system, vibratory behavior occurs during operation. When flexibility is considered, the drive system of the robot joint can be modeled as a resonant mechanical system called a two‐inertia system. Conventionally, studies of two‐inertia system have discussed semiclosed‐loop control using only motor information and a state observer. On the other hand, joint torque sensing of robots has been studied in the harmonic drives that are widely used in robot joints. The joint torque sensor is becoming available with higher performance. In this paper, we consider the control of a robot arm having two‐inertia resonance by using the joint torque sensor. The performance of the torque sensor and that of the observer are compared. © 2006 Wiley Periodicals, Inc. Electr Eng Jpn, 156(2): 75–84, 2006; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/eej.20226 相似文献