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Comparative Analysis of a Coaxial Magnetic Gearbox with a Flux Concentration Halbach Rotor and Consequent Pole Rotor Typology.

机译:具有磁通浓度Halbach转子和相应极转子类型的同轴电磁齿轮箱的比较分析。

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By utilizing magnetic field space modulation magnetic gearboxes (MGs) are able to create speed amplification without any physical contact [1-3]. An example of a flux-focusing coaxial MG is illustrated in Fig. 1. This coaxial MG consists of an inner rotor 1 that contains p1 = 4 pole-pairs an outer rotor 3 with p3 = 13 pole-pairs and a central ferromagnetic segment central rotor 2 that consists of n2 = 17 pieces. The n2 ferromagnetic segments serve to modulate the inner and outer rotor magnetic fields. In order to create the highest level of field coupling between the inner and outer rotors the number of ferromagnetic segments must be chosen to satisfy n2 = p1+p3. With this condition satisfied the rotor angular velocity relationship between each rotor is w2p2 = w3p3+w1p1 where the subscript denotes rotor number. If the outer rotor is fixed (ω3 = 0) the torque will be maximized and the gearing ratio will be w1 = Gw2 where G = n2/p1. For the example MG shown in Fig. 1 the gear ratio is G = 4.25. In order to try to increase the torque density of a MG a range of different coaxial type rotor typologies have recently been investigated [4-14]. Along with the flux focusing MG design two other coaxial radial type MG rotor typologies that have been shown to create high torque density are the flux concentration Halbach rotor typology [15] and the consequent pole triple-PM rotor MG typology [16]. In this paper, these two design typologies are compared for the first time. The objective is to provide an idealized comparative analysis of the two competing typologies and then present the experimental design and testing of the best design.
机译:通过利用磁场空间调制,磁性齿轮箱(MGs)可以在没有任何物理接触的情况下实现速度放大[1-3]。聚焦磁通的同轴MG的示例如图1所示。该同轴MG由内转子1组成,内转子1包含p 1 = 4个极对,外转子3与p 3 = 13个极对和一个由n组成的中心铁磁段中心转子2 2 = 17件。然后 2 铁磁段用于调制内部和外部转子磁场。为了在内转子和外转子之间产生最高水平的场耦合,必须选择铁磁段的数量以满足n 2 = p 1 + p 3 。在此条件下,每个转子之间的转子角速度关系为w 2 p 2 = w 3p3 + w 1 p 1 下标表示转子号。如果外转子是固定的(ω 3 = 0)扭矩将最大化并且传动比为w1 = Gw 2 其中G = n 2 / p 1 。对于图1所示的示例MG,齿轮比为G = 4.25。为了尝试增加MG的转矩密度,最近研究了一系列不同的同轴转子类型[4-14]。与磁通量聚焦MG设计一起,已显示出可产生高转矩密度的其他两种同轴径向型MG转子类型是磁通量浓度Halbach转子类型[15]和随之而来的极三重PM转子MG类型[16]。本文首次对这两种设计类型进行了比较。目的是提供两种竞争类型的理想比较分析,然后介绍最佳设计的实验设计和测试。

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