{"title":"低速应用中结果极与同极结果极无轴承电机的性能比较","authors":"H. Sugimoto, Miyabi Terashima","doi":"10.1109/ECCE47101.2021.9594970","DOIUrl":null,"url":null,"abstract":"This paper presents performance comparisons of a consequent-pole (CP) and a homopolar consequent-pole (HCP) bearingless motors. Radial directions are actively positioned, and axial and tilting directions are passively stabilized with a disk-shaped rotor. In the CP and HCP bearingless machines, the radial suspension force is generated by a two-pole suspension winding. However, the radial suspension force characteristics are considerably different in the two machines. The radial suspension force of the HCP is generated when a two-pole suspension flux is superimposed on a homopolar flux by thrust permanent magnets. In contrast, the CP bearingless motor requires $p \\pm 2$-pole suspension fluxes modulated by the salient-pole rotor core to generate the radial suspension force with a p-pole rotor permanent magnet flux. As a result, the force error angle of the HCP bearingless motor is significantly low compared with the CP bearingless motor. A prototype machine of the HCP bearingless motor is fabricated and tested. In the experiment, it is demonstrated that stable magnetic suspension and rotation are achieved at 1000 r/min.","PeriodicalId":349891,"journal":{"name":"2021 IEEE Energy Conversion Congress and Exposition (ECCE)","volume":"5 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-10-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Performance Comparison of Consequent-Pole and Homopolar Consequent-Pole Bearingless Motors for Low Speed Applications\",\"authors\":\"H. Sugimoto, Miyabi Terashima\",\"doi\":\"10.1109/ECCE47101.2021.9594970\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper presents performance comparisons of a consequent-pole (CP) and a homopolar consequent-pole (HCP) bearingless motors. Radial directions are actively positioned, and axial and tilting directions are passively stabilized with a disk-shaped rotor. In the CP and HCP bearingless machines, the radial suspension force is generated by a two-pole suspension winding. However, the radial suspension force characteristics are considerably different in the two machines. The radial suspension force of the HCP is generated when a two-pole suspension flux is superimposed on a homopolar flux by thrust permanent magnets. In contrast, the CP bearingless motor requires $p \\\\pm 2$-pole suspension fluxes modulated by the salient-pole rotor core to generate the radial suspension force with a p-pole rotor permanent magnet flux. As a result, the force error angle of the HCP bearingless motor is significantly low compared with the CP bearingless motor. A prototype machine of the HCP bearingless motor is fabricated and tested. In the experiment, it is demonstrated that stable magnetic suspension and rotation are achieved at 1000 r/min.\",\"PeriodicalId\":349891,\"journal\":{\"name\":\"2021 IEEE Energy Conversion Congress and Exposition (ECCE)\",\"volume\":\"5 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2021-10-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2021 IEEE Energy Conversion Congress and Exposition (ECCE)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ECCE47101.2021.9594970\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2021 IEEE Energy Conversion Congress and Exposition (ECCE)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ECCE47101.2021.9594970","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Performance Comparison of Consequent-Pole and Homopolar Consequent-Pole Bearingless Motors for Low Speed Applications
This paper presents performance comparisons of a consequent-pole (CP) and a homopolar consequent-pole (HCP) bearingless motors. Radial directions are actively positioned, and axial and tilting directions are passively stabilized with a disk-shaped rotor. In the CP and HCP bearingless machines, the radial suspension force is generated by a two-pole suspension winding. However, the radial suspension force characteristics are considerably different in the two machines. The radial suspension force of the HCP is generated when a two-pole suspension flux is superimposed on a homopolar flux by thrust permanent magnets. In contrast, the CP bearingless motor requires $p \pm 2$-pole suspension fluxes modulated by the salient-pole rotor core to generate the radial suspension force with a p-pole rotor permanent magnet flux. As a result, the force error angle of the HCP bearingless motor is significantly low compared with the CP bearingless motor. A prototype machine of the HCP bearingless motor is fabricated and tested. In the experiment, it is demonstrated that stable magnetic suspension and rotation are achieved at 1000 r/min.